5 , . muwhtmv . ‘ Jrswi Mam; ‘ I: . $9» wanna-e}... 5' ’3': A!» .15. 3. . n.- o. a) - I (I 131v I up. .3051. 1.... :33... {In that. than". I 3 ’5 .1. mt”; M" .5. math” at; in»? 1. x a ‘ 1.2"”! .v Enwféu .. l O. I . . 2.16:1:3 it. :- 6.11“.»3 .- II. I . » ‘|il’|.¢\flnl.l' ' no»! vJ)’$~.A. it 3.51!!! . x . « . . “u \h‘nsh 197‘ 1312.04! . b ‘5’- .1531 I [5: B ; . E . f... . :3 : ..:A..'ffn bl ... THESIS ,; \ lllllWWW"!NIUUHINIHHIIHUHIHIIHIUJIUWUI , 1 1293 01050 0712 #LIBR'KfiY Michigan State University This is to certify that the dissertation entitled Effect of Temperature on the Behavior of Biradical Intermediates: Conformational Control of Product Ratios in Photocyclization React1ons presented by Ali Reza land has been accepted towards fulfillment of the requirements for Ph.D. degreein Chemistry 9% a rprofe“r D te fl/o'y. “3/779 MS U i: an Affirmative Action/Equal Opportunity Institution 0-12771 PLACE ll RETURN BOX to remove thle checkout from your record. TO AVOID FINES return on or before dete due. DATE DUE DATE DUE DATE DUE MSU le An Atflnnetlve AotlorVEquel Opportunity lnetltttton mama-m Effect of Temperature on the Behavior of Biradical Intermediates: Conformational Control of Product Ratios in Photocyclization Reactions by Ali Reza Zand A DISSERTATION Submitted to Michigan State University In partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Department of Chemistry 1996 Abstract Effect of Temperature on the Behavior of Biradical Intermediates: Conformational Control of Product Ratios in Photocyclization Reactions by Ali Reza Zand The photochemistry of several ketones at various temperatures was investigated. Intramolecular 6-hydrogen abstraction by excited carbonyl groups results in formation of 1,5-biradicals which upon cyclization yield indanols as photoproducts. This investigation probed the effect of temperature on the diastereoselectivity of cyclization with emphasis on the role of intersystem crossing on product ratios. a—Arylacetophenones show variable product ratios at various temperatures. The Arrhenius plots are linear indicative of conformational equilibrium. The results show nonenthalpic factors to be as important as enthalpic differences at determining diastereoselectivity. The low diastereoselectivities observed for a—(2-benzylphenyl)- acetophenones is attributed to benzylic conjugation which imparts rotational freedom to both ends of the biradical intermediate. a-Aryl propiophenones show a large preference for the a-methyl group and the phenyl to be trans in the 2-phenyl-2-indanol product. This phenomenon seems to stem from the lowest energy “reactive ground state conformer” of the ketones which always mirrors one of the biradical minima. Irradiation of a-arylacetones results in formation of indanols and a-cleavage products. Indanol formation involves a singlet state 5-hydrogen abstraction followed by Yang cyclization while a-cleavage occurs from the triplet state. The fact that a-cleavage is the predominant photoreaction at low temperatures has been attributed to a competition between hydrogen abstraction which has a barrier and a barrierless intersystem crossing process. a-Arylacetones show lower indanol diastereoselectivities than their acetophenone analogs. This has been attributed to conformational control, rather than ground state control, of diastereoselectivity. The low product quantum yields of or- arylacetones have been attributed to a well known radiationless decay process which competes with singlet state hydrogen abstraction. o-tert—Butyl-a,a,a-trifluroacetophenone, like 0-tert-butylacetophenone, forms an indanol and an unsaturated alcohol upon irradiation in benzene and methanol. The unsaturated alcohol is the major product under all conditions. Capto-dative resonance thus does not provide sufficient stabilization to allow the hydroxy end of the biradical to twist out of benzylic conjugation to give higher indanol yields. 2-(2’-(2’,3’-Dimethyl)butyl)benzophenone forms three iSOmeric indanols and an unsaturated alcohol upon irradiation in solution and in the solid state. Two different reaction sites, isopropyl and methyl, seem to have comparable reactivity which shows the insensitivity of hydrogen abstraction rates to orientational factors. Formation of the unsaturated alcohol mimics the o-tert-butylacetophenone derivatives and could explain the less than unity quantum yields previously observed for tert-amylbenzophenones. This Thesis is Ded' icated To My Grandmothers Who Passed away Bef I G ore raduated iv Acknowledgments The Author wishes to thank Dr. Peter J. Wagner for his help, guidance, sense of humor and innumerable entertaining discussions during the course of this work. The author is grateful to the National Science Foundation and Michigan State University for financial support in the form of teaching, research assistantships and the Hart fellowship. The author would also like to thank the Chemistry Department for the use of its excellent facilities. The author also owes special thanks to fi-iends in the Wagner research group. Their help and support made my graduate career much more enjoyable. Last, but by no means least, I would like to thank my family for their help, support and patience throughout my graduate career. Table of Contents TABLE OF CONTENTS vi LIST OF FIGURES viii LIST OF TABLES x LIST OF SCHEMES xii LIST OF ABBREVIATIONS xiv INTRODUCTION 1 I. MEASUREMENTS OF QUANTUM YlELDS AND EXCITED STATE LIFETIMES .................................................... 3 II. A-CLEAVAGE REACTIONS ............................................................................................................................ 5 III. HYDROGEN ABSTRACTION .............................................................................................. 8 A. Conformational Control of Photoreactivity ........................................................................................ II B. Orientational Requirements of Hydrogen Abstraction ......................................................................... l 4 C. 6-Hydrogen Abstraction ....................................................................................................................... 21 D. Nature of the Excited State- Singlet vs. Triplet .................................................................................... 25 E. Eflect of Environment ........................................................................................................................... 28 F. Biradical Lifetime ................................................................................................................................. 30 G. Diastereoselectivity .............................................................................................................................. 34 H. Photoenolization of a—(2, 4, 6-tritsopropylphenyl)acetophenone ......................................................... 36 IV. GOALS OF RESEARCH ............................................................................................................................... 38 RESULTS 40 I. A-ARYLACETOPHENONES AND DERIVATIVES .............................................................................................. 40 A. General Preparation of the Ketones .................................................................................................... 40 B. Irradiation of Ketones .......................................................................................................................... 4] C. Steady-State Photokinetics. .................................................................................................................. 60 II. A-ARYLACETONES ..................................................................................................................................... 62 A. General Preparation of the Ketones. ................................................................................................... 62 B. Irradiation of Ketones .......................................................................................................................... 62 C. Identification of Photoproducts ........................................................................................................... 63 D. Steady-State Photokinetics ................................................................................................................... 70 III. 2-TERT-BUTYL TRIFLOROACETOPHENONE ............................................................................................... 72 A. Preparation .......................................................................................................................................... 72 B. Irradiation Conditions .......................................................................................................................... 72 C. Identification of Photoproducts ........................................................................................................... 72 IV. 2'-(2,3-DlMETHYL-2-BUTYL)BENZOPHENONE .......................................................................................... 74 A. General Preparation ............................................................................................................................ 74 B. Irradiation Conditions .......................................................................................................................... 74 C. Identification of photoproducts. ........................................................................................................... 75 D. Steady-State Photokinectics ................................................................................................................. 78 V. SEMIEMPIRICAL CALCULATIONS ............................................................................................................... 79 DISCUSSION 90 I. CONFORMATIONAL CONTROL OF PRODUCT RATIOS FROM TRIPLET 1,5-BIRADICALS ................................ 90 II. PHOTOBEHAVIOR 0F A-ARYLACETONES- A COMPARISON OF SINGLET AND TRIPLET BIRADICAL BEHAVIOR ........................................................................................................................ l 10 III. PHOTOENOLIZATIONS OF A-(2, 4 ,6-TRIISOPROPYLPl-IENYL)ACETOPHENONE AND ACETONE ................... l 15 vi IV. PHOTOBEHAVIOR or O-TERT-BUTYLTRIFLUOROACETOPHENONE ......................................................... l 18 V. PHOTOBEHAVIOR or 2-(2’-(2’,3’-D1METHYLBUTYL))BENZOPHEN0NE - EFFECT or DIHEDRAL ANGLE ON HYDROGEN ABSTRACTION RATES ............................................................................................................... 120 EXPERIMENTAL 131 I. GENERAL PROCEDURES ............................................................................................................................ l3l II. PREPARATION OF STARTING KETONES .................................................................................................... I32 a-(Z-Ethylphenyl) -fl,,6,fl-trideuteropropiophenone (4 d3) ...................................................................... I 32 a—(Z-Ethylphenyvpropiophenone (4) ..................................................................................................... I37 a-(2-Ethylphenyl)acetone (I 0) ............................................................................................................... I38 a-Mesitylacetone ( l I )....; ....................................................................................................................... I40 a—(2—Benzylphenyl)propiophenone (7) .................................................................................................. l 42 a—(2, 4, 6- Triethylphenyl) -)3,fl,,6-tridueteropropiophenone (5 d 3) ........................................................... I45 a-(2, 4, 6-Triethylphenyl)propiophenone (5) .......................................................................................... I 50 a-(Z, 4, 6- Triethylphenyl)acetone (12) .................................................................................................... 150 a-(2, 4, 6- T ritsopropylphenyUacetone (I 3) ............................................................................................. I 52 a—(2, 4, 6- Trizsopropylphenyl)acetophenone (9) ..................................................................................... l 5 5 o-tert-Butyl-ma, a-trifluroacetophenone (l 4) ........................................................................................ 15 7 o-(2, 3-Dimethyl-2-buty1)bemophenone (15) .......................................................................................... I 60 III. PHOTOCHEMICAL EXPERIMENTS AND PROCEDURES ........................................................................ j ...... 166 A. Purification of Chemicals ................................................................................................................... I 66 B. Equipment and Procedures ................................................................................................................ l 6 7 C. Identification of Photoproducts ......................................................................................................... l 6 9 D. Quantitative Measurements ............................................................................................................... 219 REFERENCES: . 251 vii List- of Figures FIGURE 1. SIMPLIFIED JABLONSKI DIAGRAM .................................................................................................. 1 FIGURE 2.. ......................................................................................................... 15 FIGURE 3. ORIENTATIONAL REQUIREMENTS FOR H- ABSTRACTION ............................................................... 15 FIGURE 4. EFFECT OF DIHEDRAL ANGLE ON REACTIVITY .............................................................................. l7 HGURE 5. EFFECT OF DIHEDRAL ANGLE ON REACTIVITY .............................................................................. 18 FIGURE 6. CORRELATION DIAGRAM ............................................................. 27 FIGURE 7. MINIMUM ENERGY GEOMETRIES OF A- (2- ETHYLPHENYL)ACETOPHENONE .................................. 80 FIGURE 8. MINIMUM ENERGY GEOMETRIES OF A-(2 ,4 6-TRIETHYLPHENYL)ACETOPHENONE ....................... 80 FIGURE 9. LOWEST ENERGY CONFORMERS OF A-(2-ETHYLPHENYL)PROPIOPHENONE ................................... 81 FIGURE 10. LOWEST ENERGY GEOMETRIES OF A-(2,4,6-'IRIETHYLPHENYL)PROPIOPHENONE ....................... 82 FIGURE 1 1. MINIMUM GEOMETRIES OF A-(2-BEN2YLPHENYL)ACETOPHENONE ............................................ 83 FIGURE 12. LOWEST ENERGY CONFORMERS OF A-(2-BENZYLPHENYL)PROPIOPHENONE ............................... 83 FIGURE 13. LOWEST ENERGY GEOMETRIES OF A-MESITYLPROPIOPHENONE ................................................. 84 FIGURE 14. LOWEST ENERGY GEOMETRY OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETOPHENONE ................... 85 FIGURE 15. LOWEST ENERGY GEOMETRIES OF A-(2-E1HYLPHENYL)ACETONE ............................................. 85 FIGURE 16. LOWEST ENERGY CONFORMERS OF A-MESITYLACETONE ........................................................... 86 FIGURE 17. LOWEST ENERGY GEOMETRIES OF A-(2.4,6-TRIETHYLPHENYL)ACETONE .................................. 87 FIGURE 18. LOWEST ENERGY GEOMETRY OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETONE .............................. 87 FIGURE 19. LOWEST ENERGY GEOMETRY OF 2-TERT-BUTYLTRIFLOUROACETOPHENONE ............................. 88 FIGURE 20 ................................................................................................ 89 FIGURE 21. LOWEST ENERGY BIRADICAL CONFORMATIONS OF 2 ..... 96 FIGURE 22. LOWEST ENERGY GROUND STATE CONFORMATIONS OF 2 .......................................................... 97 FIGURE 23. LOWEST ENERGY BIRADICAL CONFORMATIONS OF 3 ......... ' ......................................................... 99 FIGURE 24. LOWEST ENERGY GROUND STATE CONFORMATIONS OF 8 ........................................................ 100 FIGURE 25. LOWEST ENERGY BIRADICAL CONFORMATIONS OF 8 ................................................................ 101 FIGURE 26. LOWEST ENERGY BIRADICAL CONFORMATIONS OF 5 ................................................................ 105 FIGURE 27. LOWEST ENERGY GROUND STATE CONFORMATIONS OF 5 ........................................................ 107 FIGURE 28. LOWEST ENERGY BIRADICAL CONFORMATIONS OF 4 ................................................................ 108 FIGURE 29. LOWEST ENERGY GROUND STATE CONFORMATIONS 0F 4 ........................................................ 109 FIGURE 30. LOWEST ENERGY BIRADICAL CONFORMATIONS OF 10 .............................................................. 1 14 FIGURE 31. LOWEST ENERGY GROUND STATE AND BIRADICAL CONFORMERS OF 9 AND 13 ....................... l 16 FIGURE 32 ................................. 121 FIGURE 33. VARIABLE TEMPERATURE NMR OF A-(2, 4, 6- -TRIETHYLPHENYL)-B, B, B- TRIDEUTERIO- PROPIOPHENONE IN ACETONE- D6 ....................................................................................................... 149 FIGURE 34. lH NMR OF A-(2-ETHYLPHENYL)ACETOPHENONE BEFORE AND AFTER IRRADIATION IN TOLUENE (A > 290 NM) ...................................................................................................................... 171 FIGURE 35. ‘H NMR SPECTRA OF A-(2,4,6-1RIETHYLPHENYL)ACETOPHENONE BEFORE AND AFTER IRRADIATION IN TOLUENE (A>290 NM) .............................................................................................. 175 FIGURE 36. 'H NMR SPECTRA OF A-(z-ETHYLPHENYL)PROPIOPHENONE BEFORE AND AFTER IRRADIATION IN TOLUENE (A>290 NM) .................................................................................................................... 182 FIGURE 37. 'H NMR SPECTRA OF A-(2,4,6-TRIETHYLPHENYL)PROPIOPHENONE BEFORE AND AFTER IRRADIATION IN TOLUENE (A>290 NM) ......... - .......................................................... 186 FIGURE 38. 'H NMR SPECTRA OF A-(2-BENzYLPHENYL)ACETOPHENONE BEFORE AND AFTER IRRADIATION IN TOLUENE (A>290 NM) .......................................................................................... 191 FIGURE 39. ‘H NMR SPECTRA OF A- MESITYLPROPIOPHENONE BEFORE AND AFTER IRRADIATION IN TOLUENE (A>290 NM) ....................................................................................... 195 FIGURE 40. ‘H NMR OF A-(2, 4 6-1111lSOPROPYLPHENYL)ACETOPHENONE AFTER IRRADIATION IN TOLUENE (A > 290NM) -- ................................................................................................. 197 FIGURE 41. 'H NMR OF THE lNDANOL MIXTURE FROM A-(2- -ETHYLPHENYL)ACETONE IN BENZENE .......... 203 viii FIGURE 42. III NMR OF THE METHYL REGION OF THE INDANOL MIXTURE FROM A-(Z-ETHYLPHENYL)- ACETONE IN BENZENE ........................................................................................................................ 207 FIGURE 43. 1H NMR OF THE METHYLENE REGION OF THE lNDANOL MIXTURE FROM A-(2- ETHYLPHENYL)ACETONE IN BENZENE ................................................................................................ 208 FIGURE 44. 1H NMR OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETONE AFTER IRRADIATION IN TOLUENE (A > 290 NM, T= 297 K) ..................................................................................... 213 ix List of Tables TABLE 1. A-SUBST'ITUENT EFFECT ON o-TOLYLACETOPHENONE DERIVATIVES ............................................ 24 TABLE 2. DIASTEREOSELECTTVITY IN PHOTOCYCLOADDITION OF BENZALDEHYDE TO CYCLOALKENES ....... 35 TABLE 3. CHEMICAL YIELDS OF PHOTOPRODUCTS OF A-(2-ETHYLPHENYL)ACETOPHENONE IN TOLUENE AT VARIOUS TEMPERATURES (A > 290) ..................................................................................................... 43 TABLE 4. CHEMICAL YIELDS OF PHOTOPRODUCTS OF A-(2,4,6-TRIETHYLPHENYL)ACETOPHENONE IN TOLUENE AT VARIOUS TEMPERATURES (A >290) - ................................. ..45 TABLE 5. CHEMICAL YIELDS OF PHOTOPRODUCTS OF A-(o-TOLYL)PROPIOPHENONE IN TOLUENE AT VARIOUS TEMPERATURES (A >290) ..................................................................................................................... 46 TABLE 6. CHEMICAL YIELDS OF PHOTOPRODUCTS OF A—(2-ETHYLPHENYL)PROFIOPHENONE IN TOLUENE AT VARIOUS TEMPERATURES (A >290 NM) .......................................................................... 49 TABLE 7. CHEMICAL YIELDS OF PHOTOPRODUCTS OF A—(2, 4 ,6-TRIETHYLPHENYL) PROPIOPHENONE IN TOLUENE AT VARIOUS TEMPERATURES (A > 290 NM) ......................................................................... 50 TABLE 8. CHEMICAL YIELDS OF PHOTOPRODUCTS OF A-(2- BENZYLPHENYL)ACETOPHENONE IN TOLUENE AT VARIOUS TEMPERATURES (A > 290 NM) ................................................................ 53 TABLE 9. CHEMICAL YIELDS OF PHOTOPRODUCTS OF A-MESITYLPROPIOPHENONE IN TOLUENE AT VARIOUS TEMPERATURES (A > 290 NM) .............................................................................................................. 55 TABLE 10. MOLAR ABSORPTTVIT'Y COEFFICIENTS (M‘CM") OF 9 AND ITS ENOL AT VARIOUS WAVELENGTHSS7 TABLE 1 1. PRODUCT QUANTUM YIELDS OF 9 As A FUNCTION OF CONVERSION AND WAVELENGTH ............. 58 TABLE 12. PRODUCT RATIOS OF IRRADIATION OF 9 UNDER VARIOUS CONDmONS ...................................... 59 TABLE 13. LIFETIMES OF TRIPLET ACETO- AND PROPIOPHENONES IN BENZENE ........................................... 60 TABLE 14. QUANTUM YIELDS OF PHOTOPRODUCTS FROM ACETO- AND PROPIOPHENONES IN BENZENE ...... 61 TABLE 15. CHEMICAL YIELDS OF PHOTOPRODUCTS FROM A-(2-ETHYLPHENYL)ACETONE IN TOLUENE AT VARIOUS TEMPERATURES (A > 290 NM) .............................................................................................. 65 TABLE I6. CHEMICAL YIELDS OF PHOTOPRODUCTS FROM A-MESITYLACETONE IN TOLUENE AT VARIOUS TEMPERATURES (A > 290 NM) .............................................................................................................. 67 TABLE 17. PRODUCT CHEMICAL YIELDS OF A-(2,4,6-T‘RIETHYLPHENYL)ACETONE IN TOLUENE AT VARIOUS TEMPERATURES (A >290 NM) ............................................................................................................... 68 TABLE 18. PRODUCT CHEMICAL YIELDS OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETONE As A FUNCTION OF CONVERSION AND TEMPERATURE ........................................................................................................ 70 TABLE 19. TRIPLET LIFETIMES OF A-ARYLACETONES IN BENZENE AT ROOM TEMPERATURE (A= 313 NM) ....................................................................................................................................................... 71 TABLE 20. QUANTUM YIELDS OF PHOTOPRODUCTS OF A-ARYLACETONES IN BENZENE AT ROOM TEMPERATURE (A=313 NM) .................................................................................................................. 71 TABLE 21 . EFFECT OF TEMPERATURE AND MEDIUM ON PRODUCT RATIOS OF 15 .......................................... 77 TABLE 22. TRIPLET LIFETIMES AND PRODUCT QUANTUM YIELDS OF 2-(2'-(2',3'-DIMETHYL)BUTYL)- BENZOPHENONE AT ROOM TEMPERATURE (A= 313 NM) ...................................................................... 78 TABLE 23. EFFECT OF TEMPERATURE ON THE lNDANOL RATIOS OF A-ARYLACETOPHENONES ..................... 91 TABLE 24. ARRHENIUS DATA FROM GRAPH 2 ............................................................................................... 92 TABLE 25. ARRHENIUS DATA FROM GRAPH 3 ............................................................................................. 103 TABLE 26. EFFECT OF TEMPERATURE ON PRODUCT RATIOS FROM A-ARYLACETONES ............................... l 1 1 TABLE 27 . EFFECT OF TEMPERATURE AND MEDIUM ON PRODUCT RATIOS OF 15 ........................................ 124 TABLE 28. DETAILS OF GLOBAL MINIMIZATIONS FOR COMPOUNDS 1-9 ...................................................... 221 TABLE 29. DETAILS OF GLOBAL MINIMIZATIONS FOR COMPOUNDS 10-15 .................................................. 222 TABLE 30. GRID OF ENERGIES FOR THE GROUND STATE OPTIMIZATION OF A-(2-ETHYLPHENYL) ACETOPHENONE ........................................................................................................................ . ......... 223 TABLE 31. GRID OF ENERGIES FOR GLOBAL MINIMIZATION OF THE TRIPLET BIRADICAL OF A-(2,4,6- TRIETHYLPHENYL)ACETOPHENONE .................................................................................................... 224 TABLE 32. GRID OF ENERGIES FOR GLOBAL MINIMIZATION OF THE TRIPLET BIRADICAL OF A-(2- TOLYL)PROPIOPHENONE ..................................................................................................................... 225 TABLE 33. GRID OF ENERGIES FOR GLOBAL MINIMIZATION OF THE TRIPLET BIRADICAL OF A-(2- ETHYLPHENYL)PROPIOPHENONE ................................................ 226 TABLE 34. GRID OF ENERGIES FOR GLOBAL MINIMIZATION OF THE TRIPLET BIRADICAL OF A-(2, 4, 6- TR]ETHYLPHENYL)PROPIOPHENONE ................................................................... 227 TABLE 35. GRID OF ENERGIES FOR GLOBAL MINIMIZATION OF THE TRIPLET BIRADICAL OF A- MESITYLPROPIOPHENONE ................................................................................................................... 228 TABLE 36.GRID OF ENERGIES FOR GLOBAL MINIMIZATION OF THE TRIPLET BIRADICAL OF A-(2- ETHYLPHENYL)ACETONF .................................................................................. 229 TABLE 37. GRID OF ENERGIES FOR GLOBAL MlNlMlZATlON OF THE SINGLET BIRADICAL OF A-(2- ETHYLPHENYL)ACETONE ................................................................................ 230 TABLE 38. GRID OF ENERGIES FOR GLOBAL MINIMIZATION OF THE TRIPLET BIRADICAL OF A- (2, 4, 6- T‘RIISOPROPYLPHENYL)ACETONE ............................................................................. 23 1 TABLE 39. PRODUCT QUANTUM YIELDS OF A-(2-ETHYLPHENYL)ACETOPHENONE IN BENZENE .................. 234 TABLE 40. PRODUCT QUANTUM YIELDS OF A-(2,4,6-TRIETHYLPHENYL)ACETOPHENONE IN BENZENE ...... 235 TABLE 41. PRODUCT QUANTUM YIELDS OF A-(2-BENZYLPHENYL)ACETOPHENONE IN BENZENE ............... 236 TABLE 42. PRODUCT QUANTUM YIELDS OF A-(2-ETHYLPHENYL)PROPIOPHENONE IN BENZENE ................. 237 TABLE 43. PRODUCT QUANTUM YIELDS OF A-(2,4,6-TRIETHYLPHENYL)PROPIOPHENONE IN BENZENE ...... 238 TABLE 44. PRODUCT QUANTUM YIELDS OF A-(2-ETHYLPHENYL)ACETONE IN BENZENE ............................ 239 TABLE 45. PRODUCT QUANTUM YIELDS OF A-MESITYLACETONE IN BENZENE ........................................... 240 TABLE 46. PRODUCT QUANTUM YIELDS OF A-(2,4,6-TRIETHYLPHENYL)ACETONE IN BENZENE ................. 241 TABLE 47. PRODUCT QUANTUM YIELDS OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETOPHENONE IN BENZENE242 TABLE 48. PRODUCT QUANTUM YIELDS OF A-(2-BEN2YLPHENYL)PROPIOPHENONE IN BENZENE ............... 243 TABLE 49. PRODUCT QUANTUM YIELDS OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETONE IN BENZENE .......... 244 TABLE 50. PRODUCT QUANTUM YIELDS OF 2-(2’-(2’,3 ’-DIMETHYL)BUTYL))BENZOPHENONE ................... 245 TABLE 51. QUENCHING OF THE INDANOL FORMATION IN A-(2-ETHYLPHENYL)ACETOPHENONE WITH 2,5- DIMETHYL-Z ,4-HEXADIENE AT 313 NM IN BENZENE ................................. 246 TABLE 52. QUENCHING OF THE INDANOL FORMATION IN A- (2, 4 ,6-TRIETHYLPHENYL) ACETOPHENONE WITH 2, 5- DIMETHYL- 2, 4- HEXADIENE AT 313 NM IN BENZENE .................................................................... 246 TABLE 53. QUENCHING OF THE INDANOL FORMATION IN A-(2-BENZYLPHENYL)ACETOPHENONE WITH 2,5- DIMETHYL-2,4-HEXADIENE AT 313 NM IN BENZENE .......................................................................... 247 TABLE 54. DIMETHYL-2 ,4-HEXADIENE AT 3 I3 NM IN BENZENE ....................................... TABLE 55. QUENCHING OF THE INDANOL FORMATION IN A-(2-ETHYLPHENYL)PROPIOPHENONE WITH 2,5- 247 QUENCHING OF THE INDANOL FORMATION IN A-(2, 4 ,6-TRIETHYLPHENYL) PROPIOPHENONE WITH 2, 5- DIMETHYL-Z, 4-HEXADIENE AT 313 NM IN BENZENE .................................................................... 248 TABLE 56. QUENCHING OF THE INDANOL FORMATION IN 2'-(2, 3- DIMETHYL-2- -BUTYL)BENZOPHENONE WITH 2, 5-DIMETHYL-2, 4- HEXADIENE AT 313 NM IN BENZENE .......................................... 248 TABLE 57. QUENCHING OF THE DIARYLETHANE FORMATION IN A- -(2-ETHYLPHENYL)ACETONE WITH 2, 5- DIMETHYL-z ,4-l-IEXADIENE AT 313 NM IN BENZENE .......................................................................... 249 TABLE 58. QUENCHING OF THE DIARYLETHANE FORMATION IN A-MESITYLACETONE WITH 2,5-DIMETHYL- 2,4-HEXADIENE AT 313 NM IN BENZENE ............................................................................................. 249 TABLE 59. QUENCHING OF THE DIARYLETHANE FORMATION IN A-(2,4,6-TRISIOPROPYLPHENYL) ACETONE WITH 2,5-DIMETHYL-2,4-HEXADIENE AT 313 NM IN BENZENE ........................................................... 250 xi List of Schemes SCHEME 1. A-CLEAVAGE REACTION ................................................................................................................ 5 SCHEME 2. A-CLEAVAGE OF PIVALOPHENONE ................................................................................................. 5 SCHEME 3. CAGE AND NON-CAGE REACTIONS ................................................................................................ 6 SCHEME 4. A-CLEAVAGE IN CYCLIC KETONES ................................................................................................ 7 SCHEME 5. ORBITAL REQUIREMENTS OF TYPE 11 CLEAVAGE ............... . ......................................................... 10 SCHEME 6. ROLE OF BACK TRANSFER IN DETERMINATION OF QUANTUM EFFICIENCIES ............................... 1 1 SCHEME 7. CONFORMATIONAL, ROTATIONAL AND GROUND STATE CONTROL OF REACTIVITY .................... 12 SCHEME 8. CONFORMATIONAL CONTROL OF REACTIVITY ............................................................................. 12 SCHEME 9. GROUND STATE CONTROL OF REACTIVITY .................................................................................. 13 SCHEME 10. ROTATIONAL CONTROL OF REACTIVITY -. .......................................................... 14 SCHEME 1 1. PHOTOCYCLIZATTON OF 2,4,6-TRIISOPROPYLBENZOPHENONES ................................................. 17 SCHEME 12. BOAT-LIKE TRANSITION STATE FOR HYDROGEN ABSTRACTTON ............................................... 19 SCHEME 13. COMPETITION BETWEEN H-ABSTRACITON AND CYCLIZATION EFFICIENCIES ............................ 21 SCHEME 14. A-HYDROGEN ABSTRACTION IN OTBBP .................................................................................... 22 SCHEME 15. PHOTOBEHAVIOR OF OTAMBP ................................................................................................. 23 SCHEME 16. PHOTOCHEMISTRY OF BENzOIN ETHERS .................................................................................... 29 SCHEME l7. PHOTOCHEMISTRY OF HEXAETHYLBENZIL ................................................................................ 29 SCHEME 18. CRYSTALLINE STATE vs. SOLUTION PHOTOCHEMISTRY ............................................................ 30 SCHEME 19. PHOTOCYCLOADDmON OF BENZALDEHYDE TO CYCLOALKENES .............................................. 35 SCHEME 20. ISC CONTROL OF DIASTEREOSELECTIVITY ................................................................................ 36 SCHEME 21. PHOTOTAUTOMERIZATION OF ENOL TO KETONE ................................................................. ' ...... 37 SCHEME 22. PHOTOBEHAVIOR OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETOPHENONE ...................................... 37 SCHEME 23. CHEMICAL SHIFTS OF METHYLS TRANS AND CIS T0 PHENYL IN FIVE-MEMBERED RINGS ........ 42 SCHEME 24. PHOTOCHEMISTRY OF 1 .............................................................................................................. 43 SCHEME 25. PHOTOCHEMISTRY OF 2 .............................................................................................................. 44 SCHEME 26. PHOTOCHEMISTRY OF 3 .............................................................................................................. 46 SCHEME 27. PHOTOCHEMISTRY OF 4 .............................................................................................................. 48 SCHEME 28. PHOTOBEHAVIOR OF 5 ................................................................................................................ 50 SCHEME 29 ................................................................................................................................ 51 SCHEME 30. PHOTOBEHAVIOR OF 6 ................................................................................................................ 52 SCHEME 31. PHOTOBEHAVIOR OF 7 ................................................................................................................ 54 SCHEME 32. PHOTOCHEMISTRY OF 8 .............................................................................................................. 55 SCHEME 33. PHOTOBEHAVIOR OF 9 ................................................................................................................ 57 SCHEME 34. PHOTOPRODUCTS OF 10 ............................................................................................................. 65 SCHEME 35. PHOTOCHEMISTRY OF 1 1 ............................................................................................................ 66 SCHEME 36. PHOTOBEHAVIOR OF 12 .............................................................................................................. 68 SCHEME 37. PHOTOCHEMISTRY OF 13 ............................................................................................................ 69 SCHEME 38. PHOTOBEHAVIOR OF 14 .............................................................................................................. 73 SCHEME 39. PHOTOCHEMISTRY OF 15 ............................................................................................................ 76 SCHEME 40 ..................................................................................................................................................... 90 SCHEME 41 .................................................................... . ................................................................................ 95 SCHEME 42. LOWEST ENERGY BIRADICAL CONFORMATIONS OF 6 .............................................................. 104 SCHEME 43. REACTTVE GROUND STATE CONFORMATIONS OF 10 ................................................................ 1 15 SCHEME 44 ............................... ................................................................................ 1 19 SCHEME 45 ................................................................................................................................................... 1 l9 SCHEME 46 ................................................................................................................................................... 120 SCHEME 47 ................................................................................................................................................... 123 SCHEME 48 ................................................................................................................................................... 125 SCHEME 49 ................................................................................................................................................... 126 xii SCHEME 50.. SCHEME 5 l. SCHEME 52. SCHEME 53. SCHEME 54. SCHEME 55. SCHEME 56. SCHEME 57. SCHEME 58. SCHEME 59. SCHEME 60. SCHEME 61. SCHEME 62. SCHEME 63. SCHEME 64. SCHEME 65. SCHEME 66. SCHEME 67. SCHEME 68. SCHEME 69. SCHEME 70. SCHEME 71. SCHEME 72. SCHEME 73. SCHEME 74. SCHEME 75. SCHEME 76. SCHEME 77. ................................................................................................................................................. 127 SYNTHESIS OF A-(2-ETHYLPHENYL)PROPIOPHENONE .............................................................. 132 SYNTHESIS OF A-(2-ETHYLPHENYL)ACETONE .......................................................................... 138 SYNTHESIS OF A-MESITYLACETONE ........................................................................................ 140 SYNTHESIS OF A-(2-BENZYLFHENYL)PROPIOPHENONE ......... - ................... 142 SYNTHESIS OF A-(2,4,6-TRIETHYLPHENYL)-B,B,B-TRIDEUTEROPROPIOPHENONE .................... 145 SYNTHESIS OF A-(2,4,6-TRIETHYLPHENYL)ACETONE .............................................................. 150 SYNTHESIS OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETONE ........................................................ 152 SYNTHESIS OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETOPHENONE ............................................. 155 SYNTHESIS OF o-IERT-BUTYLTRIFLUROACETOPHENONE ......................................................... 157 SYNTHESIS OF 2-(2'-(2',3'-D1METHYL)BUTYL)BENZOPHENONE ................................................ 161 PHOTOPRODUCTS OF A-(2-ETHYLPHENYL)ACETOPHENONE ..................................................... 169 PHOTOPRODUCTS OF A-(2,4,6-TRIETHYLPHENYL)ACETOPHENONE .......................................... 172 PHOTOPRODUCTS OF A-TOLYLPROPIOPHENONE .......................................... .. 176 PHOTOPRODUCTS OF A.(2-ETHYLPHENYL)-B,B,B-TRIDEUTEROPROPIOPHENONE ..................... 178 PHOTOPRODUCTS OF A~(2,4,6-TRIETHYLPHENYL)B,B,B-TRIDEUI'ERO PROPIOPHENONE .......... 183 PHOTOPRODUCTS OF A-(2-BENZYLPHENYL)ACETOPHENONE ................................................... 188 PHOTOPRODUCTS OF A—(2-BENZYLPHENYL)PROPIOPHENONE ................................................. 190 PHOTOPRODUCTS FROM A-MESITYLPROPIOPHENONE .............................................................. 193 PHOTOPRODUCTS OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETOPHENONE ................................... 196 PHOTOCHEMISTRY OF TRIMETHYLSILYLENOL ETHER OF 9 ...................................................... 200 PHOTOPRODUCTS OF A-(2-ETHYLPHENYL)ACETONE ............................................................... 202 PHOTOPRODUCTS OF A-MESITYLACETONE .............................................................................. 206 PHOTOPRODUCTS OF A-(2,4,6-TRIETHYLPHENYL)ACETONE .................................................... 210 PHOTOPRODUCTS OF A-(2,4,6-TRIISOPROPYLPHENYL)ACETONE ............................................. 212 PHOTOPRODUCTS OF O-TERT-BUTYLTRIFLUROACETOPHENONE ............................................... 214 PHOTOPRODUCTS OF o-TERT-AMYLBENZOPHENONE ................................................................ 216 PHOTOPRODUCTS OF 2-(2'-(2',3'-DIMETHYL)BUTYL)BENZOPHENONE ...................................... 218 xiii OTBBP OTAMBP ISC SOC nOe CMC PTLC List of Abbreviations o-tert-Butleenzophenone o-tert-Amleenzophenone Intersystem Crossing Spin-Orbit Coupling Nuclear Overhauser Enhancement Critical Micellar Concentration Preparative Scale Thin Layer Chromatography xiv Introduction Many chemical reactions require the input of considerable energy to proceed. This energy is usually introduced as heat. Photochemical methods, however, provide an alternative way to add energy to reactants. The light absorbed by the photoactive portion of the molecule, the chromophore, provides energy to the system. Absorption of electromagnetic radiation by a molecule depends on a correspondence between the radiation energy and the energy of certain molecular transitions. The energy associated with ultraviolet and visible light is required to excite electrons in molecules. The first step in a photochemical reaction is excitation of a molecule through absorption of a photon. Whether this excited molecule leads to a chemical reaction or returns to the original ground State depends upon competition between various intramolecular and intermolecular interactions within the system. 81 T" "\ k. . T1 k hv {i kr Products Products Figure 1. Simplified Jablonski Diagram The photophysical and photochemical processes of molecules can best be described with the Jablonski diagram (Figure 1).1 Absorption of a photon promotes a molecule from the ground state to the Singlet excited state. The excited state molecule can decay to the ground state via emission of light (fluorescence) or radiationless decay. Rate . . 6 9 -l 5 constants for fluorescence and radiationless decay are on the order of 10 -10 s , and 10 - s -l , . . . . . 10 s respectively.2 ’3 Photochemical reactions are also pOSSible from the exc1ted Singlet. The excited Singlet can undergo intersystem crossing to an excited triplet state. Typical , , 7 II -1 rate constants for intersystem crossmg (kisc) are on the order of 10 -10 s .2’3 ’4 ’5 ‘6 ‘7 The excited triplet can decay via radiative deactivation (phosphorescence) with a rate I 6 -l . . . constant, kp, of 10 —10 s .2 It can also undergo radiationless decay and chemical reaction. Quenching'of the excited triplet by energy transfer and/or charge transfer can occur with a rate constant as high as the rate of diffusion in a given solvent I0 -I -1 s (<10 M S ).. Photochemistry of the carbonyl group has been a major target of research for many decades. Aliphatic and aromatic ketones undergo similar photochemical reactions. However, the excited states leading to these reactions are somewhat different for the two. The reactive excited state of aliphatic ketones is the n,1t* state. On excitation, an electron from the oxygen nonbonding orbital is transferred to the 1r*-antibonding orbital of the carbonyl group, creating an electron deficient oxygen. The Singlet is initially formed, but . . - - 3 II -I 2,3.4.5.6.7 intersystem crossmg to the triplet occurs With rate constants of 10 -10 s . Both Sl (lowest excited Singlet) and TI (lowest excited triplet) exhibit reactivity for aliphatic 'r 't I“ w«.. i... ’l N)». .Tm sob ketones. The chemical behavior of the n,1t* triplet state is similar to that of an alkoxy radical. (II—Cleavage, hydrogen abstraction, and charge transfer from an electron donor are the reactions frequently observed.9 "0 "1 Phenyl ketones have two low lying triplets, an n,1r* triplet and a 7t,1t* triplet, whose energy levels are affected by ring substituents and solvents. The 1r,rr* triplet arises from promotion of an electron from a n-bonding to a m-antibonding orbital. This results in a Shift of electron density from the aromatic 1:- system to the carbonyl oxygen, generating an electron rich oxygen, and makes the 1r,1t* triplet much less reactive than the n,rr* triplet. Ketones with a Tt,1t* lowest triplet state do undergo typical n,1t* triplet reactions, but at a much slower rate, which reflects the population of the reacting 11,1” State at equilibriumn'” .14 A wide variety of reactions have been reported in ketone photochemistry. Those relevant to this work are summarized below. 1. Measurements of Quantum Yields and Excited State Lifetimes Quantum yields of photoreactions are defined as the molecules of product formed per photon of light absorbed. Thus, quantum yields can be obtained by measuring the product concentration and the light absorbed during the course of the reaction. The latter is usually measured using actinometers, which are compounds with known quantum efficiencies. The quantum yield for any photochemical reaction can be expressed as the product of probabilities. Thus, for a triplet hydrogen abstraction, (D = cDisc kH TP Br 1/1 = kH + kd PBr = kI/(kr+kBt) Equation 1 where (Disc is the intersystem crossing quantum yield, k“ is the rate constant for hydrogen abstraction, kd is the rate constant for triplet decay other than hydrogen abstraction, r is the triplet lifetime, and P3, is the probability that the intermediate will go to products. In the presence of an external quencher 1 decreases and mathematically becomes: 1/1 = kH + k, + kq[Q] Equation 2 where kq is the bimolecular quenching rate constant. The Stem-Volmer equation is a mathematical relationship between quantum efficiencies in the absence (< Ph Ph/l KP h) _..\[/ +PhCHO PhCOCOPh + Eh I[ } Ph PhCHO+RSSR +Y Ph Scheme 3.8Cage and Non-cage Reactions Baum22 reported a similar study with 2-phenyl-1-indanone and 2,6-diphenyl-1- indanone. Although 2-phenyl-l-indanone cleaves efficiently to isomeric products, 2,6- diphenyl-l-indanone affords little product. This observation is consistent with the fact that 2-phenyl-1-indanone has an n,1r* lowest energy triplet and 2,6-diphenyl-l-indanone has a 1r,1r* lowest energy triplet. O R R CHO hv O. .. #(w — Ph R= H, 2-phenyl- l -indanone R= Ph, 2,6-diphenyl-l-indanone Scheme 4. (II-Cleavage in Cyclic Ketones The photochemical ring opening reactions of 2-hydroxyindan-1-ones have been reported to involve an initial Norrish type I cleavage followed by a 1,4-hydrogen transfer from a benzylic carbon.23 ’24 The possibility of 1,6-hydrogen transfer from the OH was ruled out when photolysis in methanol-d4 resulted in no deuterium incorporation in the aldehyde. In aliphatic ketones, where both singlet and triplet states can be populated, the 25 .26 Turro and co-workers have triplet cleaves about 100 times faster than the singlet. estimated the n,1r* singlet and triplet reactivities towards a-cleavage in several cyclic ketones. Their experimental results indicate that the triplet rate constant was larger than -I 25 5x1010 5", while the singlet rate constant was smaller than 2.5 x 108 s . Yang has reported that the triplet state of di-tert-butyl ketone cleaves with a rate constant of 7- -1 9x109 S , while the cleavage rate constant for the Singlet is only 6x107s'l.26 Phenyl ketones undergo (ii-cleavage at much Slower rates than aliphatic ketones. For example, triplet aliphatic t-butyl ketones a—cleave about 4000 times faster than triplet pivalophenone.27 Electron donating groups on the a—phenyl ring enhance the reaction, indicating an early transition state with some ionic character.21 Other a—substituents also Speed up the reaction, however, the rate constant for the reaction is dependent on the steric congestion in the ground state and was found to be independent of the stability of the resulting . 21 radicals. III. Hydrogen Abstraction Photoexcited carbonyl compounds may undergo a characteristic hydrogen shift to the carbonyl oxygen from hydrogen donors.”29 This process, known as hydrogen abstraction, can Occur between an excited carbonyl and an external donor molecule (intermolecular hydrogen abstraction) or internally within the same molecule (intramolecular hydrogen abstraction). AS for the a—cleavage reaction, hydrogen abstraction may occur from both Singlet and triplet states in aliphatic ketones whereas the abstraction process occurs solely from the triplet excited state in the aromatic ketones. For aromatic ketones, the intersystem crossing of the initially formed Singlet excited state is so fast (~10ll s") that reactions Of the S, state are usually not observed. 30 The reactive excited state for hydrogen abstraction is the n,1r* state. Carbonyl compounds with a It,1t* lowest excited state abstract hydrogen at much slower rates (from a thermally populated n,1t* state, or from the 1t,7r* state)”14 This inefficiency is attributed to a relatively high electron density on the oXygen atom in the 1r,n* state. By comparison, the oxygen atom in the n,1t* state is more reactive toward hydrogen donors because of its radical like character. Hydrogen abstractions by triplet carbonyls are similar to those by alkoxy radicals.“ The n,7r* triplets, like alkoxy radicals have such a high electron demand that the transition states for hydrogen transfer are stabilized by charge transfer. Therefore, electron withdrawing groups near reactive hydrogens Slow down the reaction.”48 Intramolecular hydrogen abstraction is the subject of this research and the material that follows will focus on this subject. Intramolecular hydrogen abstraction from the y—carbon atom is favored but will occur from other positions when there are no hydrogens at the 7 position and the molecular conformations allow other Sites to come into close proximity to the excited carbonyl group. In acyclic systems the rate of abstraction from these Sites is intrinSically lower Since the transition state involves more strain and there is a lower probability that the molecule will attain the required conformation.32 '48 The y-hydrogen abstraction yields a 1,4-biradical. Depending on the conformation of the initially formed 1,4-biradical, two different pathways are possible: (1) If the p orbitals of the radical centers can overlap, a cyclobutanol is the product. (2) If the p orbitals of the radical centers are parallel to the B-bond, this bond will cleave to yield an enol and an alkene (Scheme 5). These cyclization and cleavage reactions are termed the Norrish Type II reaction. The requirement that the orbitals be parallel to the B-bond is equivalent to the need for a planar transition state. This is illustrated in the reaction of a- 10 cyclohexyl-cyclohexanone in which the a,B-carbon-carbon bond must be axial in both rings for a cleavage conformation and, because of the limitations on this conformation, the cyclization process is preferred from both Singlet and triplet states.30 (Scheme 5) hv OH OH Cyclization [Cleavage M Scheme 5. Orbital Requirements of Type II cleavage OH One of the mOSt important reactions of the intermediate biradicals is disproportionation to give back the starting ketone or back transfer. Quantum efficiencies for cyclization and cleavage are determined by the extent of the back transfer (Scheme 6). Quantum yields in Lewis base solvents are generally higher than in hydrocarbons Since the former can hydrogen bond to the resulting hydroxybiradical and prevent the back transfer.33 11 O M ' hV J\/\ k /“\/\ Ph CHZR ——_’ Ph CHzR'A.’ Ph CHZR‘ Ph OH ¢Cyc=(¢isc-kH)TPCyc LCHR' PCYC= kCyc/(kCyc+k-H+ kCleav) kCleav kw RH: k-H/(kCy¢+kCle.av'+'k-H) h - (D = Quantum Yield OH * + H2C=CHR' ELTQH r= Lifetime of the triplet Ph CH2 P= probability of any R. biradical reaction 1”? Scheme 6. Role of Back Transfer in Determination of Quantum Efficiencies A. Conformational Control of Photoreactivity The efficiency of hydrogen abstraction is dependent on the preferred ground state geometry, particularly since excited states can be very Short-lived. Intrarnolecular hydrogen abstraction requires the carbonyl oxygen and the abstractable hydrogen to approach each other in such a way that proper orbital overlap and reaction can occur. This requirement makes photochemical intramolecular hydrogen abstractions sensitive to conformational equilibria, since competitive photochemical reactions can occur at rates faster than conformational motions.34 The competition between conformational change, reaction, and decay (Scheme 7) provides three boundary conditions: 35 (1) Conformational equilibrium (kl, k_, >> k,, kd) (2) Ground state control (kl, k,l << k,, kd) (3) Rotational control (k1~ kd, k,,< k,).34 12 x Y *x Y h . k-l k1 V l )(vvvvvvvvvver hv . X Y kd Decay Scheme 7. Conformational, Rotational and Ground State Control of Reactivity Wagner and Meador have reported that a—(o-alkylphenyl)acetophenones undergo efficient 5-hydrogen abstraction followed by cyclization to yield 2-indanols.36 In their investigation, the rate of hydrogen abstraction by triplet a-mesitylacetophenone was found to be 7 times faster than that of triplet a—(o-tolyl)acetophenone. The slower hydrogen abstraction rate of or—(o-tolyl)acetophenone was attributed to a conformational equilibrium between the reactive syn and the unreactive anti conformers (Scheme 8). Anti (unreactive) Syn (reactive) Scheme 8. Conformational Control of Reactivity 13 In molecules where conformational changes are comparable or Slower than photoreactions, either ground state control or rotational control may occur. Several benzoylcyclohexane derivatives have provided the most clear-cut examples of ground state control in photoreactions. Lewis37 investigated conformational effects in the photochemistry of l-methylcyclohexyl phenyl ketone and a number of substituted analogs. Lewis found that for l-methylcyclohexyl phenyl ketone, there exist two different ketone triplets, each leading to different photoproducts (Scheme 9). The ketone conformer with the benzoyl group in an axial position undergoes y-hydrogen abstraction followed by cyclization to the corresponding 6-hydroxy-l-methyl-6- phenylbicyclo-[3.1.l]-heptane. The ketone conformer having the benzoyl group in an equatorial position cannot undergo hydrogen abstraction Since the carbonyl group is oriented away from those hydrogens. Instead, it undergoes acyl cleavage giving rise to benzaldehyde as well as other products expected from the benzoyl and 1- methylcyclohexyl radicals. 0 Ph 0 Ph . Ph H O ph 9: H ‘ 1 bp .. CH3 “V \CH f , CH3 , ,. CH3 3 f V— Scheme 9. Ground State Control of Reactivity 14 Lewis found that the ratio of the products from the two different pathways is entirely dependent upon the ground state population of each ketone conformer. An example of rotational control of photoreactivity is provided in the 35 33 . . The anti rotamer is much less photoenolization of o-alkylphenylketones (Scheme 10). reactive than the syn rotamer. The lack of an H/D isotope effect on the rate of decay of the anti triplet led to the conclusion that the rate determining step was bond rotation and not hydrogen abstraction.35 O *3 hV / I R CHZR ICHzR: CH2 R \ CHZR . H |OH / / /’ \\ HR \ “CHR Scheme 10. Rotational Control of Reactivity B. Orientational Requirements of Hydrogen Abstraction One unresolved point that has been subject of much debate during the past twenty years has been the preferred transition state geometry for hydrogen abstraction process. In 1968, Turro reported that irradiation of cyclohexane solutions of cis- and trans-2m- propyl-4-t-butylcyclohexanones results in strikingly different photochemistry (Figure 2).39 Photolysis of the cis precursor resulted in the formation of 4-t-butylcyclohexanone, 15 while photolysis of the trans isomer gave the Cis compound as the major product, presumably as the result of (II-cleavage followed by reclosure with epimerization. Based on these results, Turro suggested that the striking contrast in the photochemistry of cis and trans isomers results from a stereoelectronic requirement for the Type II reaction, namely that the hydrogen on the y—carbon to be extracted must be directed toward the half-vacant n orbital of the carbonyl oxygen atom.39 C is Trans Figure 2 Scheffer has studied the Type II reaction in the crystalline state where the reactant geometry is fixed and measurable by x-ray diffraction methods.‘OS d >120 ,2 m X -0... d S 2713 cu: 0° v= 90-1200 1] = 180° Figure 3. Orientational Requirements for H-Abstraction In analyzing their reactivity, he considered the following ground state parameters, as depicted in Figure 3, to be the most important in determining the reactivity: d, the 16 distance between 0 and H; r], the O-H-C angle, v, the C=O-H angle; and a), the dihedral angle that the O-H vector makes with respect to the nodal plane of the carbonyl pi system. In several ketones, for which x-ray crystal structures were obtained, the value of d ranged from 2.3-3.1 A, n from 85-120°, v from 74-103°, and a) from 0-620.”105 ‘40 ‘4' Scheffer suggests the theoretically “ideal” values for these parameters to be those shown in Figure 3. The distance of 2.7 A is the sum of the H and 0 van der Waals radii. Scheffer points that when hydrogen is this close in the ground State, minimal molecular motion is required for hydrogen abstraction in the crystal. Molecular flexibility can, however, allow hydrogen abstraction to occur at longer distances. The deviations from ideality in case of n and a) have long been known from the reactivity of many steroidal ketones. ”’48 Morrison and coworkers reported ab initio studies (3-210 basis set) for hydrogen abstraction from methane by triplet formaldehyde.42 The calculated saddle point for the reaction had the following parameters: (1: 1.18 A, V: 109°, (0:90, n=176°. Sugiyama has reported that in some bridged polycyclic ketones (Figure 4), photolysis results in no hydrogen abstraction, although the hydrogens are extremely close to the carbonyl oxygen.‘13 He attributed this to the unfavorable dihedral angle between the hydrogens and the C-C=O plane. An alternative explanation could be that the abstraction is indeed occurring, but the biradical does not cyclize and instead disproportionates to the Starting material. This seems reasonable since cyclization will put additional strain on an already strained ring system. 17 R = H, OH Figure 4. Effect of Dihedral Angle on Reactivity Photochemical studies of solid complexes of desoxycholic acid and acetophenone derivatives provide examples of intermolecular hydrogen abstraction from the perpendicular direction of the carbonyl plane, but it was concluded that molecular motions within the crystal lattice permitted approach of the reactive hydrogen to the locus of the n orbital of the excited ketone.44 Matsuura suggested. that photocyclization of 2,4,6-triisopropylbenzophenones (Scheme 11), where abstractable hydrogens lie between 55-600 out of the plane of the carbonyl group, occurs from the 1r,1t* state.45 This was because the reaction from the n,1r* state requires rotation about several bonds and therefore, is topochemically unfavorable in the solid state. J\ h .J\OH LOH C'l' . %% ”WI 5 © ; \. _L. \2 ' \/ ’ |/J Scheme 11. Photocyclization of 2,4,6-Triisopropylbenzophenones Sauers and co-workers designed polycylic ketones that contain hydrogen atoms fixed in the plane of the 1: system (Figure 5) with the aim of setting limits on reactivity 18 based on out of plane angles.46 They reported that even when theoretical models did not reveal any barriers attributable to unusual steric strain, no reaction occurred. The short triplet lifetimes of these ketones were attributed to a reversible Norrish type I cleavage that generates very Short lived biradicals.47 A. R = H, Phenyl B. X = H. CH3,C1, Br Figure 5. Effect of Dihedral Angle on Reactivity Wagner suggested that the ease of 1,5-hydrogen transfers in acyclic systems reflects primarily a torsion free, chair-like, six-membered cyclic transition state such that the C-H-O angle is tetrahedral;48 This angle is much less than the linear arrangement calculated by theoretical models. It was also proposed that the torsional strain present in the cycloheptane-like transition state for 1,6-hydrogen transfers is responsible for the slower rate of O—hydrogen abstraction in straight chain systems. Wagner also suggested that coplanar hydrogen abstraction is not a strict requirement for the Type II process and proposed a coszco dependence for abstraction.l 19 Scheffer has reported a boat rather than a chair transition state for hydrogen abstraction in a few cases (Scheme 12). 49 His studies further reinforced the notion that hydrogen and the carbonyl need not be coplanar for the abstraction process to take place. H O hv ° OH ——'> ____, Products Ar . ' Ar H- H . H, 0 Projection down the equatorial carbon-carbon bond of ketone Scheme 12. Boat-Like Transition State for Hydrogen Abstraction Houk noted that a chair-like cyclohexane transition state requires a severely nonlinear geometry for hydrogen transfer.50 He carried out both ab initio molecular orbital calculations and force field modeling which predict the six-membered transition structure for y—hydrogen abstraction (butoxy radical) resembles a five membered ring of heavy atoms, having an envelope Shape like that of a cyclopentane, but with one long bond (2.5 A) between Ca and O.50 The seven-membered cyclic transition structure for 6— hydrogen abstraction (pentoxy radical) also had a chair form much like that of cyclohexane, but with one long bond. In both transition structures the CH0 angle was nearly linear. Based on their calculations, Houk and co-workers have suggested that the preference for a six-membered over a seven-membered transition state iS the result of a more favorable entropy of activation for the six-membered transition state.50 Similar transition state geometries were calculated for the y- and 5—hydrogen abstractions of triplet butanal and pentanal, respectively.“ 20 Sauers and co-workers found a correlation between the overall reaction and the transition state steric energy. Using computational methods, they calculated the transition structure energies for intramolecular hydrogen abstraction at 7 vs. 8 positions for triplet 52 '53 In the lowest energy conformation of cyclodecanone, a y—hydrogen cyclodecanone. lies close (2.54 A) to the carbonyl group. The e-hydrogen, on the other hand, is not only remote (4.12 A), but is on the wrong side of the molecule. However, another low energy conformation was found in which the e-hydrogen lies close (2.48 A) to the carbonyl moiety.53 The out of plane angles are 560 and 90.20 for the y and e hydrogens in the two structures, respectively. lrradiations in cyclohexane are reported to yield only lO-decalols, products of e-hydrogen abstraction. Computed transition structure energies Show a clear preference for reaction via a 6-membered ring, over an 8-membered ring. Static Energy-21.4 keallmol Static Energy=23.8 keel/mot The reason for this apparent paradox lies in the ratio of cyclization vs. disproportionation rates, since there would be a large difference in ease of formation of the two ring systems: 21 decalin vs. bicyclo[6.2.0]decane (Scheme 13).53 This hypothesis was confirmed with the observation that irradiation in tert-butanol produced 1-hydroxybicyclo[6.2.0]decane as the major product. This is due to stabilization of biradical by H-bonding to the solvent which will increase the biradical lifetime and the amount of cyclization. OH 0*3 OH .. —>'“ H H k-8 'hv k-v kccyc O kycyc 0.. OH Scheme 13. Competition Between H-Abstraction and Cyclization Efficiencies The above mentioned studies Show that in most cases the transition state for hydrogen abstraction deviates from ideality. Furthermore, the dependence of reactivity on the value of a) is not clearly understood. This point will be addressed later in this thesis. C. S-Hydrogen Abstraction Intrarnolecular hydrogen abstraction by the carbonyl function occurs from sites other than the y—position when this position has no hydrogens or when the chemical or geometrical features of the molecule allow for effective competition from other positions. In 6—methoxy-valerophenone, for example, B—hydrogen abstraction has the same rate as the y—abstraction due to activation of the 5—position and deactivation of the y-position by the methoxy group.30 The biradicals produced from these 5-abstractions, 22 however, cannot undergo simple cleavage to give electron paired products and in some cases cyclize very efficiently. Wagner reports that irradiation of o-tert-butylbenzophenone (OTBBP) as a solid or in solution results in its quantitative cyclization to 1-phenyl-3,3-dimethyl-l- indanol.54 ’55 ’56 A large solvent effect was also reported on the quantum efficiency and the lifetime of the 1,5-biradical (Scheme 14). CH3 ' “304,0 0 . es." k... > 109 M'1 S'1 at 25°; Ea: 2.5 kcal/mole ; log A= 10.6 biradical lifetime = 43 ns in methanol, 4ns in toluene (”benzene: 0-04 mmethanol= 1-00 Scheme 14. S-Hydrogen Abstraction in OTBBP The large value of kH for OTBBP is attributed to an ideal conformation for hydrogen abstraction. The x-ray structure Shows that one of the tert-butyl hydrogens is 2.46 A from the carbonyl oxygen (HA, (1): 40°), while another is 2.67 A away (H3, m=90°). 23 In order to determine which hydrogen is attacked, an unsymmetrical analog, 0- tert-amylbenzophenone was investigated. o-tert-Amylbenzophenone (OTAMBP) was reported to yield a 60:40 ratio for hydrogen abstraction from methyl (1E and 12) and ethyl (2E and 22) groups of the tert—amyl unit when irradiated in benzene at ambient temperatures (Scheme 15).57 Furthermore, solid state irradiation of OTABP resulted in abstraction from ethyl and methyl positions at a ratio of 70:30. Scheme 15. Photobehavior of OTAMBP This was an interesting result Since the primary and secondary hydrogens in OTABP adopt different positions in the crystal. The x-ray structure Shows the closest ethyl hydrogen is 2.63A from the oxygen (co= 45°), while the methyl hydrogen is 2.53A away but with a different dihedral angle (m=95°). 24 ,The abstraction of methyl hydrogens in the crystal is engaging Since theoretically these hydrogens should not be abstracted. It was mentioned earlier that a—(o-alkylphenyl)acetophenones undergo efficient cyclization to 2-indanols. Introduction of an a-substituent not only decreases the efficiency of indanol formation but also introduces (at-cleavage as an alternative pathway for triplet relaxation (Table 1).58 This phenomenon was explained in terms of the starting geometry of ketones. In the unsubstituted acetophenones, the most stable conformer is the one with the a-aryl group eclipsing the carbonyl. This geometry is very close to the reactive geometry. For the a-substituted acetophenones, however, the a-alkyl substitutent eclipses the carbonyl and the a-aryl group is twisted away, thus creating a poor geometry for hydrogen abstraction. As Shown in Table 1, as the rate of hydrogen abstraction drops, due to a poor starting geometry, reactions such as a-cleavage begin to compete. Table l. a-Substituent Effect on o-Tolylacetophenone Derivatives Ketone chm e..." III, 108 SI a-(o-Tolyl)acetophenone 1 .0 0 1 .2 a-(o-Tolyl)propiophenone 0.05 0.28 0.6 a-(o-Tolyl)isobutyrophenone 0 0.38 0.5 a-(o—Tolyl)valerophenone 0.014 0.032l 2 .2 0.34b a) Type I cleavage b) Type II cleavage 25 D. Nature of the Excited State- Singlet vs. Triplet One of the most intriguing questions in organic photochemistry is whether the differences in Spin multiplicity between singlet and triplet states will be reflected in their reactivity in primary photochemical processes. Yang has shown that in aliphatic ketones the rate of cleavage from the triplet is about 100 times faster than the Singlet.26 Dialkylketones are known to undergo hydrogen abstraction in both the T, and S. 59 ,60 .28 states. Photolysis of the optically active ketone (S)-(+)-5-methyl-2-heptanone Showed that photoracemization occurs from the triplet state, suggesting the existence of a triplet biradical sufficiently long lived to allow racemization at the y—carbon.“ The results obtained with the optically active ketone shOwed that the total quantum yield of observed events from T1 is only 0.14.61 Since (Disc was determined to be 0.11 and the quantum yield for reaction from S, is 0.07, the remaining quantum yield of 0.79 must represent non radiative decay from S,.‘51 This decay appears to lead to no racemization and is not affected by changes in the solvent, which implies that if it does involve formation of a Singlet biradical and subsequent back hydrogen transfer, then the biradical must be extremely short-lived. Stephenson, et al., have also presented evidence which is 2 consistent with the intermediacy of a singlet biradical in the type II reaction.‘5 It has also been suggested that the type II reaction from 81 state may occur via a concerted pathway.28 Heller has proposed that the electronic energy might be transferred into vibrational stretching energy of a C-H bond, with further partitioning into a pair of 26 radicals (or biradical) or to a relaxed ground state.63 Hammond has also postulated that chemical reactions of the excited states are special forms of radiationless decay.64 Salem has calculated the activation energies and surface crossings for singlet and triplet state hydrogen abstractions.65 He showed that Simple symmetry considerations indicate that the n,rr* singlet of the carbonyl correlates with the Singlet diradical product, whereas the ground state correlates with a zwitterionic species.65 Since the plane of symmetry is not maintained in most hydrogen abstractions, an avoided crossing between the excited and ground state surfaces occur (Figure 6). Hydrogen abstraction therefore requires a radiationless decay which can occur easiest at the point of the smallest energy 11.65 difference between the two surfaces. Conversion of the electronic energy into vibrational energy populates the ground state at a maximum, from which relaxation to diradical product or to ground state reactant can occur.”65 In other words, Singlet hydrogen abstraction is inherently inefficient. Scaiano et al. have studied fluorescence quenching of acetone by several hydrogen donors.66 They report the excited singlet of acetone to be 2-10 times more reactive than the triplet toward hydrogen donors. They have ascribed this to a more exothermic reaction from the singlet (singlet being higher in energy than triplet) which results in a lower activation energy for hydrogen abstraction. Furthermore, the lower quantum yield for product formation from the singlet relative to triplet was attributed to a lower efficiency of photoreduction from the singlet, i.e., the actual rate of transfer for the 60,63 hydrogen atom to the excited singlet is lower than in the triplet. The authors attribute 27 this inefficiency to deactivation of the excited state to yield the reactants from an avoided crossing (Figure 6 ) before a radical pair is reached. Correlation Diagram [x Y] 0 A + H-SnBu; A + .SIIBII3 Figure 6. Correlation Diagram It was concluded that the interaction of the singlets with hydrogen donors is not a chemical reaction but a physical quenching mechanism, where the hydrogen donor causes deactivation by accepting part of the electronic excitation energy as vibrational energy . . . 60.65 and promoting internal conversron from S, to SO. ' Turro recently reported that a—(o-tolyl)acetones undergo S-hydrogen abstraction followed by cyclization to yield 2-indanols.67 Quenching studies indicate that O-hydrogen abstraction occurs from the singlet while a-cleavage occurs form the triplet. The rate constants of hydrogen abstraction and intersystem crossing from the singlet in tolylbenzyl 28 ketone were reported to be 2 x109 and 5 x 108 s", respectively.67 a-(o- Tolyl)acetophenone, in contrast, does not cleave but undergoes an efficient (290 nm) or Uranium glass (>334 nm) filters. For solid state irradiations, crytals were packed in capillary tubes and irradiated. The resulting solid (crystal) was then dissolved in CDC13 and analyzed by NMR. The irradiation sources included a medium pressure mercury arc lamp and a Rayonet reactor. The ketones were irradiated at -72°, 0°, room temperature (24°) and 110°C to determine the effect of temperature on product ratios. The desired temperatures were attained by dry ice-ethanol. ice-water, water (at RT) and heated Silicon oil baths, respectively. Irradiation solvents included deuterated benzene, toluene and methanol. In most cases the starting ketones disappeared after 30-40 minutes of irradiation with the corresponding appearance, of diastereomeric mixtures of 2-phenyl-2-indanols. In all cases material balances were > 95%. In the cases of compounds 3, 4 and 7, type I cleavage products were also formed. Irradiation of compound 4 at -72°C, however, did not result in type I cleavage. For compound 9, longer wavelength irradiation (366 nm) was necessary to determine the quantum efficiency, Since the enol product absorbs strongly between 300 and 340 nm. Chemical yields were measured by irradiating 0.01 M solutions of ketones in benzene-d6 or toluene-d3 at room temperature (24°C), with methyl benzoate as an internal standard. The resulting mixtures were then analyzed by NMR or GC or both. Chemical yields at other temperatures were calculated based on product ratios and overall chemical yield at room temperature. The values at high temperature were checked by heating samples that had been irradiated at 42 room temperature to 110°C for three hours. Subsequent analysis gave the same product yields as before, indicating that dehydration was not effecting the product ratios. The structural assignments of indanols were straightforward in most cases. Methyl doublets at 0.6-1.5 ppm were most informative because it is generally accepted that a methyl cis to the phenyl is significantly shielded relative to one trans, as previously . 89 .90 observed in a number of such products. For example, in photoproducts from 0- ethoxybenzophenone, the chemical Shift of methyl group of E isomer was Shifted much more upfield than that of Z isomer, as Shown in Scheme 23.91 o ./ 4.58 ppm ”Ill/CH3 s“ OH \ Ph 0.83 ppm E-isomer Z-isomer Scheme 23. Chemical Shifts of Methyls Trans and Cis to Phenyl in Five-Membered Rings a. a-(o-EthylphenyDacetophenone (I) Irradiation of 1 in benzene or methanol resulted in formation of isomeric 2- phenyl-2-indanols, previously identified by Park.”88 Preparative scale irradiation of l in benzene followed by preparative scale TLC (PTLC) using 3% ethyl acetate in hexane as eluent resulted in separation of the two products which were identified as two isomeric 2- phenyl-Z-indanols (lindZ and lindE) by their NMR Spectra in CDCl3 (Scheme 24). The signal of the trans methyl appears at 1.16 ppm, while that of the cis methyl appears at 43 0.72 ppm. It is also noteworthy that the methine hydrogen cis to the OH is more Shielded than one cis to phenyl. Ph , \W __h\_'__. H O Toluene / H ”CH3 H3C 0H\ 3.32 ppm 0.72 ppm 1.16 ppm 3.47ppm 1 "ME lindZ Scheme 24. Photochemistry of 1 Quantitative analysis of product ratios at several temperatures was achieved by irradiating 0.01 M solutions of l in toluene-d3 through a Pyrex filter followed by NMR analysis. GC analysis of the mixtures showed Similar product ratios as NMR. Quantitative results of temperature studies for compounds 1-8 are listed in Table 23. Irradiation of crystalline 1 at 0°C resulted in formation of lindZ and lindE in a ratio >30: 1. The chemical yields are listed in Table 3. Table 3. Chemical Yields of Photoproducts of a-(2-Ethylphenyl)acetophenone in Toluene at Various Temperatures (A > 290) Temperature (0 C) lindZ lindE -72 92.5% 3.5% 0 91% 5% 24 90% 6% I 10 88% . 8% 44 . b. a-(2,4,6-Triethylplienyl)acetophenone (2) Irradiation of a 0.01 M solution of 2 in benzene-d6 resulted in formation of two isomeric 2-phenyl-2-indanols (2indZ and 2indE, Scheme 25) previously identified by Park.“88 Preparative scale irradiation of 2 in benzene followed by PTLC, using 5% ethyl acetate in hexane as eluent, resulted in isolation of the photoproducts, which were identified from their corresponding NMR spectra in CDCI3. Each isomer showing a methyl doublet, a methine quartet and an AB quartet signal with coupling constants 87.88 similar to previously identified indanols. The NMR Signal of the trans methyl appears at 1.25 ppm while that of the cis methyl appears at 0.70 ppm. Ph hv O Toluene 3.39 ppm 0.70 ppm 1.25 ppm 3-60 PDT" 2 ZindE ZindZ Scheme 25. Photochemistry of 2 The product ratios were determined by integration of the methyl doublet signals of each isomer and by GC analysis. Photolysis of crystalline 2 resulted in 2indZ as the only detectable photoproduct. Chemical yields are listed in Table 4. 45 Table 4. Chemical Yields of Photoproducts of a-(Z,4,6-Triethylphenyl)acetophenone in Toluene at Various Temperatures (1. >290) Temperature (0 C) ZindZ ZindE -72 97% 3% 0 96% 4% 24 95% 5% l 10 94% 6% c. a-(o-Tolyopropiophenone (3) Photochemistry of 3 was previously studied by Wagner and Zhou.58 However, in our effort to study the effect of temperature on product ratios we reinvestigated its photochemistry. Preparative scale irradiation of 3 in methanol followed by PTLC resulted in isolation of eight products, identified by their NMR spectra in CDCl3 as two isomeric 2-phenyl-2-indanols (3indZ and 3indE), two isomeric l-phenyl-2-tolyl-1-propanols (photoreduction products- 3red), two isomeric diarylethanes (or-cleavage products- 3cleav), B-tolylpropiophenone and benzaldehyde. Isolation of two indanol isomers was surprising since the previous investigators had reported the formation of only the Z- isomer.58 The two indanols isolated had the same spectroscopic data as those isolated from 1. The signal of the trans methyl appears at 1.16 ppm while that of the cis methyl appears at 0.72 ppm. Table 23 contains the product ratios of irradiation of 3 at various temperatures. Chemical yields are listed in Table 5. 46 Table 5. Chemical yields of Photoproducts of a-(o-Tolyl)propiophenone in Toluene at Various Temperatures (1 >290) Temperature (°C) 3indZ 3indE B—Phenylpropiophenone a-Cleavage -72 48% 1% - l 7% 0 36% 2% 8% 3 1% 24 30% 2% 8% 35% l 10 20% 2% 12% 44% Ph hv 0 Toluene 3imfl 3indE 0.95 and 1.30 ppm 1.0 and 1.20 ppm 3cleav-Two isomers 3red-Two isomers Scheme 26. Photochemistry of 3 47 d. a—(o-Ethylphenyl)propiophenone (4, 4d,) Irradiation of 4 at room temperature in benzene or methanol results in formation of a mixture of products, most of which were previously identified by Park.88 Preparative scale irradiation of 4 in methanol followed by PTLC, using 3% ethyl acetate in hexane, resulted in isolation of these photoproducts. The products were identified (by their NMR spectra in CDC13) as two isomeric 2-phenyl-2-indanols (4indZZ and 4indZE), two isomeric diethylphenylbutanes (oz-cleavage products- 4c1eav), two isomeric l-pheny1-2- (o-ethylphenyl)-1-propanols (photoreduction products- 4red) and benzaldehyde. The symmetric ZZ-indanol had a doublet signal at 1.19 ppm corresponding to both methyls while the ZE isomer had two distinct methyl doublet signals, the methyl trans to phenyl appearing at 1.3 ppm, and the methyl cis to phenyl at 0.74 ppm. Furthermore, the spectrum of the 22 isomer shows only one methine signal due to the symmetry of the structure while that of the ZE isomer shows two distinct methine signals. Product ratios were determined by NMR integration and GC analysis. The ratio of the two isomeric indanols (4indZZ and 4indZE) from 4 were 5:1 and 1:1 in benzene and methanol respectively. It was important to know which methyl group ends up cis to phenyl in the ZE isomer. Irradiation‘of the oc—trideuteriomethyl 4 showed that only the ethyl methyl ends up cis to phenyl in the ZE isomer, Since the ZE-indanol had a methyl doublet Signal at 0.74 ppm but not one at 1.3 ppm (Scheme 26). The 2H NMR spectra of the 22 and the ZE-indanols Show broad singlets at 1.29 and 1.4 ppm, respectively. These chemical shifts 48 are 0.1 ppm higher than those from the fully protonated 4. The difference could be due to using the DMSO-dg sample rather than CDC], as the reference. 3.5 ppm 0.74 ppm 1.19 ppm 3-23 PPm \ \ \ \ \ H C \ Ph ‘ hv /' 0 Toluene 1.19 ppm 3.5 ppm 1.30 ppm 3.90 ppm 4 4rmrzz mar: 325 ppm 3.20 and 3.26 ppm 3 5 3 28 ppm . ppm \ /0.74 ppm OH 'V’I’Ph C03 \ 3.90 3.5 ppm 1.40 ppm PPm 1.29 ppm mam, Mums-d. Scheme 27. Photochemistry of 4 49 An interesting solvent effect was observed in the photolysis of compound 4. Irradiation in toluene-d3 results in a 1:9 ZZ/ZE ratio at -72°C (Table 23). However, irradiation at ~72°C in methanol results in formation of 4indZE as the exclusive photoproduct. Type I cleavage products were not observed in the low temperature irradiation mixtures. Irradiation of crystalline 4 was unsuccessfirl Since the crystals melted during photolysis. IndanolS were the only products observed in the oil obtained from crystal irradiations, in a 1:2 ZZ/ZE ratio. Low temperature irradiation of crystals at 0 and -72°C resulted in no reaction. Chemical yields are listed in Table 6. Table 6. Chemical Yields of Photoproducts of a—(2-Ethylphenyl)propiophenone in Toluene at Various Temperatures (1. >290 nm) Temperature (0 C) 4indZZ 4indZE a-Cleavage -72 9% 91% - O 27% l 8% 47% 24 4 l % 7% 46% iiiiiii l l 0 3 7% 4% 5 6% e. a-(2,4,6—Triethylphenyopropiophenone (5) Irradiation of 0.01 M solutions of 5 in benzene-d6 and methanol-d4 at room temperature results in formation of two isomeric 2-phenyl-2-indanols (SindZE and SindEZ, Scheme 28) previously identified by Park.88 Preparative s‘cale irradiation of 5 in toluene followed by PTLC, using 7% ethyl acetate in hexane, results in isolation of 50 photoproducts which were identified by their corresponding NMR spectra in CDC13. Chemical yields are listed in Table 7. Table 7. Chemical Yields of Photoproducts of a—(2,4,6-Triethylphenyl) propiophenone in Toluene at Various Temperatures (A > 290 nm) Temperature (° C) SindZE 5indEZ -72 86% l 4% 0 60% 40% 24 54% 46% I 10 40% 60% 3.45 ppm 0.86 ppm 5 5mm SindEZ Scheme 28. Photobehavior of 5 The structural assignment for the isomeric indanols 5indZE and 5indEZ was a difficult task in the fully protonated species since both isomers had NMR signals corresponding to methyl doublets cis and trans to the phenyl ring. (Scheme 29) 51 3.45 ppm 1.29 ppm 5indZE-d3 SindEZ-d3 Scheme 29 In the ZE isomer, the trans methyl signal appears at 1.47 ppm while that of the cis methyl appears at 0.86 ppm. In the EZ isomer, the trans methyl Signal appears at 1.29 ppm while that of the cis methyl appears at 0.82 ppm. Introduction of an a—CD3 group in place of or—CH3 made the assignments much easier, Since the ZE isomer displayed only the methyl doublet signal cis to phenyl, while the EZ isomer had one trans to phenyl. The 2H NMR spectra of the ZE and the EZ-indanols Show singlets at 1.48 and 0.82 ppm (CDC13 reference), respectively. Low temperature irradiation at -72°C in toluene and methanol resulted in 6:1 and 12:1 ZE/EZ ratios, respectively. Irradiation of crystalline 5 results in formation of 5indZE as the only observable product (5% conversion). Irradiation of crystal for 22 hours resulted in an oil, the NMR of which indicated the presence of both indanols 5indZE and 5indEZ in a 17 to 1 ratio. Irradiation of 5 on silica resulted in a 10:1 ZE/EZ ratio of indanols. Table 23 contains the product ratios of irradiation of 5 at various temperatures. 52 fl a-(o-BenzylphenyDacetophenone(6) Irradiation of 6 in benzene resulted in formation of two isomeric 2-phenyl-2- indanols (6indZ and 6indE, Scheme 30) previously identified by Park.88 Preparative scale irradiation in toluene followed by PTLC, using 5% ethyl acetate in hexane, resulted in isolation of the photoproducts which were identified by their corresponding NMR spectra. Stereochemical assignment of the two isomers was made using nuclear Overhauser enhancement (nOe) experiments. Irradiation of the doubly benzylic methine signal at 4.61 ppm in the E-isomer in benzene-d6 resulted in enhancement of the OH signal at 2.45 ppm (5%), while Similar irradiation in the Z-isomer resulted in no such enhancement. The signal at 2.45 ppm disappeared upon addition of two drops of D20 to the solution. The product ratios were determined by NMR and GC analysis. For the NMR analysis, the ratio of the AB quartet signals of the Z-isomer, which appears at 3.4 and 3.65 ppm, to that of the E-isomer, which appears at 3.3 and 3.85 ppm, was used. Table 8 contains the product ratios of irradiation of 6 at various temperatures. Irradiation of 6 in methanol resulted in a 1:1 ratio of indanols. Irradiation of cystalline 6 also results in a 1:1 Z/E indanol ratio. Chemical yields are listed in Table 8. Ph Ph 0 Toluene Scheme 30. Photobehavior of 6 53 Table 8. Chemical Yields of Photoproducts of a-(Z-Benzylphenyl)acetophenone in Toluene at Various Temperatures (1. > 290 nm) Temperature (° C) 6indZ 6indE -72 41% 59% O 50% 50% 24 55% 45% I 10 60% 40% g. a-(o-Benzylph enprropiophenone (7) Irradiation of a 0.01 M solution of 7 at room temperature in benzene-d6 resulted in formation of a mixture of products. Preparative scale irradiation in toluene followed by PTLC, using 3% ethyl acetate in hexane, resulted in isolation of photoproducts which were identified by their NMR spectra (in CDC13) as two isomeric 2-phenyl-2-indanols (7indZZ and 7indZE), two isomeric di(benzylphenyl)butanes (OI-cleavage products- 7cleav) and benzaldehyde (Scheme 31). Although the chemical shift of the methyl doublet Signals from both indanols indicated a trans configuration relative to the 2- phenyl, the stereochemical orientation of the 3-phenyl groups in the two isomers was ambiguous. NOe experiments were performed. Irradiation of the benzylic methine signal of one isomer at 4.50 ppm resulted in a small enhancement (0.47%) of the methyl doublet at 1.30 ppm. However, irradiation of the benzylic methine signal of the other isomer at 4.95 ppm did not result in signal enhancement of the methyl doublet at 1.25 ppm. Thus, 54 the former was assigned as the 213 while the latter was assigned as the Z2 isomer. Irradiation of 7 at -72°C resulted in formation of both type I and type 11 products. Two indanols were formed in a 1:1 ratio at all temperatures studied. The chemical yields were measured by NMR analysis and were 55% and 35% for indanols and d-cleavage products at room temperature, respectively. Ph Ph hv O Toluene 7 4.5 ppm 7indZE 320 ppm 1.10 ppm 1.10 ppm 7cleav-Two isomers Scheme 31. Photobehavior of 7 h. a-Mesitylpropiophenone (8) The photochemistry of compound 8 was previously studied by Wagner and Zhou,58 but temperature effects on the diastereoselectivity of the biradical closure were not studied. Irradiation of 8 in benzene results in formation of two isomeric 2-phenyl-2- 55 indanols (8indZ and 8indE, Scheme 32). Preparative scale irradiation followed by PTLC. using 3% ethyl acetate in hexane, resulted in isolation of photoproducts which were identified by their NMR spectra in CDCl;,. Analysis of product ratios by NMR was simple since the methyl doublet signal from the Z-isomer appeared at 1.36 ppm while that for the E-isomer appeared at 0.7 ppm. The product ratios were determined by both NMR and GC analysis. Table 23 contains the product ratios at various temperatures. Chemical yields are listed in Table 9. Table 9. Chemical Yields of Photoproducts of a—Mesitylpropiophenone in Toluene at Various Temperatures (1» > 290 nm) Temperature (0 C) 8indZ 8indE -72 96% 4% 0 94% 6% 24 9 1 % 9% I 10 82% l 8% Ph hv O Toluene Scheme 32. Photochemistry of 8 56 i. a-(2,4,6-Triilsopropylphenyl)acetophenone (9) The photochemistry of 9 (Scheme 33) was previously studied by Wagner, Meador and Zhou.87 Here, a systematic study of product ratios as a function of temperature and conversion is presented. Irradiation of 9 at -72 °C in both methanol and toluene forms only enols (9ean and 9enlE), together with 5-10% benzaldehyde. Only Z-enol was observed in toluene at low temperature, while a 4:1 Z/E enol ratio was observed in methanol. The Z-enol was identified by the following NMR signals in toluene: a vinylic CH signal at 6.1 ppm, an OH signal at 4.8 ppm and methyl doublet signals at l.2-1.30 ppm. The E—enol has a vinylic CH signal at 6.4 ppm, an OH signal at 4.75 ppm and methyl doublet Signals at 1.1-l.2 ppm (in toluene-d3). The vinylic CH signal of the Z- isomer is further upfield than that of the E-isomer presumably due to partial shielding by the phenyl group. The enols are stable for days at room temperature in the dark, but tautomerize completely to ketone within 5 hours at 90 °C. Upon irradiation at 313 nm at room temperature they revert to 9, whereas the Z-trimethylsilyl enol ether of 9, synthesized by treating 9 with KH and trimethylsilylchloride, affords only the E-isomer. The Z:E enol ratio in toluene decreases as irradiation time increases, ranging from 10:] to 2:1. A study of product yields as a function of conversion, temperature, and excitation wavelength (Table 12) indicated that indanol (9ind) builds up very slowly following several interconversions between ketone and enol at 313 nm excitation but is obtained in a constant quantum yield at 366 nm (Table 11), where the enol does not absorb (Table 10). Irradiation of 9 at 366 nm thus results in a constant 8:1 enol/indanol ratio. Irradiation of crystals of 8 produces only Z-enol up to 20% conversion. 57 Table 10. Molar Absorptivity Coefficients (M'lcm'l) of 9 and its Enol at Various Wavelengths Compound 83,3 833,, 8366 9 79 70 = 6.2 Enol of 9 1230 22 0 Z-Trimethylsilylenol ether of 9 1912 98 0 6.40 m ppl 4.75 ppm \ Ph H \ hv OH 0 Toluene , —— / "’1 + 0 Ph 1.29 ppm (in CDCl 3) 0.78 ppm (in CDCI 3) 9 9ind 9enlE 1.95 ppm (in CDCI 3) 6 1 P131“ 4 79 ppm (in CDCl 3) / H3C H H/ 110;me —_:\75+ ppm 9ean 9alc Scheme 33. Photobehavior of 9 Table 11. Product Quantum Yields 58 of 9 as a Function of Conversion and Wavelength 1. (nm) °/oConversion [Enol] (Dem, ' [Indanol] (bindmo, "b 3 I 3 6 0.0065 0.35 - - 313 15 0.013 0.234 0.003 0.062 313 19 0.014 0.15 0.006 0.059 313 24 0.014 0.09 0.009 0.052 366 10 0.13 0.64 - - 366 18 0.18 0.64 0.024 0.085 366 25 0.24 0.64 0.034 0.085 a) Quantum yields were measured by NMR (b) Quantum yields were measured by GC [Ketone]= 0.0143 M (GC studies), [Ketone]= 0.0983 M (NMR studies) [Valerophenone]= 0.024 M (GC studies), [Valerophenone]= 0.1165 M (NMR studies) [C20 standard]= 0.0033 M (GC studies), [Methyl benzoate-standard]= 0.03 M (NMR Studies) 59 Table 12. Product Ratios of Irradiation of 9 Under Various Conditions T (° C) 1. (nm) Solvent % Conv. 9ind 9(2an 9enlE Cleavage -72 >290 Toluene >95 0 90 0 1 0 -72 >290 Methanol >95 0 72 1 8 10 24 >290 Benzene 40 20 73 7 0 24 >290 Benzene 50 28 62 7 3 24 >290 Benzene 64 30 53 7 1 0 24 >290 Benzene 70 50 16 8 26 24 >334 Benzene 17 29 71 - - 24 >3 34 Benzene 3 23 24 63 1 3 - 24 >3 34 Benzene . 46 26 59 15 - 24 >3 34 Benzene 66 20 53 24 23 24 >334 Benzene >95 55 0 0 45 90 >290 Toluene 24 1 7 66 1 7 0 90 >290 Toluene 38 3 5 52 l 3 0 90 >290 Toluene 70 69 25 6 0 90 >290 Toluene >95 1 00 0 0 0 60 C. Steady-State Photokinetics. The quantum yields were measured by irradiation of degassed solutions of ketones (0.025-0.04 M) in tubes containing a fixed amount of internal Standard parallel to valerophenone actinometer. For quenching studies, these tubes also contained varying amounts of 2,5-dimethyl-2,4-hexadiene quencher. Product yields at 5-18% were measured using CC or NMR and were converted to quantum yields. Stern-Volmer plots were linear with slopes equal to qu. The kinetic data are listed in Table 13 and Table 14. Triplet lifetimes, based on a kq value of 6x109 M'ls'l, are also listed.30 The errors represent deviation of 2-4 measured values from the average. Table 13. Lifetimes of Triplet Aceto- and Propiophenones in Benzene Ketones kqt’ M" “1, 1098-1 1 8.04 i 0.4 0'75 """"" 2 6.95 i 0.3 0'86 """""" 4 17.40 i 0.8 0'34 ............. 5 7.98 i 0.4 0.75 ............. 6 3.99 i 0.2 1.5 61 Table 14. Quantum Yields of Photoproducts from Aceto- and Propiophenones in Benzene Ketones (Dcyc (DCleavage 1 0.48 i 0.02 - 2 0.48 i 0.02 - 4 0.064 i 0.004 0.43 i”. 0.02 5 0.27 i 0.015 - 6 0.40 i 0.011 - 7 0.10 i’ 0.005 0.06 i 0.005 9 0.055, 0.0853 i 0.003 - a) Quantum Yield measured at 366 nm. 62 II. a-Arylacetones A. General Preparation of the Ketones. a-Arylacetones were prepared by chloromethylation of the appropriate arylbenzene, cyanation with sodium cyanide, hydrolysis with concentrated hydrochloric acid, and coupling with methyllithium. AS a result, the following compounds were prepared and/or used in this Study. B. Irradiation of Ketones NMR scale irradiations were carried out using 0.01 M solutions of ketones in deuterated benzene and toluene. The solutions were irradiated through a Pyrex filter (>290 nm). The ketones were irradiated at -72°, 24° and 110°C to determine the effect of temperature on product ratios. In most cases, the starting ketones disappeared after 24 hOurs of irradiation with corresponding appearance of mixtures of 2-methyl-2-indanols 63 and (Jr-cleavage products. In the case of compounds 10 and 12, two isomeric indanols were detected after irradiation. The isomeric ratios of these indanols were determined by GC and/or NMR. Chemical yields were measured by irradiating 0.01 M solutions of ketones in benzene-d6 at room temperature (24°C) using methyl benzoate as an internal standard. The resulting mixtures were then analyzed by NMR or GC or both. Chemical yields at other temperatures were calculated based on product ratios and overall chemical yield at room temperature. The values at high temperature were checked by heating the solution, which had been irradiated at room temperature, to 110°C for three hours followed by analysis to ensure that dehydration of indanols was not affecting the product ratios. In most cases material balances were > 95%. Stem-Volmer quenching experiments using 2,5-dimethyl-2,4-hexadiene as quencher, Show a quenchable a-cleavage reaction while no quenching of indanol formation was observed. Our experiments thus indicate that 8—hydrogen abstraction occurs from the singlet while a-cleavage occurs from the triplet in a-alkylphenylacetones, in agreement with Turro’s67 results. C. Identification of Photoproducts a. a-fl-Ethylphenybacetone (10) The behavior of 10 is temperature and environment dependent. Irradiation of 10 in benzene resulted in formation of a mixture of compounds. Preparative scale irradiation followed by PTLC, using 3% ethyl acetate in hexane, resulted in separation of Photoproducts which were identified as two isomeric 2-methyl-2-indanols (10indZ and lOindE, Scheme 34) and 1,2-di-(o-ethylphenyl) ethane (or-cleavage product- l0cleav). 64 Analysis of product ratios in benzene by NMR was not easy due to overlapping peaks, thus irradiations were performed in toluene which gave much better peak separations. The structural assignment for the isomeric indanols 10indZ and 10indE proved to be a difficult task since all methyl Signals appeared in close proximity to each other in the NMR Spectrum. The NMR spectra of the cis and trans l-methyl-2-indanols were previously reported in literature92 , however, the presence of the methyl group at the 2- position Should change the chemical Shifts, so comparisons are not reliable. The structural assignments of the indanols were based on the use of shift reagents and nOe experiments. Addition of Rondeau’s reagent, tris(6,6,7,7,8,8,8-heptafluoro-2,2-dimethy1-3,5- octanedionato) praseodymium, to 0.01 M solutions of each indanol in CDC13 caused an upfield shift of all proton signals. The methine Signal at 3.08 ppm of the minor isomer moved upfield (to 2.97 ppm) twice as much as its methyl signal at (1.19 ppm to 1.16 ppm), while the upfield shift of both methyl (1.28 to 1.0 ppm) and methine (2.97 to 2.68 ppm) signals of the major isomer were comparable. Addition of europium shift reagent caused a similar downfield shifi of the signals but caused peak broadening which made assignments difficult. Furthermore, irradiation of the methine signal in the minor isomer caused an nOe enhancement of the OH signal. These data strongly suggest that the minor isomer has E-stereochemistry. The product ratios and indanol diastereoselectivities were measured by NMR analysis. The Z:E indanol ratio was determined by the ratio of the methyl doublet signal of the Z-isomer at 1.12 ppm to that of the E-isomer at 1.0 ppm in toluene-d8. Irradiation of 10 resulted in 20:80, 50:50 and 60:40 indanol/diarylethane ratios at -72°C, 24°C and 90°C, respectively. Furthermore, the ratio of the two isomeric 65 indanols (10indZ: 10indE) were 3.2:1, 2.521 and 1.421 at 0°C, 24 °C and 90 °C . respectively. Irradiation of 10 inside sodium dodecylsulfate micelles (0.4 g in 100 m1 of water, 14 mM, critical micellar concentration (CMC) = 10 mM)93 at 24°C resulted in a 75:25 indanol/ci—cleavage ratio, while the lOindE: 10indZ ratio remained 2.5:]. Chemical yields are listed in Table 15. Table 15. Chemical Yields of Photoproducts from a-(2-Ethylphenyl)acetone in Toluene at Various Temperatures (1. > 290 nm) Temperature (° C) 10indZ lOindE l0cleav -72 20%” -3 80% 0 34% 1 1% T 47% 24 33% 13% 48% 1 10 28% 28% i 39% a. Only the Z-indanol was observed in the product mixture irradiated at -72°C, the E- isomer might have been present in trace amounts but could not be detected by NMR. C I \ / H CH3 1-23 131"“ 2.97 ppm 3‘08 ppm 10 101ng 10MB 10cleav Scheme 34. Photoproducts of 10 66 b. a-Mesitylacetone (11) Irradiation of compound 11 (Scheme 35) in toluene-d8 resulted in formation of two products which were identified as an indanol (llind) and a diarylethane (1 lcleav) by their NMR Spectra. Preparative scale irradiation in toluene followed by PTLC, using 3% ethylacetate in hexane, resulted in separation of photoproducts. The product ratios were determined by comparing the NMR integration of the AB quartet signal of the indanol at 3.0 ppm to that of the methylene Signal of the diarylethane at 2.8 ppm. Irradiation of 11 at -72 °C, 24°C and 110°C resulted in a 0:100, 60:40, and 70:30 indanol/diarylethane ratio, respectively. No reaction takes place upon irradiation of crystals. Chemical yields are listed in Table 16. 1.30 ppm (in CDC13) 2-80 ppm (in CDCI 3) 1‘ llind llcleav Scheme 35. Photochemistry of 11 67 Table 16. Chemical Yields of Photoproducts from a-Mesitylacetone in Toluene at Various Temperatures (1. > 290 nm) Temperature (0 C) llind llcleav -72 0 i 98% 24 56% 42% l 10 69% 29% c. a-(2,4,6-Triethylphenybacetone (12) Irradiation of compound 12 in benzene-d6 or toluene-d3 resulted in formation of a mixture of two isomeric indanols(12indZ and 12indE) and a-cleavage products, 12cleav and acetaldehyde (Scheme 36). Preparative scale irradiation in benzene followed by PTLC, using 5% ethyl acetate in hexane, resulted in separation of the indanols as a mixture from the diarylethane. The indanol/diarylethane ratios were measured by NMR analysis to be 20:80, 70:30, and 85:15 at -72°C, 24°C, and 110°C, respectively. They were determined from the ratio of the methyl signal of the Z-indanol at 1.26 ppm to that of the methylene of the diarylethane at 2.5 ppm. The ratio of the two isomeric indanols, measured by NMR and GC, was 10:1 in favor of the Z-isomer for irradiations at 24°C in benzene. The indanol ratios were determined by NMR integration of the methyl doublet signal of the Z-indanol at 1.19 ppm to that of the E-indanol at 1.11 ppm in C6D6. The peaks for the two isomeric indanols overlap and separation is difficult. The Z- Stereochemistry for the major indanol was based on the comparison of the peaks to that of the Z-indanol of o-(ethylphenyl)acetone. Chemical yields are listed in Table 17 . 68 Table 17. Product Chemical Yields of a-(2,4,6-Triethylphenyl)acetone in Toluene at Various Temperatures (1. >290 nm) Temperature (°C) 12indZ 12indE 12cleav -72 l 7% ~2%a 7 l % 24 5 8% 6% 27% 1 l 0 71 % ~6%a l 2% a) The yield of the 12indE was estimated based on the 12indZ yield and a constant 10:1 indanol ratio, since ratios at other temperatures were hard to determine due to overlapping peaks. \ l- \ i / 0 H H / 2.50 ppm 1.19 m 1.11 m 99 2.72 ppm 99 2.56 ppm 12 IZInfl 121:1 dE 12cleav Scheme 36. Photobehavior of 12 d. a-(2,4,6-Triisopropylphenyl)acetone (13) The photobehavior of 13 (Scheme 37) at room temperature is conversion dependent. At low conversions the Z-enol (Ben!) is the major photoproduct. It was identified by the following NMR signals in benzene: an allylic methyl at 1.8 ppm, a vinylic CH at 5.4 ppm and a OH at 4.4 ppm. The Z-stereochemistry was assigned based on its stability relative to the E-isomer and by comparison of its NMR data to the 69 literature values (Z-enol of phenylacetone is reported to have a vinylic CH signal at 5.0 ppm in benzene).94 At high conversions an indanol (13ind) and a diarylethane (13cleav) are the only observable photoproducts. The indanol is identified by the following NMR signals in benzene-d6: three methyl singlet signals at 1.10 at 1.30 and 1.36 ppm, an OH Signal at 1.8 and an AB quartet signal at 2.95 at 2.99 ppm (in CDC13). Formation of the enol is interesting since it mimics the behavior of the acetophenone analog. The enol of 13, however, is not as Stable as acetophenone enols and tautomerizes back to ketone in a few hours in the dark at 24°C, and in a few minutes at 110°C. The behavior of 13, like its analogs, is also temperature dependent. At -72°C, only cleavage products are formed while at 110°C indanol is the only photoproduct. At room temperature Z-enol, indanol and cleavage products are formed but no reaction takes place upon irradiation of crystals. Table 18 lists product chemical yields as a function of conversion and temperature. The product ratios are determined by NMR integration of the vinylic CH signal of the enol, the methyl singlet signal of the indanol and the methylene singlet signal of the diarylethane. 5.2 ppm 1.36 ppm(CDCl 3) / l hv / O “'CH .\ C 6D 6 3 + H H H30 CH3 ‘ \ l 1.10 and 1.30 ppm(CDC13) 2.90 ppm(CDCI 3) l3 131m! 1301! 13cleav Scheme 37. Photochemistry of 13 70 Table 18. Product Chemical Yields of a-(2,4,6-Triisopropylpheny1)acetone as a Function of Conversion and Temperature Temperature(°C) Solvent %Conversion 13¢:an 13ind 13cleav -72 Toluene >95 0 0 100 24 Benzene 36 46 40 14 24 Benzene 55 33 45 22 24 Benzene 74 23 47 30 24 Benzene 80 1 7 48 3 5 l 10 Toluene >95 0 100 0 D. Steady-State Photokinetics. The quantum yields were measured by irradiation of degassed solutions of ketones (0.02-0.03 M) in tubes containing a fixed amount of internal standard parallel to a valerophenone actinometer. For quenching Studies, these tubes also contained varying amounts of 2,5-dimethyl-2,4-hexadiene quencher. Product yields at 5-18% were measured using GC or NMR and were converted to quantum yields. Stern-Volmer plots were linear with Slopes equal to kq‘t. The kinetic data are listed in Table 19 and Table 20. Triplet lifetimes, based on a kq value of 6x109 M'ls'l, are also listed.30 The errors represent deviation of 2-4 measured values from the average. 71 Table 19. Triplet Lifetimes of a-Arylacetones in Benzene at Room Temperature (1.= 313 nm) Ketones k4, M'l UT 11 109 s'1 10 ' 6.7 i 0.3 0.89 11 31.4i1.5 0.31 ' 13 107.1 i 5 0.009 Table 20. Quantum Yields of Photoproducts of a-Arylacetones in Benzene at Room Temperature (A=313 nm) Ketones (DC,c (Dwarykmm 10 0.0128 i 0.0005 0.0156 i 0.0005 11 0.085 i 0.003 0.054 i 0.002 12 0.036 i 0.003 0.018 t 0.002 13 0.012 ((DEno, = 0.028) 0.005 i 0.0002 72 III. 2-tert-Butyl trifloroacetophenone A. Preparation 2-tert-Butyl trifloroacetophenone (14) was prepared by nitration of the tert- butylbenzene followed by bromination, reduction of nitro group, formation and reduction of diazonium salt, formation of Grignard and reaction with ethyl triflouroacetate. “j: HNo3 2 -, V/ 11.50 H2304 Ag2504 B. Irradiation Conditions 1. BuLi 2. CF3COOEt NMR scale irradiations were carried out using 0.01 M solutions of 14 in deuterated benzene, methanol or toluene. The solutions were irradiated through a Pyrex filter. The starting ketone disappeared after 2 hours of irradiation with corresponding appearance of mixtures of 3,3-dimethyl-1-triflouromethyl-1-indanol (14ind)and 1-{2’-(3- (2”—methyl)propargyl)-phenyl}triflouromethylethanol (l4alc). Material balance was > 95%. C. Identification of Photoproducts Large scale irradiation was performed in benzene. The products were isolated by PTLC using 30% ethyl acetate in hexane solution as eluent. The products are an 73 unsaturated alcohol and an indanol and are formed in a 10:1 ratio (Scheme 38). The unsaturated alcohol was the predominant photoproduct in both methanol and hydrocarbon solvents (benzene). The unsaturated alcohol is identified by the following NMR signals: an allylic methyl Signal at 1.8 ppm, an OH Signal at 2.4 ppm (d, J=4.8 Hz), an AB quartet signal at 3.4 ppm, two vinylic CH signals at 4.5 and 4.8 ppm and a methine (dq, J=4.8, 6.8 Hz) signal at 5.3 ppm (in CDC13). Furthermore, l9F NMR of the alcohol showed a doublet (J=6.8 Hz) signal at -2.0 ppm relative to ethyl trifluoroacetate standard. The indanol had two methyl singlet Signals at 1.37 and 1.42 ppm and an AB quartet at 2.2 and 2.45 ppm (in CDC13). A weak w-type coupling was observed in the indanol between the CF, group and the trans hydrogen on the five-membered ring (2.2 ppm). Chemical yields were measured by irradiating 0.01 M solutions of 14 in benzene-d6 at room temperature in the presence of a methyl benzoate standard. NMR analysis of the resulting mixture showed it to consist of 88% Male, and 9% Mind. 4.88 ppm 1.8 ppm 4.5 ppm 2.20 ppm \ 5-3 1’1"" 0 H H H CF3 hV CF3 OH \ I 2.8 ppm 2.42 ppm 14 Mind 14alc Scheme 38. Photobehavior of 14 74 IV. 2'-(2,3-Dimethyl-2-butyl)benzophenone A. General Preparation 0-(2,3-Dimethyl-2-butyl)benzophenone was prepared by addition of isopropyl Grignard to acetone, treatment of the resulting alcohol with concentrated HCl, Friedel-Crafts alkylation of benzene with the resulting alkyl chloride, nitration, bromination, reduction of nitro group, formation and reduction of diazonium salt, formation of Grignard and coupling to benzoyl chloride. >‘Br 1 Mg L7<_fl:_l_’ HC6H6 2. (CI-I co /' 3h FeCl3 OW H2504 Br H2 HCl PtO 2.PhCOCl 2. “31,02 2 NHZ B. Irradiation Conditions Brz H2304 A82504 NMR scale irradiations were carried out using 0.01 M solutions of 2'-(2,3- dimethyl—2-butyl)benzophenone in deuterated benzene, methanol and toluene. The 75 solutions were irradiated through a Pyrex filter. In most cases the starting ketone disappeared after 30 minutes of irradiation with corresponding appearance of mixtures of isomeric indanols (lSindmZ, lSinde, lSindip, lSalc). The quantum efficiencies were higher in methanol than in benzene. Chemical yields were measured by irradiating 0.03 M solutions of 15 in benzene and methanol with methyl benzoate as a standard. The resulting solutions were then analyzed by NMR. In all cases, material balances were >95%. C. Identification of photoproducts. The indanol products were difficult to isolate because of rapid dehydration on silica gel. An unsaturated alcohol similar to those obtained from irradiation of o-tert- butylaceto- and trifloroacetophenones was also observed as a photoproduct. o-(2,3-Dimethyl-2-butyl)benzophenone (0.011 M) in deuterated benzene was irradiated with Pyrex-filtered light from a medium pressure mercury arc lamp. The reaction was complete within 1.5 hours of irradiation and four products formed (Scheme 39). The reaction mixture had to be analyzed immediately after irradiation because photoproducts dehydrated rapidly. 15inde, lSindmZ and lSalc (Scheme 39) measure abstraction of a primary methyl hydrogen while 15indip measures abstraction of a tertiary hydrogen. This reaction was repeated in several solvents and product ratios were determined by NMR. The stereochemical assignments of lSinde and lSindmZ were made by comparison of the NMR data to those of E- and Z-3-ethyl-3-methyl-1-phenyl-l - indanol (tamlE and tale), photoproducts of OTAMBP.” The NMR data of tamlE 76 and tale in benzene indicate that the methyl group of the ethyl substituent appears at 0.6 ppm in the E-isomer with a methyl singlet signal at 0.90 ppm which are, respectively, upfield and downfield relative to the signals in the Z-isomer (0.5 and 1.10 ppm respectively). 0.62 ppm 0.78 ppm CH3 \ CH3 0.85 ppm 0 ..~\‘CH3 \\ \ hV . ..~“ CH3 C D | Ph 6 6 1.40 ppm + / "9,! 3'” HO P“ HO Ph 15 15mm lSinde 1.10, 1.16, 1.18, 1.45 ppm 3.26 ppm (collapsed AB quartet) OH + Ph / \ 0.92 and 0.95 ppm 5.92 ppm lSindip ‘50“, Scheme 39. Photochemistry of 15 0'5 ppm ”0 PM“ 0.9 ppm 0.6 ppm 77 Thus, the isomer with the isopropyl doublet signals at higher field and the methyl singlet signal at lower field was assigned the E-stereochemistry. lSindmZ has two isopropyl doublet signals at 0.62 at 0.78 ppm and a methyl singlet signal at 1.40ppm while the isopropyl and methyl signals of lSinde appear at 0.76, 0.85 and 1.10 ppm, respectively. Identification of 15alc by NMR was also simple, since lSalc shows similar NMR signals to the unsaturated alcohol of 14 with two vinylic CH signals appearing at 4.47 and 4.84 ppm, a bibenzylic OH signal at 5.92 ppm, an AB quartet signal at 3.26 ppm and two isopropyl doublet signals at 0.92 and 0.95 ppm. The reaction proceeds in solid as well as solution similar to tert-amylbenzophenone Table 21 shows the chemical yield in benzene and methanol at room temperature along with product ratios under various conditions. Table 21. Effect of Temperature and Medium on Product Ratios of 15 Reaction T (°C) 15indmZ 15inde 15alc lSindip medium Benzene 24 27 52 7 l4 Methanol 24 32 32 l 3 23 Toluene 1 10 22 29 8 41 Toluene -72 3 3 48 5 1 4 solid 24 23 27 - 50 78 D. Steady-State Photokinectics The quantum yields were measured by irradiation of degassed solutions of ketones (0.15 M) in tubes containing a fixed amount of internal standard parallel to valerophenone actinometer. For quenching studies, these tubes also contained varying amounts of 2,5- dimethyl-2,4-hexadiene as a quencher. Product yields at 5-18% were measured using GC or NMR and were converted to quantum yields. Stem-Volmer plots were linear with slopes equal to kq'c. The kinetic data are listed in Table 22. Triplet lifetimes, based on a 1(q value of 6x109 M'ls'l, are also listed.30 The errors represent deviations from the average. Table 22. Triplet Lifetimes and Product Quantum Yields of 2-(2'-(2',3'- Dimethyl)butyl)—benzophenone at Room Temperature (k= 313 nm) 501%!“ ME MI “T X 109 S" (DlSindlnl-Z 30:l >30:] 1:2.5 10:1 1:1 16:1 24 Methanol 2:1 - 5:1 1:] 12:1 - - 24 Crystal >30:l 100:0 - - 100:0 1 :1 - 24 Toluene 14.5:1 21:1 15:1 5:1 1.2:1 1.3:1 10:1 110 Toluene 11.5:1 16:1 10:1 10:1 111.5 1.5:] 4.5:1 92 4 ITI I rjII I I I I I I l—I I I I l I ITI lnk 15 #Jlljllllllllllljllllll 2.5 3 3.5 4 4.5 1000/1‘ 5 1( ), 2(9) . 3(A), 8(0) Graph 2. Arrhenius Plot 1 Table 24. Arrhenius Data from Graph 2 Ketone Az/AE AE,, Kcal/mole I Az/AE = 4.6 EE-EZ = 0.69 2 AZ/AE = 8.2 EE-Ez = 0.55 3 Az/AE = 2.0 EE-EZ = 1.2 8‘l AE/AZ = 7.0 I EE-EZ = 2.4 a) from the three lowest points Product ratios are influenced by the energies and hydrogen abstraction rates of reactive excited state conformers as well as interconversion and cyclization rates of 93 biradical rotamers. Energies of reactive triplet conformers mirror those of reactive ground state minima since the only significant change in geometry due to ma" excitation is a slight lengthening of the C-0 bond.107 The hydrogen abstraction rates are dependent on the orientation of the abstractable hydrogen relative to the nodal plane of the carbonyl group95 and are assumed to be similar for various conformers. These factors control the product ratios only when cyclization is faster than interconversion of biradical rotamers (ground state control). When biradicals interconvert faster than they cyclize, which is the case for most triplet biradicals due to their long lifetime, only energies and cyclization rates of various conformers influence product ratios (conformational control). Thus, in cases where the photocyclization is conformationally controlled, the product ratios can be calculated using Equation 4, me = (xz/XE).(chy./k%y.) Equation 4 where X2 and XE are the populations of the biradicals leading to Z and E indanols and kzcyc and kECyc are the rates of the cyclizations for different conformers. The populations of different rotamers are determined by the difference in their free energies which are presumed to be dominated by enthalpies. There are several known mechanisms for ISC of biradicalsg° In short biradicals, ISC is mainly driven by spin-orbit coupling, which is known to be very much dependent upon the distance and orientation of radical 76.97 ,98 .99 centers. The observed diastereoselectivities can, thus, be explained by the calculated energies, which reflect the conformational population, and cyclization rates which contain the intersystem crossing term. Semiempirical calculations have been 94 performed on the conformational distribution of the hydroxybiradical from 1. In these calculations, only the biradicals with the methyl at the S-radical site trans to the hemipinacol radical moiety were considered, since the syn isomer was found to lie 4 kcal/mole above the trans. There are only two minima within 5 kcal/mole of the global minimum (Brlz). Only one of these conformers (BrlE), which lies 0.5 kcal/mole above the global minimum, can cyclize directly. The other conformer (Brlx) requires a rotation around the ethylphenyl ring to achieve a cyclizable geometry. Brlx can form Brlz and Br”; by small rotations around bonds a and b, respectively. Analysis of the minimization map reveal that these interconversions have similar barriers such that Br,z (2.3 kcal/mole) and Br”; (3.1 kcal/mole) are formed in a 3:1 ratio from Brlx. This results in almost the same population ratio expected form a 0.5 kcal/mole energy difference. Thus, even though Brlx can not cyclize directly, it acts as a transitional geomtery from which either one of the two reactive (cyclizable) geometries can be formed. It was also observed that the rotamer with the hydroxyl group pointing toward the central benzene ring is more stable (about 1.0-2.0 kcal/mole) than the one with the hydroxy group pointing away. This 100.101 . and IS phenomenon represents hydrogen bonding of the OH to the benzene ring prevented by Lewis base solvents. The large solvent effects on the photobehavior of 1 strongly support such a stabilizing effect in the biradical. In Brm, the two singly occupied p orbitals are almost orthogonal but not pointed at each other as they are in Brlz. These different orbital orientations seemingly lead to less triplet-singlet mixing in Br“; and to less efficient intersystem crossing, which appears as a lower pre-exponential factor for cyclization (Scheme 41). 95 Scheme 41 If we assume that intersystem crossing is independent of cyclization and that at each minimum the system intersystem crosses to the singlet surface, then we must determine what happens to Brlx after it becomes a singlet. Since Brlx cannot cyclize directly, it must convert into either Brlz or BrlE. The calculated rotational barriers noted above suggest that Brlx can form Brlz 3-times more efficiently than it can BrIE. Boltzman population ratios of Brlz, Brlx and Br”; are 0.42, 0.42 and 0.16, respectively. If we assume that Brlz intersystem crosses faster than Brlx and Brlg, due to a better orbital orientation, the ratio of intersystem crossing rates at room temperature can be measured, as follows, from the product ratios. 15 =(0-42(kisc1/kisc2)+ 0.28)/(0.16+0.14) thus kiscl/kisc2= 10 Where km, and kisc2 are the intersystem crossing rates of Brlz and Brlx or BrlE, respectively. This ratio seems too high to arise simply from different orbital orientations. Thus, it is believed that Brlx converts into Brlz and Br”; prior to intersystem crossing. 96 The fact that 1 yields only Z-indanol in the crystal confirms that Brlz is the predominant initial biradical geometry and rotations around the hydroxyradical site are necessary for formation of E-indanol. Similar explanation can be offered for the photobehavior of 2 at various temperatures. The Arrhenius plot is linear which indicates that the biradical conformers are equilibrated at all temperatures. Semiempirical minimizations reveal the presence of two minima (2A and 2B) within 1.2 kcal/mole of each other. The global minimum 2A is in the pro-Z geometry while 2B is in the pro-E geometry. The calculated enthalpic difference between the two biradical rotamers is twice the measured value (Table 24). 2A 28. 1.2 kcal/mole less stable than 2A Figure 21. Lowest Energy Biradical Conformations of 2 It was thought that ground state control might be operative. Global minimizations of the ground state ketone show the presence of two minima (2C and 2D) within 0.6 kcal/mole of each other, with the global minimum 2C in the pro-Z geometry. However, 97 analysis of the lowest energy rotational path for the interconversion of the two biradical conformers did not reveal significant barriers (4-5 kcal/mole). Thus, biradical minima can interconvert and ground state control can not be operative. It is believed that reactivity is rotationally controlled, with the discrepancy between the calculated and measured values attributable to over estimation of calculated pro-E energy. The large difference in the A factors may be attributed to: 1) the pro-Z biradical cyclizing faster than the pro-E biradical and 2) a larger entropic loss for the pro-E relative to pro-Z biradical due to phenyl and methyl ending up cis to each other in the E-isomer. 2C 2D. 0.6 kcal/mole less stable than 2C Figure 22. Lowest Energy Ground State Conformations of 2 Arrhenius data for 3 indicate that the conformation leading to 32 should be 1.2 kcal/mole more stable than that one leading to 3E. Our minimizations, however, reveal the presence of 5 minima within 2 kcal/mole of each other. Three of these (3A, 3B and 3D) are in a pro-Z and the other two (3C and 3E) are in a pro-E geometry. The global minimum (3A) has the hydroxyradical end twisted away from the benzylic radical such that cyclization requires a rotation around tolyl-a-carbon bond. Conformations 3B, 3C 98 and 3D are respectively 0.1, 1.0 and 1.3 kcal/mole higher in energy than 3A. The highest energy conformer (3D) is 2.0 kcal/mole higher than 3A and will not contribute much to the overall yield of 3indE. Thus, the observed product ratios in case of 3 are the result of products stemming form three conformations. In all reactive conformers (3B, 3C, and 3D), the two singly occupied p orbitals are orthogonal and are pointing toward each other. Thus, the A factor ratio simply represents the ratio of number of conformers leading to Z and B (Table 24). It is worth noting that the measured 1.2 kcal/mole enthalpy difference reflects an 88:12 ratio of pro-Z: pro-E conformers at RT. This ratio is also achieved by the Boltzman population of the three calculated conformers [3B(76%), 3C(15%), 3D(9%)]. 3C. 1.0 kcal/mole less stable than 3A 3D. 1.3 kcal/mole less stable than 3A 3E. 2.0 kcal/mole less stable than 3A Figure 23. Lowest Energy Biradical Conformations of 3 The Arrhenius plot of 8 is curved. It was thought that the curvature could be associated with the dehydration of indanols at high temperatures, thus leading to erroneous product ratios. However, control experiments revealed that dehydrations do not occur during the timeline of irradiations. This curvature can, however, be explained by one of the following: 1) A curved Arrhenius plot means a change in the mechanism of the reaction. Thus the curvature can be attributed to a change in the factors that control the reactivity. The measured isomeric ratio at -72°C is much less than the expected value predicted by the line through the other three points. Therefore, it is reasonable to assume that a mechanism other than conformational control is operative. The stereoselectivity of 8 depends on geometric variations at the a-hydroxy radical site. Rotation of the mesityl ring is too slow 3°g"°2 If rotations around the a- to compete with biradical decay at low temperatures. carbon-hydroxyradical site are also slow (semiempirical calculations show a 6.0 kcal/mole barrier), then the biradical must react from the geometry in which it is formed and ground state control becomes operative. Semiempirical minimizations have revealed the presence of two reactive ground state minima; with the low energy minimtun in a pro- 100 Z and the high energy one in the pro-E geometry. The difference in energy of 2.1 kcal/mole, however, warrants a Z:E ratio of 250:1, much greater than the 25:1 observed ratio. The 10-fold contrast between calculated and measured ratios can, however, be attributed to the difference in partitioning of the resulting biradicals, with the pro-E biradical cyclizing 10-times more efficiently than the pro-Z. Indeed, the ratio of A factors shows that the pro-E biradical cyclizes 7-times more efficiently than the pro-Z biradical. 8A. Lowest Energy Geometry of 8 SE. 2.1 kcal/mole less stable than 8A Figure 24. Lowest Energy Ground State Conformations of 8 2) Global minimizations on the hydroxybiradical from 8 reveal the presence of 4 minima within 1.0 kcal/mole of each other. Three of these conformations (8C, 8D, 8E) are in a pro-Z geometry. Of these conformations, 8E has the hydroxyradical end twisted away from the benzylic radical such that cyclization requires 180° rotation around the mesityl- a-carbon bond. It was mentioned earlier that this rotation is too slow to compete with biradical decay at low temperatures, as seen from variable temperature NMR which shows coalescence of the ortho-methyl groups of 8 near 0°C. Thus, even though cyclization is possible from SE and 8G above 0°C, it can not happen at -72°C which 101 should lead to a lower than expected Z:E ratio at this temperature. This explanation, however, can be disregarded if one considers the rotational map that shows the interconversion of these conformers. Conversion of 8C, which is essentially the initial biradical geometry, to the other conformers suffers from relatively high barriers (6-9 ' kcal/mole). This means that at low temperatures biradical interconversion can not compete with cyclization which in turn means that ground state control is operative. SE. 0.7 kcal/mole less stable than 8C 8F. 0.8 kcal/mole less stable than 8C Figure 25. Lowest Energy Biradical Conformations of 8 102 32 30 _ ' E {l u g 23 _ ¢ ' . .I _ 'i - fi 25 _ .- -. '1' ".1 ‘1'. V . | I; ,|' .3 2 - '. '2‘ n _ I-l-l . ' .h . '1'. 22 - ' ' ' 8E '. /' " 8D 20 r 1 r r A -4 -2 0 2 4 6 8 Lowest Energy Rotational Path Photobehavior of 8 at higher temperatures is assumed to be conformationally controlled. The Arrhenius data indicate the pro-Z biradical to be 2.4 kcal/mole more stable than the pro-E. This gives a 2: E population ratio of 98:2. Our calculations, however, indicate a lower population ratio of 85:15 based on the energies of cyclizable minima 8C, 8D and BF. This discrepency may be attributed to competition between ground state and biradical controls at 0°C (since it is not clear at what point the plot starts to curve, one can not be sure of such competition). The difference in the A factors is attributed to a more efficient cyclization of the pro-E conformer. 103 3 I I I r TI I I I l I I I I I I I I I I I I I I N IIIIlIIII ;[> 1/ i Ink 0 3llllllllllllllllllllllll - 2.5 3 3.5 4 4.5 1000/T 5 4 (0). 5(A), 6(X) Graph 3. Arrhenius Plot 2 Table 25. Arrhenius Data from Graph 3 Ketone Az/AE AF.” Kcal/mole 4a All/A25 = 2325 Ezs'Ezz = 4.0 5 AEZ/AZE= 18.8 EEZ'EZE = 1.88 6 AZ/AE = 3.7 Ez-EE = 0.67 a) from the best-fit line The lack of stereoselectivity in photocyclization of 6 is similar to earlier results from the Wagner group.5°"°3 The two biradical geometries with phenyl tilted up or down 104 are very similar in energy but have different orbital orientations which leads to different cyclization rates (Scheme 42). Scheme 42. Lowest Energy Biradical Conformations of 6 Arrhenius data for 5 indicate the pro-ZE precursor to be enthalpically more stable than the pro-EZ one by 1.88 kcal/mole. Global minimizations on the biradical from 5 reveal the presence of 3 minima within 0.5 kcal/mole of each other. The global minimum(5A) is in a pro-EZ while the other two (SB and 5C) are in a pro-ZE geometries. The fact that the global minimum has a pro-EZ geometry contrasts with the Arrhenius data. Another interesting observation is that the Arrhenius plot of 5, unlike 8, is not curved. The curvature in the plot of 8 was rationalized in terms of either 1) ground state control or 2) lack of cyclization of several biradical conformations. Option 2 is not valid for 5 since the next closest minimum is 2.4 kcal/mole higher in energy than 5A and will not contribute much to the product ratios. This suggests that photobehavior of 5 is ground state controlled. The rotational energy map for interconversion of 5A to SB indicates an 105 11 kcal/mole barrier. This barrier is much too large for the interconversion of these biradical conformers to compete with cyclization. Thus, ground state control of reactivity must be operative. 5C. 0.5 kcal/mole less stable than 5A Figure 26. Lowest Energy Biradical Conformations of 5 Semiempirical minimizations on the ground state of 5 revealed two minima (5E and SF) within 1.8 kcal/mole of each other. If bond rotations are slow as expected and ground state control is operative, then these geometries should give the products in the correct ratios. Arrhenius data predict the two reactive geometries to be different in energy 106 by 1.88 kcal/mole (good agreement with calculated results) with the lower energy geometry resulting in the ZE-isomer. Indeed, the global ground state minimum is in the pro ZE-geometry. eelc_energy 7.08 to 18.98 keel .tnole 5A 53 Energy (kcalJ mole) Lowest Energy Rotational Path The difference in the A factors is attributed to the difference in rotational entropies of the two conformers. The pro-ZE conformer has a higher rotational. fieedom than the pro-EZ conformer since in the latter phenyl and methyl are cis (gauche) to each other. Thus, for the ground state control of reactivity, interconversion of the pro-EZ conformer to the pro-ZE one is entropically favored while the reverse is entropically disfavored. The fact that quantum efficiencies of formation for the ZE (0.14) and El 107 indanols (0.12) are similar indicates that the pro-EZ biradical is cyclizing more efficiently. 5E 5F. 1.8 kcal/mole less stable than 5E Figure 27. Lowest Energy Ground State Conformations of 5 The photobehavior of 4 is striking in that the ZE isomer, the minor indanol formed at room temperature, is the predominant product at low temperatures in hydrocarbon solvents and is the only product at low temperature in methanol. The Arrhenius plot of 4 ,similar to that of 8, is curved. Furthermore, the Arrhenius data obtained from the best fit line have unrealistic values of AB, and A for an equilibrated system. The data would indicate the pro-ZE biradical to be more stable than the pro-ZZ by 4.0 kcal/mole. Global minimizations on the biradical of 4, however, show the global minimum to have a pro-ZZ geometry, with the closest cyclizable pro-ZE biradical (4D) 1.5 kcal/mole higher in energy. 108 4C. 0.5 kcal/mole less stable than 4A 4D. 1.5 kcal/mole less stable than 4A Figure 28. Lowest Energy Biradical Conformations of 4 The curvature in the plot is believed to involve competition between bond rotation and cyclization in the hydroxybiradical at low temperatures. The lowest energy rotational map for interconversion of these biradical conformers shows 4-10 kcal/mole barriers. At low temperatures slow bond rotation in the biradical can not compete with cyclization, as in S and 8, and ground state control is operative. As temperature increases, the rotation 109 becomes faster and competes with cyclization. At or near room temperature, rotation becomes faster than cyclization and conformational control takes over. 30 23 ~ 25 _. i 24 ~ 5 E 20 L '5 18 P 16 l- _ m ,4 4n 3‘3 . 4B 0 5 1o 15 20 LowestEmgyRombmlPath The ZE:ZZ ratio of 9:1 at -72°C thus must be the result of the ground state control. Global minimizations on ground state of 4 reveal the presence of two minima within 1.0 kcal/mole of each other, with the lower energy one being in the pro-ZE geometry. It is thus believed thatithese two conformers are responsible for the observed 9:1 ZE:ZZ ratio at -72°C. 4E 4F. 1.0 kcal/mole less stable than 4E Figure 29. Lowest Energy Ground State Conformations of 4 110 The low quantum efficiency for cyclization (0.06) in 4 is attributed to a competing on- cleavage reaction and an efficient back transfer which occurs at geometries along the rotational path of interconversion of calculated minima. Finally, the absence of the EZ-isomer from photoproducts of 4 can be explained by considering that the lowest energy biradical conformer leading to El lies 2.2 kcal/mole above the global minimum and thus is scarcely populated. 4G. Pro-EZ biradical H. Photobehavior of a-Arylacetones - A Comparison of Singlet and Triplet Biradical Behavior The main goal of this project was to determine the similarities and differences in reactivity and selectivity of 1,5-singlet and triplet biradicals. From a mechanistic point of view, the difference in the reactivity of the singlet and triplet 1,5-biradicals and the role of environmental and conformational factors in determining the overall efficiency and chemical yield of indanol formation must be addressed. As mentioned earlier, the reactive excited states for aliphatic ketones are both singlet and triplet states. Thus, the excited states responsible for the two observed photoreactions in a-arylacetones, namely S-hydrogen abstraction and a-cleavage, have to 111 be determined. Turro has shown that in a-(o-tolyl)acetones S-hydrogen abstraction occurs only from the singlet while (rt-cleavage occurs only from the triplet.67 Our quenching studies corroborate Turro’s results. Table 26. Effect of Temperature on Product Ratios from a-Arylacetones Compound Indanol/Diarylethane Indanol/Diarylethane Indanol/Diarylethane -72 °C 24 °C 1 10°C 10 20:80 50:50 (3:1-Z:E) 60:40 (1.4:1 Z:E) 11 0:100 60:40 70:30 12 15:85 70:30 (10:1-Z:E) 85:15 13 0:100 70:30 100:0 Temperature effects on quantum yields are quite interesting. Diphenylethanes (DPEs) are the major and sometimes the only products at low temperature while indanol yields increase with increasing temperature. The high yield of DPEs, which result from (rt-cleavage followed by coupling of the resulting free radicals, demonstrates that there is an enthalpic barrier to hydrogen abstraction at low temperature whereas intersystem crossing has none. Thus, as temperature decreases, intersystem crossing to the triplet which only ot-cleaves becomes predominant. Indanol yield increases with increasing temperature. This may be due to two reasons: First, a higher population of excited singlets undergoing hydrogen abstraction because they have higher kinetic energy; and 112 second, a higher percent of the resulting singlet biradicals cyclizing rather than disproportionating. The latter would support Wagner’s suggestion that cyclization reactions have large barriers (due to loss of rotational freedom, ring strain and steric crowding around the forming bond) even on the singlet surface.87 The decrease in the quantum efficiencies of indanol formation in the trialkyl series from mesityl to the triisopropyl can be attributed to an increasingly more efficient disproportionation of the singlet biradical as the size of the alkyl group increases (which impedes cyclization due to increased strain during cyclization). Wagner er al. reported that a-mesitylacetophenone has a more rapid hydrogen abstraction but a lower indanol quantum yield than a-(o-tolyl)acetophenone, which they attributed to a charge-transfer quenching process competing with hydrogen abstraction in the former.87 An increase in indanol quantum yield in the acetone series from a-tolyl to a-(o-ethylphenyl) to a-mesitylacetone indicates the absence of any significant charge transfer quenching process from the singlet state. The effect of environment on the reactivity of acetones has also been addressed by Turro67 who reports a significant increase in indanol chemical yield in micellar solutions relative to homogeneous solutions. Our results show a 25% increase in indanol yield in micellar solutions. The conformational factors involved in hydrogen abstraction of or-arylacetones might be expected to be similar to those for a-arylacetophenones. However, a 2-6 fold decrease in diastereoselectivity was observed in acetones. 113 1.2 I I I I I I I I I I I r I I I I 1 I I l I I I lnk 0.2 11111111111111111111111 2.6 2.8 3 3.2 3.4 3.6 3.8 1000/T AE/AZ=5 EZ'EE= 1.6 kcal/mOle Graph 4. Arrhenius Plot of a-(o-Ethylphenyl)acetone The singlet biradicals have very short lifetimes and the ground state control might be assumed to control their reactivity. However, our results with a-(o-ethylphenyl) acetone seem to indicate conformational control of reactivity in photocyclization of singlet biradicals. Experimental results show the Z-indanol to be the major cyclization product under all conditions. Ground state global minimizations indicate the presence of two reactive geometries, a low energy in a pro-E and a pro-Z geometry 0.55 kcal/mole higher in energy (Scheme 43). Furthermore, semiempirical minimizations on the biradical of 10 show the presence of three minima within 1.8 kcal/mole of each other. The global minimum (10A) is not in a good geometry to cyclize, but the two higher energy 114 conformations can and are in a pro-Z (10B) and pro-E (10C) geometries, an can cyclize. 10C is higher in energy than 10B by 1.6 kcal/mole, in good agreement with the experimental values. The difference in A factors can be attributed to a faster cyclization rate of the pro-E precursor, due to its higher energy which in turn means a lower activation energy for cyclization. Therefore, the photocyclization of (X-(2- ethylphenyl)acetone is believed to be conformationally controlled which means that the singlet biradical lives long enough to allow equilibration. Furthermore, the difference in the A factors indicates that there needs to be an activation energy for cyclization. 10C. 1.6 kcal/mole less stable than 10A Figure 30. Lowest Energy Biradical Conformations of 10 115 Another explanation for the observed diastereoselectivity is that ground state control is operative but the pro-E biradical disproportionates 9 times more efficiently than the pro-Z biradical. This could be the case since the cyclization of the pro-E biradical suffers from larger steric/non-bonded interactions during the closure than the pro-Z. Pro-E PTO-Z Scheme 43. Reactive Ground State Conformations of 10 III. Photoenolizations of a-(2,4,6-Triisopropylphenyl)acetophenone and Acetone Formation of enol from compound 9 had already been documented.°°°’°°'87 Our reinvestigation of this reaction along with temperature and phase effects indicate that the enol is the only initial product formed under all conditions. Furthermore, our investigation into the photobehavior of a—(2,4,6-triisopropylphenyl)acetone (13) reveals that enol formation also occurs from the singlet states. We have demonstrated that in both cases enol photochemically and thermally reverts back to ketone. Thus the formation of enol and its reversion to ketone with hydrogen exchange between the benzylic and a— carbons demonstrates that disproportionation involving a 1,4-hydrogen transfer can compete with cyclization. The large preference for formation of enols from 9 and 13 might be blamed on the normal steric hindrance to cyclization of two tertiary radical sites. 116 However, since ot-(2,5-diisopropylphenyl)acetophenone cyclizes quite efficiently, the 36 37 . . . °‘ The semiempirical effect of the second o-isopropyl group warrants scrutiny. calculations strongly suggest that the other isopropyl group forces the biradical into a geometry in which one a-hydrogen is pointed directly at the other radical site, thus inviting disproportionation. Cyclization, on the other hand, requires bond rotation which may be impeded by the second isopropyl. The fact that enol is the only product at low temperature and from crystalline 9 demands that the indanol-forming biradical conformation be different from that initially formed. The minimized geometries of ketones 9 and 13 lead to the minimum energy biradical geometries, which favor disproportionation, as just noted. For this reason, the singlet and triplet biradicals behave very similarly. Figure 31. Lowest Energy Ground State and Biradical Conformers of 9 and 13 117 An explanation is required for the fact that the enol is a stable product at long wavelength irradiation but not at shorter wavelengths. A solution containing only enols, obtained by low temperature irradiation, showed strong UV absorption below 330 nm, with km, near 270 nm. Initially, the indanol is formed in low yield but the yield increases with conversion. This means that enol is converted photochemically to indanol, and is in agreement with the observed decrease in enol quantum yield with time for irradiations at wavelengths where the enol absorbs strongly. Our time dependent studies for irradiation of both ketone and enol show that indanol is not formed directly from enol but only from ketone, which must be regenerated continually from the enol. The mechanism of this disproportionation is unclear. Hart has proposed a simple 1,3-hydrogen shift, which seems reasonable even though the trimethylsilyl enol ether of 9 does not undergo the same 1,3-shift. For ketone 13, (at-cleavage is the only photoreaction at low temperature. This demonstrates that there is an enthalpic barrier to hydrogen abstraction, whereas intersystem crossing has none. Thus, as temperature decreases, the intersystem crossing to a triplet that undergoes only radical cleavage becomes predominant. The overall quantum efficiency is low for 13 because of the well known highly efficient radiationless decay that accompanies singlet state hydrogen transfers.11 The stability of solid 13 is attributed to the large ground state C=O---H distance (3.2 A). We have considered the possibility of similar enol formation for the other a-aryl acetones and acetophenones studied. In our investigations, however, we were unable to detect any, except maybe for a-(2,4,6—triethylphenyl)acetone where a vinyl peak was 118 observed in the NMR spectrum of the photolysis mixture but disappeared too quickly to allow careful analysis. The less hindered enols are expected to be much less stable with respect to ketone and if formed apparently are too short-lived to detect. IV. Photobehavior of o-tert-Butyltrifluoroacetophenone Wagner et al. reported a sharp contrast in the photobehavior of o-tert- 54.56 . . . Irradiation of benzophenones results in butylacetophenones and benzophenones. efficient formation of indanols while that of acetophenones results mainly in an unsaturated alcohol. Rotation of the 1,5-biradical produced by 6-hydrogen abstraction in o-tert—butylphenyl ketones is necessary for cyclization but destroys the benzylic conjugation. n—Conjugation is more important in excited states than in ground state.'°4 In the benzophenone derivatives, the benzylic radical center of the biradical can remain unconjugated with the unsubstituted phenyl ring while the butylphenyl ring rotates. The absence of the second phenyl ring in the acetophenone derivatives causes a retarded rotation. Thus, the difference in behavior was attributed to the retarded rotation of the benzylic center of the biradical which slows down the indanol formation and allows the biradical to undergo a less favorable reaction, namely rearrangement to an unsaturated alcohol. The authors cited two possibilities for the formation of the unsaturated alcohol, disproportionation of a rearranged 1,5-biradical or a 1,5-sigmatropic hydrogen shift in a . 54 sprroenol. 119 Scheme 44 The photobehavior of o-tert-butyltriflouroacetophenone was investigated to determine whether the capto-dative resonance of the benzylic radical center to the trifluromethyl group is sufficient to allow a free rotation of the benzylic center, leading to an indanol as a major product. OH +°OH \ CF3 Cl:2 / Scheme 45 Our results clearly indicate that capto-dative resonance is not sufficient to allow a free rotation of the benzylic radical center since the unsaturated alcohol comprised ~90% 120 of the products in all solvents. Our calculated barrier to rotation of the benzylic radical center of acetophenone and triflouroacetophenone totally out of conjugation is 8 kcal/mole. If the benzylic center has to rotate only 45° to get into a geometry suitable for cyclization the barrier drops to 4 kcal/mole. Clearly, capto-dative resonance does not provide 4 kcal/mole stabilization to speed up cyclization process, thus the less favorable rearrangement to unsaturated alcohol remains the predominant relaxation pathway. 90% Scheme 46 V. Photobehavior of 2-(2’-(2’,3’-Dimethylbutyl))benzophenone - Effect of Dihedral Angle on Hydrogen Abstraction Rates The primary purpose of this study was to gain insight into the orbital orientational requirements for hydrogen abstraction by triplet carbonyls. Global minimizations (AMI) with dihedral drivers around phenyl-tert-carbon bond have revealed the presence of two distinct minima on the energy surface of 15 . (Figure 32). The lowest energy minimum (15A) has the isopropyl group perpendicular to 121 the plane of the phenyl and occupying the same side of the plane as the carbonyl oxygen. In this geometry both isopropyl (HA, d= 2.3 A) and methyl hydrogens (H3, d= 2.5 A) are close enough for abstraction. In the other minimum (15B), which lies 1.0 kcal/mole above ISA, only methyl hydrogens (d=2.3 A) are close enough for abstraction. The global minimum 15A has a geometry similar to the X-ray structure of OTAMBP.57 15A. Lowest Energy Geometry of 15 15B. 1.0 kcal/mole less stable than 15A Figure 32 Our calculations have revealed that a methyl hydrogen is within abstraction 105 has distance of the carbonyl oxygen over a wide range of geometries. Scheffer established that distance is the principal determinant of reactivity,‘06 so the reaction can occur from a geometry other than the two minima. However, the very low activation energy for triplet decay in OTBBP5° rules out more than slight departures from conformational minima in reaching the transition state. Despite favorable distances, the methyl hydrogens have different dihedral angles with respect to the nodal plane of the carbonyl in the two minima. In 15A, the angle to is 96° while in 158 (o is 79°. If we 122 consider a Coszo) dependence on reactivity, as has been proposed by Wagner,48 methyl hydrogens in both conformations should be unreactive toward abstraction. Despite this, 15 forms indanol photoproducts that represent 50-90% hydrogen abstraction from a poorly positioned methyl group. Even in the crystalline state 50% of the products originate from methyl abstraction. It is conceivable that the flexibility of the tert-hexyl group might cause significant improvements in a) at the transition state relative to the reactant. It is also noteworthy that the reactant is the triplet, not the ground state on which the calculations have been performed. This, however, shouldn’t alter our treatment since the only significant change in geometry due to n,rt* excitation is slight lengthening of the C-0 bond. ‘07 Biradical Partitioning. The quantitative treatment of our results involves converting product ratios into relative rate constants for hydrogen abstraction. Scheme 47 depicts the competition that produces the observed product ratios. The product ratios are determined by the ratios of hydrogen abstraction rates times the partitioning of biradical between coupling and reversion back to ketone. An extra feature of the photobehavior of 15 is the formation of 15alc. To our knowledge, such intermediates (spiro-intermediate) and photoproducts have been observed for o-alkoxy and o-tert-butylacetophenones but not benzophenones.54 Formation of the unsaturated alcohol from a spiro intermediate in 2,4- di-tert-butylacetophenone has quantum efficiencies of 0.02—0.05 in benzene and methanol.54 Thus, the biradical and the spiro intermediate revert back to starting ketone with a combined 95-98% efficiency. 123 O h hv v \ ————> Ph C D D 6 6 C6 6 l / rs H30 C2; H30 9H3 H30 CH3 ._.\\ 3 ....t\\\\ C H3 l \ C H3 / . + ., CH3 How"Ph Ho"Ph ”0 Ph \ 15alc lSindmZ 15:..de k lSindip , Y 1" Radical Products 3° Radical Products Scheme 47 If one considers that the biradical from OTBBP forms the indanol product with a quantum efficiency of 1 and that both biradicals from OTBBP and 2,4-di-tert- butylacetophenone are solvated to the same extent, we can conclude that all of the 95% disproportionation back to ketone in methanol arises from the spiro intermediate. However, such values are not available for benzophenone derivatives and the mechanism of reversion of the spiro-intermediate back to ketone (radical or ionic) is unknown. Thus, for simplicity, two boundary conditions have been considered: a) The spiro-intermediate which leads to formation of 15alc has a quantum efficiency of 1 for product formation, so that all partitioning is presumed to occur in the biradical. Thus product ratios can be determined using Equation 5. l/3=(15indmZ + 15inde + 15alc ) / lSindip = (kmeH / kip") (PB,,/ Pm) Equation 5 124 One must understand how the PB,,/ Pm ratio can vary in order to correctly deduce km,“ / kip” ratios from product ratios. There is a large solvent effect on product ratios and quantum efficiencies. Table 27. Effect of temperature and Medium on Product Ratios of 15 Reaction T (° C) 15indmZ lSinde 15alc 15indip media Benzene 24 27 52 7 1 5 Methanol 24 32 32 l 3 23 Toluene 1 10 22 29 8 41 Toluene -72 33 48 5 15 solid 24 23 27 - 50 This solvent effect shows that the two biradicals cyclize with different efficiencies. In benzene, all biradicals from OTBBP, OTAMBP and 15 disproportionate to starting ketone with high efficiency. In methanol, all of the biradicals from OTBBP cyclize but not quite half of those from OTAMBP and 15 cyclize. The P3, value for the biradical from OTBBP is 0.04 in benzene but rises to unity in methanol, where hydrogen bonding to solvent suppresses biradical disproportionation back to the ground state ketone. Similarly, the PB, value for a solvated biradical is unity in OTAMBP, while those for unsolvated biradicals are 0.05 and 0.028 for a primary (methyl) and secondary (ethyl) radicals, respectively. The low quantum yields for 15 and the methanol induced increase 125 in the yield of lSindip suggest that P3,, cyclizes less efficiently than does PB”. The fact that Pm is more sterically crowded than P3,, will lead to a lower rate of cyclization in unsolvated biradicals. This point will be emphasized when the temperature effects on product ratios are considered. Since methanol increases the total quantum yield of 15 only to 42%, its biradicals, similar to those of OTAMBP, hydrogen bond to solvent less efficiently than the less sterically crowded biradical of OTBBP. Because methanol traps only 42% of biradicals, we rely on an estimate of Br3/Br. for the 58% that still revert to starting ketone. We have assumed two boundary conditions, described below, in order to calculate the ratios of hydrogen abstraction rates. One option is to assume that all primary biradicals cyclize with 100% efficiency in methanol as is the case for the biradical from OTBBP. In this case, Br3/Brl is 2.2 and Pad/P3,, becomes 6 and 19 in methanol and benzene, respectively. Therefore, kHip/kac is calculated to be 2.24 methanol and benzene. However, this treatment would demand an unlikely P3,, value of 0.27 in benzene, seven times higher than that of OTBBP (PB,= 0.04 in benzene). (Dubmmfi 0.0835 (Dumflmolfi 0.309 (Dnmmefi 0.01 (Dzmctmol): 0.107 Br,/Br,= 69/31= 2.2 In Methanol: Pan/Parf 1/0.155= 6.45 kmp/kflm= 2.24 In Benzene: PBrl/P8r3= 0.27/0.015= 18.75 kHip/kflm= 2.24 Scheme 48 126 Another option is to assume that the ka/kae is the same as the product ratios. Partial suppression of disproportionation is common in bulky hydroxybiradicals and is thought to reflect an equilibrium between hydrogen-bonded and free biradicals, with none of the former disproportionating. Since Br, and Br3 share a common conformational preference, the equilibrium constant for solvation should be similar for both biradicals and the Br3/Br1 ratio should approximate kHip/kac. In this situation, P3,, and PM, become 0.108 and 0.05 respectively for the unsolvated biradicals. It is important to note that ~95% of the reaction in methanol arises from the solvated biradicals. (Dubenzene): 0°0835 (blflnetllanol): 0309 ¢2(benzene)= 0'01 (Dzuncthanol): 0°107 kaJkHip=77/23 In Methanol: ¢ll¢3=(77/23){0.34+0.67(0.108)/0.34+0.66(0.05)}= 0.309/0.107 In Benzene: (I),/_m81 Mg >;—7 Figure 34. 1H NMR of a-(Z-Ethylphenyl)acetophenone Before and After Irradiation in Toluene (A > 290 nm) 172 Products from a—(2,4,6-Triethylphenyl)acetophenone a-(2,4,6-Triethylphenyl)acetophenone (0.002 g) in 0.8 mL of deuterated benzene was irradiated until starting material could not be observed by NMR. The signals corresponding to two isomeric indanols were detected in the NMR spectrum of the mixture. The effect of temperature on product ratios was investigated by conducting the photochemiStry in acetone/ethanol, ice-water and silicon oil (110°C) baths. Solid state irradiation was performed by packing a melting point capillary with the compound and irradiating it through Pyrex-filtered uv light for three hours. The diasteriomeric ratio of the products was determined by NMR integration of the methyl doublet peaks corresponding to each isomer. Large scale irradiation using 0.35 g of a—(2,4,6- triethylphenyl)acet0phenone in 150 mL of toluene was performed until 100% conversion (GC). Solvent was removed to leave a yellow oil which was separated by PTLC using 5% ethyl acetate in hexane to separate the two isomers. The Z-isomer was eluted before the E-isomer. The proucts were recovered as oils. \\.. Ph \ hv / O Toluene 2 ZindE 2indZ Scheme 62. Photoproducts of a-(2,4,6-TriethylphenyI)acetophenone 173 Z-l-methyl-4,6-diethyl-Z-Qhenyl-Z-indanol IH NMR(CDC13): 5 1.25 (t, J=7.5 Hz, 3H, CH3CH2), 1.25 (d, J=7.5 Hz, 3H, CH3CH), 1.32 (3H, t, J: 7.5 Hz, 3H, CH3CH2), 2.1 (s, 1H, 0H), 2.6 (q, J=7.5 Hz, 2H. CHZCH3). 2.7 (q, J=7.5 Hz, 2H, CHzCH3), 3.2, 3.43 (AB quartet, J= 18 Hz, 2H, CH2), 3.6 (q, J=7.5 Hz, 1H, CHCH3), 6.95 (s, 1H, Ar), 6.98 (s, 1H, Ar), 7.3 (1H, t, J=6.7 Hz, 1H, Ar), 7.45 (2H, dd, J= 6.7, 7.0 Hz, 2H, Ar), 7.68 (d, J= 7.0 Hz, 2H, Ar) lH NMR(Toluene-d8): 5 1.12 (d, J=6.9 Hz, 3H, CH3), 1.15 (t, J=7.8 Hz, 3H, CH3), 1.23 (t, J=7.8 Hz, 3H, CH3), 1.4 (s, 1H, 0H), 2.45 (q, J=7.8 Hz, 2H, CH2), 2.59 (q, J=7.8 Hz, 2H, CH2), 2.88, 3.13 (AB quartet, J=16.2 Hz, 2H, CHZCOH), 3.30 (q, J=7.8 Hz, 1H, CHCH3), 6.84 (s, 1H, Ar), 6.87 (s, 1H, Ar), 7.11 (t, J= 6.6 Hz, 1H, Ar), 7.21 (dd, J=6.6, 7.2 Hz, 2H, Ar), 7.5 (d, J=7.2 Hz, 2H, Ar) l3C NMR(CDC13): 5 10.08, 14.21, 15.64, 26.01, 28.62, 47.16, 50.08, 84.88, 120.34, 125.01, 125.70,126.48, 127.76, 135.05,139.81, 143.36,144.04,144.79 IR(CC14): 3592, 2966.9, 2934.1, 2874.2, 1240.4, 1174.8, 991.54, 935.59, 871.94, 700.25 E-l-methyl-4,6—diethyl-2-phenyl-Z-indanol ‘H NMR(CDC13): 5 0.79 (d, J=7.2 Hz, 3H, CH3CH), 1.20 (t, J=7.5 Hz, 3H, CH3CH2), 1.25 (t, J=7.5 Hz, 3H, CH3CH2), 2.0 (broad s, 1H, CH), 2.62 (q, J=7.5 Hz, 2H, CHZCH3), 2.63 (q, J=7.5 Hz, 2H, CHZCH3), 3.12, 3.65 (AB quartet, J=18 Hz, 2H, CH2), 3.39 (q, J= 7.2 Hz, 1H, CHCH3), 6.90 (s, 1H, Ar), 6.92 (s, 1H, Ar), 7.25-7.5 (m, 5H, Ar) lH NMR(Toluene-d3): 5 0.78 (d, J=6.9 Hz, 3H, CH3CH), 1.15 (t, J=7.5 Hz, 3H, CH3CH2), 1.23 (t, J=7.5 Hz, 3H, CH3CH2)s 1.4 (broad s, 1H, OH), 2.44 (q, J=7.5 Hz, 2H, 174 CHZCH3), 2.59 (q, J=7.5 Hz, 2H, CHZCH3), peaks between 3.0-7.5 overlapped with those from the major isomer. l3C NMR(CDC1,): 5 14.52, 15.82, 17.84, 26.48, 28.87, 42.53, 52.55, 85.98, 121.30, 125.35, 125.89, 126.17, 127.26, 128.09,135.18, 140.02, 143.30, 146.80 IR(CCI4): 3472, 2968.8, 2930.24, 2872.37, 1277, 1211.4, 1066.8, 881.58, 746.55, 700.25 Products from a-(o- Tolprropiophenone (3) a—(o-Tolyl)propiophenone (0.002 g) in 0.8 mL of deuterated benzene was irradiated until starting material could not be observed by NMR. The signals corresponding to several products were detected in the NMR spectrum of the mixture. These products were identified as two isomeric 2-phenyl-2-indanols, two isomeric diarylethanes, B-tolylpropiophenone and benzaldehyde. The effect of temperature on product ratios was investigated by conducting photochemistry in dry ice-ethanol, ice- water and silicon oil (110°C) baths. The diasteriomeric ratio of indanols was determined by NMR integration of the methyl doublet signals corresponding to each isomer. Large scale irradiation using 0.3 g of a-(o-tolyl)propiophenone in 150 mL of methanol was performed until 100% conversion by NMR. The products were separated by PTLC using 5% ethyl acetate in hexane as eluent and characterized. Two additional products which were identified as two isomeric 1-phenyl-2-tolyl-1-propanols were also recovered. The order of elution was as follows: diarylethenes followed by B-tolylpropiophenone, the Z- indanol, the E-indanol and photoreduction products. The products were recovered as oils. 175 W Haw-r w—a 1.8. I.“ 1.48 7.16 4.1. 0 31 Figure 35. 1H NMR Spectra of a-(2,4,6-Triethylphenyl)acetophenone Before and After Irradiation in Toluene (D290 nm) 3cleav-Two isomers 3red-Two isomers Scheme 63. Photoproducts of a-Tolylpropiophenone Z-l-meth 1-2- hen l-2-indanol lH NMR(CDC13): 5 1.16 (d, J=7.0 Hz, 3H, CH3), 3.05, 3.40 (AB quartet, J=16.3 Hz, 2H, CH2), 3.48 (q, J=7.0 Hz, 1H, CH), 7.15-7.3 (m, 5H, Ar), 7.36 (t, J=7.0 Hz, 2H, Ar), 7.60 (d, J=7.0 Hz, 2H, Ar) l3C NMR(CDCl3): 5 10.3, 49.3, 50.4, 85.4, 121.7, 124.8, 125.4, 126.9, 127.0, 127.1, 128.2, 140.0, 144.1, 145.0 IR(CC14): 3600, 1175, 1043 E-l-methyl-2-phenyl-2-indanol IH NMR(CDCl3): 5 0.73 (d, J=7.0 Hz, 3H, CH3), 3.10,3.70 (2H, AB quartet, J=16.0 Hz, 2H, CH2), 3.23 (q, J=7.0 Hz, 1H, CH), 7.21 (m, 4H, Ar), 7.29 (m, 1H, Ar), 7.34 (t, J=6.6 Hz, 2H, Ar), 7.45 (d, J=6.56 Hz, 2H, Ar) l3C NMR(CDC13): 5 17.6, 44.6, 52.4, 86.1, 124.3, 124.9, 126.2, 126.9, 127.0, 127.3, 128.1,140.1,140.2,146.7 177 IR(CC14): 3605, 1165, 1050 (33) and (S,S)-1-Phenyl-2-tolyl-l-propanol lH NMR(CDC13): 5 0.95 (d, J=7.0 Hz, 3H, CH3CH), 2.15 (s, 3H, CH3Ar), 3.25 (dq, J=7.0, 6.7 HZ, 1H, CHCH3 ), 4.47 (d, J=6.7 Hz, 1H, CHOH), 7.0-7.3 (m, 9H, Ar) (3,8) and 1S,R)-l-Phenyl-2-tolyl-l-propanol IH NMR(CDC13): 5 1.30 (d, J=7.0 Hz, 3H, CH3C1-1), 1.92 (s, 3H, CH3Ar), 3.25 (dq, J=7.0, 6.7 Hz, 1H, CHCH3), 4.47 (d, J: 6.7 Hz, 1H, CHOH), 7.0-7.3 (m, 9H, Ar) 1,2-Ditolylbutanes lH NMR(CDC13): 5 1.0 (d, J=7.0 Hz, 6H,2CH3C1~I), 1.20 (d, J: 7.0 Hz, 6H, 2CH3CH), 2.0 (s, 6H, 2CH3Ar), 2.2 (s, 6H, 2CH3Ar), 3.15 (m, 4H, CHCH3), 6.8-7.3 (m, 16H, Ar) Products from a—(2-Ethylphenyl)-,6,,6,,6—trideuteropropiophenone and/or a-(2- Ethylphenybpropiophenone (4, 4d 3) a—(2—Ethylphenyl)-B,[3,B-tfideuteropropiophenone (0.003 g) in 0.8 mL of deuterated benzene was irradiated until no trace of starting material could be observed by NMR. A mixture of several products including two isomeric indanols, two isomeric diphenylethanes, and benzaldehyde were detected, by their signals, upon analysis of the NMR spectrum of the photolysis mixture. The effect of temperature and phase on product ratios was also investigated by conducting the photochemistry in acetone/ethanol, ice- water and silicon oil (110°C) baths and in solid. The diasteriomeric ratio of indanols was 178 determined by NMR integration of the methyl doublet signals corresponding to each isomer. Large scale irradiation using 0.25 g of a—(2-ethylphenyl)-B,B,B—trideutero propiophenone in 100 mL of benzene was performed. Solvent was evaporated to leave a colorless oil which was chromatographed by preparative scale tlc using 3% ethyl acetate in hexane solution. The order of elution was as follows: diarylethenes, the Z-indanol, the E-indanol and photoreduction products. The indanols and photoreduction products were recovered as oils. 4cleav-Two isomers 4red-Two isomers Scheme 64. Photoproducts of a-(Z-Ethylphenyl)—B,B,B-trideuteropropiophenone Z-l-Meth l-Z-3-trideuterometh 1-2- hen l-2-indanol lH NMR(CDC13): 5 1.19 (d, J=7.0 Hz, 3H, CH3CH), 1.52 (broad s, 1H, 0H), 3.50 (s, 1H, CHCD3), 3.50 (q, J=7.0 Hz, 1H, CHCH3), 7.18 (dd, 1:0.7, 4.5 Hz, 1H, Ar), 7.20 (broad, 1H, Ar), 7.25-7.27 (m, 2H, Ar), 7.29 (t, J=7.7 Hz, 1H, Ar), 7.38 (dd, J=7.7, 7.1 Hz, 2H, Ar), 7.60 (d, J=7.1 Hz, 2H, Ar) 179 'H NMR(Toluene-d8): 5 0.92 (d, J=7.2Hz, 3H, CH3CH), 3.12 (s, 1H, CHCD3), 3.12 (q, J=7.2 Hz, 1H, CHCH3), 7.0-7.6 (m, 9H, Ar) 2H NMR(CC14): 5 1.29 (s, 3D) l3C NMR(CDC13): 5 9.90, 9.91 (septet), 50.05, 88.23, 123.35, 125.7, 126.9, 127.16. 128.1, 144.3 IR(CC14): 3588, 2966, 2932, 2224, 1489, 1176.7, 1055, 985.8, 951, 912.4, 871.9, 746.5 (Z,Z)-lé-Dimethyl-2-phenyl-2-indanol lH NMR(CDC13): 5 1.19 (d, J=7.0 Hz, 6H, 2CH3CH), 1.52 (broad s, 1H, OH), 3.50 (q, J=7.0 Hz, 2H, 2CHCH3), 7.18 (dd, J=0.7, 4.5 Hz, 1H, Ar), 7.20 (broad, 1H, Ar), 7.25- 7.27 (m, 2H, Ar), 7.29 (t, J=7.7 Hz, 1H, Ar), 7.38 (dd, J=7.7, 7.1 Hz, 2H, Ar), 7.60 (d, J=7.1 Hz, 2H, Ar) 111 NMR(Toluene-d8): 5 0.92 (d, J=7.2Hz, 6H, 2CH3CH), 3.12 (q, J=7.2 Hz, 2H, 2CHCH3), 7.0-7.6 (m, 9H, Ar) l3C NMR(CDC13): 5 9.90, 9.91, 50.05, 88.23, 123.35, 125.7, 126.9, 127.16, 128.1, 144.3 IR(CC14): 3588, 2966, 2932, 1489, 1176.7, 1055, 985.8, 951, 912.4, 871.9, 746.5, 700.25 E-l-methyl-Z-3-trideuteromethyl-Z-phenyl-Z-indanol lH NMR(CDC13): 5 0.74 (d, J=7.35 Hz, 3H, CH3CH), 1.65 (broad s, 1H, OH), 3.28 (q, 1:740 Hz, 1H, CHCH3), 3.90 (s, 1H, CHCD3), 7.20-7.28 (m, 4H, Ar), 7.32 (t, J=7.2 Hz, 1H, Ar), 7.37 (dd, J=7.35, 7.2 Hz, 2H, Ar), 7.52 (d, J=7.35 Hz, 2H, Ar) 180 1H NMR(Toluene-d8): 5 0.55 (d, J=7.5Hz, 3H, CH3CH), 2.95 (q, J=7.5 Hz, 1H, CHCH3), 3.43 (s, 1H, CHCD3), 7.0-7.6 (m, 9H, Ar) 2H NMR(CC1,): 5 1.4 (s, 3D) ”C NMR(CDC13): 5 11.1 (septet), 18.3, 43.3, 52.5, 79.9, 123.9, 124.4, 126.0, 126.58, 127.1, 127.3, 127.9, 1282,1283, 128.7 IR(CC14): 3470, 2966.9, 2932.2, 2874, 2229.9, 1223, 1062, 970, 870, 740.7 1LLZHé-Dimethyl-Z-phenyI-2-indanol lH NMR(CDC13): 5 0.74 (d, J=7.4 Hz, 3H, CH3CH), 1.34 (d, J=7.3 Hz, 3H, CH3CH), 1.65 (broad s, 1H, OH), 3.28 (q, J=7.40 Hz, 1H, CHCH3), 3.90 (q, J=7.3 Hz, 1H, CHCH3), 7.20-7.28 (m, 4H, Ar), 7.32 (t, J=7.2 Hz, 1H, Ar), 7.37 (dd, J=7.35, 7.2 Hz, 2H, Ar), 7.52 (d, J=7.35 Hz, 2H, Ar) lH NMR(Toluene-d8): 5 0.55 (d, J=7.5Hz, 3H, CH3CH), 1.1 (d, J=7.4 Hz, 3H, CH3CH), 2.95 (q, J=7.5 Hz, 1H, CHCH3), 3.43 (q, .1: 7.4 Hz, 1H, CHCH3), 7.0-7.6 (m, 9H, Ar) l3C NMR(CDC13): 5 11.1, 18.3, 43.3, 52.5, 79.9, 123.9, 124.4, 126.0, 126.58, 127.1, 127.3, 127.9, 128.2, 128.3, 128.7 IR(CC14): 3470, 2966.9, 2932.2, 2874, 1223, 1062, 970, 870, 740.7 (M) and (S,S)—2,§-di(ethylphenyl)butane lH NMR(CDC13): 5 1.09 (t, J=7.48 Hz, 3H, CH3CH2), 1.27 (3H, t, 1:754 Hz, 3H, CH3CH2), 2.36 (dq, J=7.42, 14.56 Hz, 1H, CHZCH3), 2.60 (dq, J=7.47, 14.56 Hz, 1H, CHZCH3), 2.72 (1H, dq, J=7.49, 14.49 Hz, 1H, CHZCH3), 2.84 (dq, J=7.41, 14.56 Hz, 1H, 181 CHZCH3), 3.20 (s, 1H, CHCD3), 3.26 (s, 1H, CHCD3), 6.96 (1H, dt, J=2.l9, 7.7 Hz, 1H, Ar), 6.98 (dt, J=1.38, 7.5 Hz, 1H, Ar), 7.05 (dt, J=2.19, 7.7 Hz, 1H, Ar), 7.15 (dt, J=l.37, 7.7 Hz, 1H, Ar), 7.19 (dt, J=2.14, 7.7 Hz, 1H, Ar), 7.23 (broad d, J=7.7 Hz, 1H, Ar), 7.25 (dt, J=1.98, 7.5 Hz, 1H, Ar), 7.34 (broad d, J=7.41 Hz, 1H, Ar) l3C NMR(CDCl3): 5 15.5, 15.89, 20.84, 21.33, 25.54, 26.33, 39.84, 40.34, 125.45, 125.7, 125.8, 126.27, 126.51, 128.15, 128.68, 140.5, 141.99, 144.46, 144.51 (LLS) and (S,R EZQ-dilethylphenylwutane lH NMR(CDC13): 5 1.05 (t, J=7.60 Hz, 6H, 2 CH3CH2), 2.34 (dq, J=7.63, 14.35 Hz, 2H, CHZCH3), 2.58 (dq, J=7.69, 14.56 Hz, 2H, CHZCH3), 3.25 (broad s, 2H, 2CHCD3). 6.94 (dt, 1:2.19, 7.5 Hz, 2H, Ar), 6.96 (dt, 1:1.35, 7.5 Hz, 2H, Ar), 7.03 (dt, J=2.19, 7.5 Hz, 2H, Ar), 7.21 (broad d, J=7.42 Hz, 2H, Ar) l3C NMR(CDC13): 5 15.5, 20.84, 25.54, 39.83, 125.43, 126.50, 128.15 l-Phen 1-2- 2’-eth l hen 1 3 -trideutero-1- ro anol one isomer lH NMR(CDC13): 5 1.10 (t, J= 7.6 Hz, 3H, CH3CH2), 2.5 (AB quartet of q, J=7.6 Hz, 1:15 Hz, 2H, CH2CH3), 3.35 (d, 1H, CHCD3), 4.8 (d, 2H, CHOH), 7.1—7.5 (m, 9H, Ar) l-Phen 1-2- 2’-eth l hen l -trideutero-1- ro anol second isomer lH NMR(CDC13): 5 1.25 (t, J: 7.6 Hz, 3H, CH3CH2), 2.7 (AB quartet of q, J=7.6, 15 Hz, 2H, CHZCH3), 3.35 (d, 1H, CHCD3), 4.7 (d, 2H, CHOH), 7.1-7.5 (m, 9H, Ar) 182 CH3 CH3 P“ hv OH " OH O ' 4., + ’a. +Typel P" A CH3 01-13 A B 1 Figure 36. 1H NMR Spectra of ar(2-Ethylphenyl)propiophenone Before and After Irradiation in Toluene (D290 nm) 183 Products from a—(2,4,6-Triethylphenyl)-fl,,6,,6—trideuteropropiophenone and/or a- (2,4,6-Triethylphenybpropiophenone (5, 5d3) 01—(2,4,6-Triethylphenyl)-[3,0,B-trideuteropropiophenone (0.005 g) in 0.8 mL of deuterated benzene was irradiated until no trace of starting material could be observed by NMR. The signals for two isomeric indanols were detected upon analysis of the NMR spectrum of the photolysis mixture. In our investigation we separated the products from both the deuterated and fully protanated species. The effect of temperature and phase on product ratios was also investigated by conducting the photochemistry in acetone/ethanol, ice-water and silicon oil (110°C) baths and in solid. The diasteriomeric ratio of indanols was determined by NMR integration of methyl doublet signals corresponding to each isomer. In order to separate the two indanols, large scale irradiation using 0.30 g of or- (2,4,6-'triethylphenyl)-B,[3,B—trideuteropropiophenone in 100 mL of benzene was performed. Solvent was evaporated to leave a yellow oil which was chromatographed by PTLC 7% ethyl acetate in hexane solution. The plate had to be diluted several times to separate the two isomers (oils). The ZE-isomer was the top fraction eluted. Ph hv fl 0 Toluene 5 SindZE 5indEZ Scheme 65. Photoproducts of a-(2,4,6-Triethylphenyl)B,B,[3-trideutero propiophenone 184 4 6-Dieth l-Z-l-trideuterometh I-E-3-meth l-2- hen l-2-indanol 'H NMR(CDCl3): 5 0.86 (d, J=7.14 Hz, 3H, CH3CH), 1.24 (t, J=7.8 Hz, 3H, CH3CH2), 1.29 (t, J=7.8 Hz, 3H, CH3CH2), 2.0 (broad s, 1H, OH), 2.6 (q, J=7.8 Hz, 2H, CHZCH3), 2.7 (dq, J=7.8, 14.5 Hz, 2H, CHZCH3), 3.45 (q, J=7.1 Hz, 1H, CHCH3), 3.6 (broad s, 1H. CHCD3), 6.74 (s, 1H, Ar), 6.90 (s, 1H, Ar), 7.15-7.3 (m, 5H, Ar) lH NMR(Toluene-d8): 5 0.92 (d, J=7.2 Hz, 3H, CH3CH), 1.16-1.3 (m, 6H), 2.0 (broad s, 1H, OH), 2.5 (dq, J=7.2, 14.4 Hz, 2H, CHZCH3), 2.6 (q, J=7.5Hz, 2H, CH2CH3), 3.20 (q, J=7.1 Hz, 1H, CHCH3), 3.34 (broad s, 1H, CHCD3), 6.8-7.3 (m, 7H, Ar) 2H NMR(CC14): 5 1.48 (s, 3D) l3C NMR(CDC13): 5 13.62, 14.4 (septet), 14.77, 15.22, 24.84, 28.42, 46.29, 48.80, 86.20, 120.22, 125.42, 126.05, 126.42, 127.38, 138.45, 140.95, 142.90, 144.10, 144.44 IR(CC14): 3470.2, 3061.4, 2966.9, 2932.2, 2874.3, 2230, 1280.9, 1062.9, 970.3, 870, 806.4, 740.7 4.6-Dietl_1yl-Z.Eiidimethvl—Z-phenyl-Z-indanol lH NMR(CDC13): 5 0.86 (d, J=7.14 Hz, 3H, CH3CH), 1.24 (t, J=7.8 Hz, 3H, CH3CH2), 1.29 (t, J=7.8 Hz, 3H, CH3CH2), 1.47 (d, J=7.2 Hz, 3H, CH3CH), 2.0 (broad s, 1H, OH), 2.6 (q, J=7.8 Hz, 2H. CH,CH,), 2.7 (dq, J=7.8, 14.5 Hz, 2H, CHZCH3), 3.45 (q, J=7.1 Hz, 1H, CHCH3), 3.6 (q, J=7.2, 1H, CHCH3), 6.74 (s, 1H, Ar), 6.90 (s, 1H, Ar), 7.15—7.3 (m, 5H, Ar) 185 lH NMR(Toluene-d8): 5 0.92 (d, J=7.2 Hz, 3H, CH3CH), 1.16-1.3 (m, 9H), 2.0 (broad s, 1H, OH), 2.5 (dq, J=7.2, 14.4 Hz, 2H, CHZCH3), 2.6 (q, J=7.5Hz, 2H, CHZCH3), 3.20 (q. J=7.1 Hz, 1H, CHCH3), 3.34 (q, J=7.2 Hz, 1H, CHCH3), 6.8-7.3 (m, 7H, Ar) l3C NMR(CDC13): 5 13.62, 14.4, 14.77, 15.22, 24.84, 28.42, 46.29, 48.80, 86.20, 120.22, 125.42, 126.05, 126.42, 127.38, 138.45, 140.95, 142.90, 144.10, 144.44 IR(CC14): 3470.2, 3061.4, 2966.9, 2932.2, 2874.3, 1280.9, 1062.9, 970.3, 870, 806.4, 740.7 4 6-Dieth l-E-l-trideuterometh I-Z-3-meth 1—2- hen l-2-indanol lH NMR(CDC13): 5 1.291 (t, J=7.56 Hz, 3H, CH3CH2), 1.294 (t, J=7.56 Hz, 3H, CH3CH2), 1.36 (d, J=7.0 Hz, 3H, CH3CH), 2.0 (broad s, 1H, 0H). 2.6 (dq, J=7.56, 14.3 Hz, 2H, CH2CH3), 2.7 (q, J=7.8 Hz, 2H, CHZCH3), 3.30 (broad s, 1H, CHCD3) , 3.95 (q, J=7.0 Hz, 1H, CHCH3),6.92 (s, 2H, Ar), 7.30 (t, J=7.3 Hz, 1H, Ar), 7.40 (2H, dd, J=7.3, 7.5 Hz, 2H, Ar), 7.6 (d, J=7.5 Hz, 2H, Ar) lH NMR(Toluene-d8): 5 1.32 (d, J=7.2 Hz, 3H, CH3CH), 1.16-1.3 (m, 6H), 2.0 (broad s, 1H, OH), 2.52 (dq, J=7.2, 14.4 Hz, 2H, CH2CH3), 2.61 (q, J=7.5Hz, 2H, CHZCH3), 3.32 (broad s, 1H, CHCD3), 3.71 (q, J=7.1 Hz, 1H, CHCH3), 6.8-7.3 (m, 7H, Ar) 2H NMR(CC1,): 5 0.816 (s, 3D) l3C NMR(CDC13): 5 10.58, 15.28, 15.72, 17.20 (septet), 24.95, 28.95, 42.20, 50.65, 87.92, 121.04, 126.08, 126.70, 127.26, 128.24, 139.92, 141.20, 141.73, 143.42, 143.84 IR(CC14): 3572, 3061.4, 3030.6, 2966.9, 2932.2, 2230, 1282.8, 1033.9, 987.6, 951, 871.9, 787 186 Figure 37. 'H NMR Spectra of a-(2,4,6-Triethylphenyl)propiophenone Before and After Irradiation in Toluene (D290 nm) 187 4,6—DiethyI-E,Z-lé-dimethyl-Z-phenyl—Z-indanol lH NMR(CDC13): 5 0.82 (d, J=7.0 HZ, 3H, CH3CH), 1.291 (t, J=7.56 Hz, 3H, CH3CH2), 1.294 (t, J=7.56 Hz, 3H, CH3CH2), 1.36 (d, J=7.0 Hz, 3H, CH3CH), 2.0 (broad s, 1H, OH), 2.6 (dq, J=7.56, 14.3 Hz, 2H, CHZCH3). 2.7 (q, J=7.8 Hz, 2H, CHZCH3), 3.30 (q, J=7.0 Hz, 1H, CHCH3) , 3.95 (q, J=7.0 Hz, 1H, CHCH3),6.92 (s, 2H, Ar), 7.30 (t, J=7.3 Hz, 1H, Ar), 7.40 (2H, dd, J=7.3, 7.5 Hz, 2H, Ar), 7.6 (d, J=7.5 Hz, 2H, Ar) lH NMR(Toluene-d8): 5 0.8 (d, J=7.1 Hz, 3H, CH3CH), 1.16-1.3 (m, 9H), 2.0 (broad s, 1H, OH), 2.52 (dq, J=7.2, 14.4 Hz, 2H, CHZCH3), 2.61 (q, J=7.5Hz, 2H, CHZCH3), 3.32 (q, J=7.1 Hz, 1H, CHCH3), 3.71 (q, J=7.1 Hz, 1H, CHCH3), 6.8-7.3 (m, 7H, Ar) l3C NMR(CDCl3): 5 10.58, 15.28, 15.72, 17.20, 24.95, 28.95, 42.20, 50.65, 87.92, 121.04, 126.08, 126.70, 127.26, 128.24, 139.92, 141.20, 141.73, 143.42, 143.84 IR(CC14): 3572, 3061.4, 3030.6, 2966.9, 2932.2, 1033.9, 987.6, 951, 871.9, 787 Products from a—(2-Benzylphenyl)acetophenone (6) or—(2-Benzylphenyl)acetophenone (0.003 g) in 0.8 mL of deuterated benzene was irradiated until no trace of starting material could be detected by NMR. The signals for two isomeric indanols in a 1:1 ratio were detected. NOe experiments were performed on isolated indanols to correctly assign their stereochemical arrangement. The effect of temperature and phase on product ratios was also investigated by conducting the photochemistry in acetone/ethanol, ice-water and silicon oil (110°C) baths and in solid. The diasteriomeric ratio of indanols was determined by NMR integration of the methylene (AB quartet) signals corresponding to each isomer. Large scale irradiation (0.4 188 g in 100 mL benzene) was performed and the two indanols were separated by preparative scale tlc using 5% ethyl acetate in hexane solution. The Z-indanol was the first eluted isomer. Ph 0 6 6indZ 6indE Scheme 66. Photoproducts of a-(2-Benzy1phenyl)acetophenone Z-lg-diphenyl-Z-indanol 1H NMR(CDC13): 5 1.85 (s, 1H, OH), 3.4, 3.65 (AB quartet, J=16.5 Hz, 2H, CH2), 4.95 (s, 1H, CHPh), 7.05 (dd, J= 7.38, 2.97 Hz, 2H, Ar), 7.12 (d, J= 7.41 Hz, 1H, Ar), 7.2-7.45 (m, 9H, Ar), 7.53 (d, J= 7.38 Hz, 2H, Ar) lH NMR(Toluene-d8): 5 1.85 (s, 1H, OH), 3.22, 3.33 (AB quartet, J=16.2 Hz, 2H, CH2), 4.64 (s, 1H, CHPh), 7.00-7.6 (m, 14H, Ar) l3C NMR(CDC13): 5 48.93, 63.92, 84.99, 124.85, 125.36, 125.49, 126.84, 127.46, 127.64, 128.04, 128.48, 129.97, 136.15, 141.71, 142.74, 145.18 IR(CC14): 3557, 3030.6, 1495, 1452.6, 1286.7, 1053.3, 702.18 Noe (CDC13): irradiation of the peak at 5 1.85 (OH) enhanced peaks at 3.4 ppm (2%), and 7.0-7.6 ppm (25%) 189 Irradiation of the peak at 5 4.95 ppm (methine) enhanced peaks at 3.4 ppm (2.5%), 3.65 ppm (2.1%), 7.05,7.12 ppm (27%), 7.2-7.45 ppm (18.6%), and 7.53 ppm (3.0%) Irradiation of the peak at 5 3.65 ppm enhanced peaks at 3.4 ppm (37%), 4.95 ppm (1.3%), and 7.0-7.4 ppm (32%) Irradiation of the peak at 5 3.4 ppm enhanced peaks at 1.85 ppm (3.8%), 3.65 ppm (22%), and 7.0-7.6 ppm (16%) E—l -di hen l-2-indanol lH NMR(CDC13): 5 2.45 (broad s, 1H, OH), 3.30, 3.85 (AB quartet, J=16 Hz, 2H, CH2), 4.61 (s, 1H, CHPh), 6.61 (dd, J=7.86, 1.92 Hz, 2H, Ar), 6.90-7.10 (m, 8H, Ar), 7.13 (1H, d, J=7.71 Hz), 7.25 (t, J=7.14 Hz, 1H, Ar), 7.34 (t, J=7.14 Hz, 1H, Ar), 7.43 (d, J=7.2 Hz, 1H, Ar) 'H NMR(Toluene-d3): 5 1.85 (s, 1H, 0H), 2.94. 3.53 (AB quartet, J=16.2 Hz, 2H, CH2), 4.45 (s, 11-1,CHPh), 6.8-7.6 (m, 14H, Ar) ”C NMR(CDC13): 5 46.0, 65.18, 87.3, 124.6, 125.96, 126.0, 126.3, 126.87, 127.2, 127.4, 127.6, 128.9, 139.6, 141.5, 142.64, 144.0 IR(CC14): 3560, 3030.5, 1495, 1286, 702.3 Noe (CDC13): irradiation of the peak at 5 2.45 ppm (OH) enhanced peaks at 3.3 ppm (1%), and 4.61 (2.1%) Irradiation of the peak at 5 4.61 ppm (methine) enhanced peaks at 2.45 ppm (5.5%), 6.60 ppm (12%), and 6.9-7.1 ppm (14.5%) 190 Irradiation of the peak at 5 6.60 ppm enhanced peaks at 3.3 ppm (3%), 4.61 ppm (7.75%), and 6.9-7.14 ppm (24%). Products from a—(Z-Benzylphenyl)propiophenone ( 7) a-(2-Benzylphenyl)propiophenone (0.005 g) in 0.8 mL of deuterated benzene was irradiated until no trace of starting material could be observed by NMR. The signals for two isomeric indanols and two diarylethanes were detected upon analysis of the NMR spectrum of the photolysis mixture. The diasteriomeric ratio of indanols was determined by NMR integration of methyl doublet signals corresponding to each isomer. Products were separated by performing large scale irradiation using 0.30 g of 01—(2- benzylphenyl)propiophenone in 100 mL of benzene. Solvent was evaporated to leave a yellow oil which was chromatographed by PTLC using 3% ethyl acetate in hexane solution. The diarylbutanes moved with the solvent line and had a rf value of nearly 1.0, the indanols had an rf value of nearly 0.4 with the ZZ-indanol having a slightly higher value. The indanols were recovered as oils. Ph / \ 7cleav-Two isomers Scheme 67. Photoproducts of a—(Z-Benzylphenyl)propiophenone 191 Figure 38. 1H NMR Spectra of a-(2-BenzylphenyI)acetophenone Before and After Irradiation in Toluene (2)290 nm) 192 Z-l-meth 1-3 -di hen l-Z-indanol lH NMR(CDC13): 5 1.30 (d, J= 6.72 Hz, 3H, CH3CH), 2.20 (broad s, 1H, OH), 3.95 (q, J=6.72 Hz, 1H, CHCH3), 4.50 (s, 1H, CHPh), 6.50 (dd, J=7.7, 1.9 Hz, 2H, Ar), 6.9-7.3 (10H, m, Ar), 7.4 (d, J=7.0 Hz, 2H, Ar) l3C NMR(CDC13): 5 10.9, 44.8, 64.8, 88.8, 123.9, 126, 126.2, 126.3, 126.9, 127.5, 127.6, 127.7, 128.1, 128.8, 139.9, 141.2, 143.4, 145.8 IR(CC14): 3570, 3065.3, 3028.6, 2963, 2932.2, 1475.9, 1275.1, 1076.4, 1032, 951, 873.8, 785.1, 729.2, 702.18 Z-l-methyl-3 (Z),2-diphenyl-2-indanol 1H NMR(CDC13): 5 1.25 (d, J= 6.72 Hz, 3H, CH3CH), 1.60 (broad s, 1H, OH), 3.66 (q, J=6.72 Hz, 1H, CHCH3), 4.95 (s, 1H, CHPh),7.0 (dd, J=7.4, 3.0 Hz, 2H, Ar), 7.10 (d, J: 7.4 Hz, 1H, Ar), 7.2-7.4 (m, 9H, Ar), 7.5 (d, J= 6.9 Hz, 2H, Ar) l3C NMR(CDC13): 5 10.2, 50.6, 62.8, 87.8, 123.3, 125.2, 125.8, 126.8, 126.9, 127.5, 128, 128.4, 130, 136, 141.8, 143.4, 145.9 IR(CC14): 3584, 3065.3, 2966.9, 2928.3, 1495, 1176.7, 1076.4, 972.3, 873.9, 729.2, 698.3 2R1SléRiS)-Di(2’-ben_zylphenyl)butane lH NMR(CDC13): 5 0.6 (d, J= 6.72 Hz, 6H, 2CH3CH), 3.10 (broad, 2H, 2CHCH3), 4.0 (AB quartet, J= 15.8 Hz, 4H, 2CH2Ph), 6.8-7.3 (m, 18H, Ar) 13C NMR(CDC13): 5 20.7, 38.7, 40.4, 125.6, 125.8, 126.4, 126.9, 128.8, 130.1, 138.3, 141.1,145.4 193 2R(SL381R)-Di(2’-begglphenyl)butane IH NMR(CDC13): 5 1.10 (d, J: 6.72 Hz, 6H, 2CH,CH), 3.20 (broad, 2H, 20101,), 3.7 (AB quartet, J= 15.8 Hz, 4H, 2CH2Ph), 6.8-7.3 (m, 18H, Ar) l3C NMR(CDC13): 5 20.5, 38.7, 39.6, 125.4, 125.9, 126.3, 126.8, 128.7, 130.7, 137.5, 141.2, 145.3 Products from a-Mesifllpropiophenone (8) a—Mesitylpropiophenone (0.002 g) in 0.8 mL of deuterated benzene was irradiated until no trace of starting material could be observed by NMR. The signals for two isomeric indanols were detected upon analysis of the NMR spectrum of the photolysis mixture. In our investigation, photochemistry was conducted at various temperatures to ascertain the effect of temperature on product ratios. The diasteriomeric ratio of indanols was determined by NMR integration of the methyl doublet signals corresponding to each isomer. In order to separate the two indanols, large scale irradiation using 0.25 g of a—mesitylpropiophenone in 100 mL of benzene was performed. Solvent was evaporated to leave a colorless oil which was chromatographed by PTLC using 3% ethyl acetate in hexane solution. The Z-isomer was the first compound eluted. O Toluene 8 8indZ 8indE Scheme 68. Photoproducts from a-Mesitylpropiophenone 194 Z-l,5,7-Trimethyl-2-phenyl-Z-indanol lH NMR(CDC13): 5 1.36 (d, J=7.0 Hz, 3H, CH3CH), 2.10 (broad s, 1H, OH), 2.35 (s, 3H, CH3Ar), 2.37 (s, 3H, CH3Ar), 3.35 (AB quartet, J=15.6 Hz, 2H, CH2), 3.55 (q, J=7.0 Hz, 1H, CHCH3), 6.90 (s, 1H, Ar), 6.95 (s, 1H, Ar), 7.10 (t, J=6.8 Hz, 1H, Ar), 7.25 (2H, dd, J=6.8, 7.0 Hz, 2H, Ar), 7.53 (d, J= 7.0 Hz, 2H, Ar) lH NMR(Toluene-d3): 5 1.15 (d, J=7.2 Hz, 3H, CH3CH), 1.7 (broad s, 1H, OH), 2.06 (s, 3H, CH3Ar), 2.15 (s, 3H, CH3Ar), 3.05, 3.12 (AB quartet, J=15.9 Hz, 2H, CH2), 3.23 (q, J= 7.2 Hz, 1H, CHCH3), 6.90-7.5 (m, 7H, Ar) l3C NMR(CDC13): 5 13.18, 18.77, 20.80, 47.42, 49.48, 83.55, 122.47, 124.76, 126.46, 127.74, 129.37, 133.5, 136.26, 139.72, 140.65, 146.52 IR(CC14): 3602, 2976, 2939, 1455, 1374, 1248.9, 1036, 845.5, 700.25 E-l,5,7-Trimethyl-2-phenyI-Z-indanol lH NMR(CDC13): 5 0.70 (d, J=7.0 Hz, 3H, CH3CH), 2.0 (1H, broad s, 1H, 0H), 2.99 (s, 3H, CH3Ar), 2.31 (s, 3H, CH3Ar), 3.0,3.85 (AB quartet, 1=15.4 Hz, 2H, CH2), 3.35 (q, J=7.0 Hz, 1H, CHCH3), 6.85 (s, 1H, Ar), 7.0 (s, 1H, Ar), 7.30 (t, J=6.9 Hz, 1H, Ar), 7.40 (dd, J=6.9, 7.1 Hz, 2H, Ar), 7.58 (d, J=7.1 Hz, 2H, Ar) lH NMR(Toluene-d3): 5 0.62 (d, J=7.2 Hz, 3H, CH3CH), 1.7 (broad s, 1H, OH), 2.09 (s, 3H, CH3Ar), 2.21 (s, 3H, CH3Ar), 2.63, 3.58 (AB quartet, J=15.9 Hz, 2H, CH2), 3.18 (q, J= 7.2 Hz, 1H, CHCH3), 6.90-7.5 (m, 7H, Ar) IR(CC14): 3462, 3061.4, 2968.8, 1448, 1240.3, 912.4, 848.8, 700.25 195 hv + o I. . my", 1‘ Ph C A H3 CH3 A L Y—r 1 v v v -—r i v 1 T v f *7 1 T fi' ' 1 v v i fi 7 6 s 4 3 2 1 ppm Figure 39. 1H NMR Spectra of ot-Mesitylpropiophenone Before and After Irradiation in Toluene 09290 nm) 196 Products from a—(2,4,6-Triisopropylphenyl)acetophenone ( 9) a-(2,4,6-Triisopropylphenyl)propiophenone (0.005 g) in 0.8 mL of deuterated benzene was irradiated through Pyrex filter. The signals for two products, an enol and an indanol, were detected upon analysis of the NMR spectrum of the photolysis mixture. The effect of temperature and phase on product ratios was also investigated by conducting the photochemistry in acetone/ethanol, ice-water and silicon oil (110°C) baths and in solid. A small amount of the other disproportionation product, 1-phenyl-2-(2-(2- propenyl)-4,6-diisopropylphenyl)ethanol, was observed at 24°C and 90°C irradiations. The enol indanol ratio was determined by NMR integration of the vinylic singlet signals of the enols and the upfield methyl singlet signal of the indanol. In order to separate the products, large scale irradiation using 0.40 g of 01—(2,4,6-triisopropylphenyl) propiophenone in 100 mL of benzene was performed. Solvent was evaporated to leave a yellow solid which was separated by PTLC using 3% ethyl acetate in hexane solution. 9ean 9alc Scheme 69. Photoproducts of 01-(2,4,6-Triisopropylphenyl)acetophenone '2'. 5' 5 Figure 40. 1H NMR of a-(2,4,6-Triisopropylphenyl)acetophenone After Irradiation in Toluene (A > 290nm) E 2 r1 Md! 197 lLA_LA111ALIJLLL11AL1ILJLLIAA 198 WWW lH NMR(CDC13): 5 0.78 (s, 3H, CH3), 1.29 (d, J=7.3 Hz, 12H, 2 (CH3)2CH), 1.36 (s, 3H, CH3), 2.14 (broad s, 1H, OH), 2.92 (septet, J= 7.2 Hz, 2H, 2CH(CH3)2), 3.08, 3.81 (AB quartet, J= 16.1 Hz, 2H, CH2), 6.90 (s, 1H, Ar), 7.0 (s, 1H, Ar), 7.24-7.40 (m, 3H, Ar). 7.60 (d, J= 7 Hz, 2H, Ar) lH NMR(Toluene-dg): 5 0.75 (s, 3H, CH3), 1.20 (d, J=7.2 Hz, 6H, 2 (CH3)2CH), 1.30 (d, J=7.2 Hz, 12H, 2 (CH3)2CH), 1.35 (s, 3H, CH3), 2.80, 3.60 (AB quartet, J= 16.1 Hz, 2H, CH2), 2.85 (septet, J= 7.2 Hz, 1H, CH(CH3)2), 3.30 (septet, J= 7.2 Hz, 2H, 2CH(CH3)2), 6.90 (s, 1H, Ar), 7.1 (s, 2H, Ar), 7.1-7.3 (m, 3H, Ar), 7.5 (d, J: 7 Hz, 2H, Ar) l3C NMR(CDC13): 5 19.6, 22.9, 23.1, 24.2, 24.3, 28.1, 31.0, 34.4, 42.2, 51.6, 87.2, 118.4, 121.6, 126.6, 127.1, 127.7, 133.6, 141.8, 144.8, 148.4, 150.3 IR(neat): 3420, 3080,2850, 1494, 1384, 876.8 cm'1 1Z1-1-Phenyl-2j2,4,6-triisopropylphenyl)ethenol lH NMR(Toluene-d3): 5 1.20 (d, J=7.2 Hz, 6H, 2 (CH3)2CH), 1.30 (d, J=7.2 Hz, 12H, 2 (CH3)2CH), 2.85 (septet, J= 7.2 Hz, 1H, CH(CH3)2), 3.30 (septet, J= 7.2 Hz, 2H, 2CH(CH3)2), 4.75 (broad s, 1H, OH), 6.1 (s, 1H, Vinyl), 7.0-7.2 (m, 3H, Ar), 7.2 (s, 2H, Ar), 7.8 (d, 1= 7 Hz, 2H, Ar) I lH NMR(Methanol-d4): 5 1.16 (d, J= 7.2 Hz, 6H, (CH3)2CH), 1.18 (d, J= 7.2 Hz, 6H, (CH3)2CH), 1.24 (d, J: 7.2 Hz, 6H, (CH3)2CH), 2.85 (septet, J= 7.2 Hz, 2H, 2CH(CH3)2), 3.27 (septet, J: 7.2 Hz, 1H, CH(CH3)2), 5.91 (s, 1H, vinylic), 7.0 (s, 1H, Ar), 7.2-7.4 (m, 5H, Ar), 7.70 (d, 1: 7 Hz, 2H, Ar) 199 (E)-l-Phenyl-2-(2,4,6-triisopropylphenyl)ethenol lH NMR(Toluene-d8): 5 1.10 (d, J=7.2 Hz, 6H, 2 (CH3)2CH), 1.18 (d, J=7.2 Hz, 12H, 2 (CH3)2CH), 2.85 (septet, J= 7.2 Hz, 1H, CH(CH3)2), 3.30 (septet, J= 7.2 Hz, 2H, 2CH(CH3)2), 4.75 (broad s, 1H, OH), 6.4 (s, 1H, Vinyl), 7.0 (s, 2H, Ar), 7.1-7.2 (m, 3H, Ar), 7.7 (d, J= 7 Hz, 2H, Ar) lH NMR(Methanol-d4): 5 0.88 (d, J: 7.2 Hz, 6H, (CH3)2CH), 1.08 (d, J= 7.2 Hz, 6H, (CH3)2CH), 1.2 (d, J= 7.2 Hz, 6H, (CH3)2CH), 2.85 (septet, J= 7.2 Hz, 2H, 2CH(CH3)2), 3.27 (septet, J= 7.2 Hz, 1H, CH(CH3)2), 5.88 (s, 1H, vinylic), 6.90 (s, 1H, Ar), 7.2-7.4 (m, 5H, Ar), 7.65 (d, J= 7 Hz, 2H, Ar) l-Phenyl-2-12-(2-propenyl)4,6-diisopropylp_henyl)ethanol lH NMR(Toluene-d8): 5 1.15 (d, J=7.2 Hz, 3H, (CH3)2CH), 1.25 (d, J=7.2 Hz, 3H, (CH3)2CH),1.3 (6H, t, J=7.2 Hz, 6H, (CH3)2CH), 1.6 (broad s, 1H, OH), 1.95 (s, 3H, allylic CH3), 2.85 (septet, J= 7.2 Hz, 1H, CH(CH3)2), 3.1, 3.24 (2H, AB quartet of d, J= 8.4, 2.7, 5.4 Hz, 2H, CH2), 3.45 (septet, J= 7.2 Hz, 1H, CH(CH3)2), 4.79 (1H, dd, J= 2.7, 5.4 Hz, 1H, CHOH), 4.85 (d, J= 1.5 Hz, 1H, vinylic), 5.15 (d, J= 1.5 Hz, 1H, vinylic), 6.95 (s, 1H, Ar), 7.05 (s, 1H, Ar), 7.1-7.2 (m, 3H, Ar), 7.3 (2H, d, 1= 7 Hz, 2H, Ar) IR(CC14): 3582.3, 2964, 2931.2, 1464.2, 1384.1, 1167, 1055.2, 901.8, 808.3, 738.8 Products from 1-Trimethylsiloxy-I-phenyl-2-(2 ’,4 ’,6 ’-triisopropylphenyl)ethene Photochemical conversion of enol to indanol was checked by synthesis and irradiation of trimethylsilyl enol ether of a-(2,4,6triisopropylphenyl)acetophenone. The 200 Z-enol ether was synthesized by treatment of ketone with KH and trimethylsilyl chloride. Irradiation of this enol ether in benzene resulted in formation of the E-isomer but no indanol or ketone. —- hv — OSiMea P“ 1H NMR(C6D6): 5 -0.1 (s, 9H, Si(CH3)3), 1.3-1.5 (broad, 18H, 3 (CH3)2CH), 2.85 (septet, J= 7.1 Hz, 1H, CH(CH3)2), 3.5 (septet, J=7.2 Hz, 2H, 2 CH(CH3)2), 6.5 (s, 1H, vinylic), 7.0-7.2 (m, 5H, Ar), 7.7 (d, J: 6.9 Hz, 2H, Ar) l3C NMR(CDC13): 5 0.13, 24.21, 29.74, 30.55, 34.41, 107.28, 120.24, 125.43, 127.76, 128.24, 129.93, 147.28, 147.61, 149.33 E-l-Trimeth lsilox -l- hen 1-2- 2’ 4’ 6’-triiso ro 1 hen lethene 1 H NMR(C6D6): 5 0.0 (s, 9H, Si(CH3)3), 1.3-1.5 (broad, 18H, 3 (CH3)2CH), 2.85 (septet, J: 7.1 Hz, 1H, CH(CH3)2), 3.5 (septet, J=7.2 Hz, 2H, 2CH(CH3)2), 6.7 (s, 1H, vinylic), 7.0-7.2 (m, 5H, Ar), 7.5 (d, J= 6.9 Hz, 2H, Ar) 201 Products from a—(2-Ethylphenyl)acetone (10) a—(2-Ethy1phenyl)acetone (0.002 g) in 0.8 mL of deuterated benzene was irradiated until starting material could not be observed by NMR. The signals for three products were detected in the NMR spectrum of the mixture. These products included two isomeric indanols and a diarylethane. The effect of temperature and phase on product ratios was also investigated by conducting the photochemistry in acetone/ethanol, ice- water and silicon oil (110°C) baths and in solid. The product ratios were determined by NMR integration of the methyl doublet signals of the indanols and the methylene singlet signal of the diarylethane. The structural assignments of the indanols was accomplished by performing shift and nOe experiments. Addition of Rondeau’s reagent to 0.01 M solution of each indanol in CDC13, caused an upfield shift of all proton signals. However, the methine signal in the minor isomer moved upfield twice as much as the methyl signal, while the upfield shifts of both methyl and methine signals in the major isomer were comparable. Furthermore, irradiation of the methine signal in the minor isomer caused an enhancement of the OH signal. These data strongly suggest that the minor isomer has an E-stereochemistry. Large scale irradiation using 0.20 g of oc—(2-ethylphenyl)acetone in 150 mL of toluene was performed until 100% conversion (GC). Solvent was removed to leave a yellow oil which was chromatographed by PTLC using 3% ethyl acetate in hexane to separate the products. The Z-indanol was the first eluted isomer. The indanols were recovered as oils. 202 10 Scheme 71. Photoproducts of a-(2-Ethylphenyl)acetone Z-lg-Dimethyl-Z-indanol lH NMR(CDC13): 5 1.28 (d, J=7.1 Hz, 3H, CH3CH), 1.45 (s, 3H, CH3), 2.93 (Half of an AB quartet, J=16 Hz, 1H, CH2), 2.97 (q, J= 7.1 Hz, 1H, CHCH3), 3.02 (Half of an AB quartet, J= 16 Hz, 1H, CH2), 7.13-7.23 (m, 4H, Ar) lH NMR(C6D6): 5 1.12 (d, J=7.2 Hz, 3H, CH3CH), 1.2 (s, 3H, CH3), 1.6 (s, 1H, OH), 2.65 (q, J=7.2 Hz, 1H, CHCH3), 2.7 (AB quartet, J= 15.94 Hz. 2H, CH2), 7.0-7.15 (m, 4H, Ar) lH NMR(Toluene-d8): 5 1.11 (d, J=7.2 Hz, 3H, CH3CH), 1.18 (s, 3H, CH3), 1.6 (s, 1H, OH), 2.65 (q, J=7.2 Hz, 1H, CHCH3), 2.7 (AB quartet, J= 15.94 Hz, 2H, CH2), 7.0-7.15 (m, 4H, Ar) l3C NMR(C6D6): 5 14.5, 25.4, 47.7, 49.3, 81.1, 124, 125.1, 126.8, 126.9, 141.2, 146.9 IR(CC14): 3580.4, 3072.9, 3024.7, 2966.9, 2934.1, 1460.3, 1246.2, 1157.4, 1072.6, 951, 775.4, 763.9, 740.7 203 Figure 41. 1H NMR of the Indanol Mixture from a-(2-Ethylphenyl)acetone in Benzene 204 IH NMR(C6D6): 5 1.0 (d, J=7.2 Hz, 3H, CH3CH), 1.02 (s, 3H, CH3), 2.73 (AB quartet, J= 15.5 Hz, 2H, CH2), 2.88 (q, 1: 7.2 Hz, 1H, CHCH3), 7.0 (dd, J=2.4, 2.3 Hz, 1H, Ar), 7.03 (d, J=1.4 Hz, 1H, Ar), 7.05 (d, J=2.4 Hz, 1H, Ar), 7.09 (dd, J=2.3, 1.4 Hz, 1H, Ar) lH NMR(Toluene-d8): 5 1.0 (d, J=7.2 Hz, 3H, CH3CH), 0.99 (s, 3H, CH3), 2.73 (AB quartet, J= 15.5 Hz, 2H, CH2), 2.88 (q, J= 7.2 Hz, 1H, CHCH3), 7.0 (dd, J=2.4, 2.3 Hz, 1H, Ar), 7.03 (d, J=1.4 Hz, 1H, Ar), 7.05 (d, J=2.4 Hz, 1H, Ar), 7.09 (dd, J=2.3, 1.4 Hz, 1H, Ar) lH NMR(CDC13): 5 1.19 (d, J=7.3 Hz, 3H, CH3CH), 1.30 (S, 3H, CH3), 2.96 (collapsed AB quartet, 2H, CH2), 3.05 (q, J=7.2 Hz, 1H, CHCH,), 7.0—7.3 (m, 4H) ”C NMR(C6D6): 5 14.4, 22.6, 47.4, 50.9, 82.0, 123.9, 124.9, 126.8, 126.9, 127.9, 147.0 IR(CC14): 3431.8, 3072.9, 3024.9, 2964.7, 2932.2, 1255.8, 1145.8, 1032, 987.7, 927.9, 763.9, 740.7 Shift Reagent Experiments: Addition of Rondeau’s reagent, tris(6,6,7,7,8,8,8-heptafluoro-2,2-dimethyl-3,5- octandionato) praseodymium, to 0.01 M solution of each indanol in CDC13, caused the following upfield shifts: Z-lJ-Dimethyl-Z-indanol: methyl doublet signal at 1.30 ppm moved to 1.01 ppm, methyl singlet signal at 1.47 ppm moved to 1.06 ppm, methine quartet signal at 2.97 ppm moved to 2.68 ppm, and the AB quartet signals at 2.95 and 3.04 ppm moved to 2.54 and 2.74 ppm. 205 E-l,2-Dimethy1—2-indanol: methyl doublet signal at 1.18 ppm moved to 1.13 ppm, methyl singlet signal at 1.27 ppm moved to 1.20 ppm, methine quartet signal at 3.05 ppm move to 2.96 ppm, and the AB quartet signal at 2.96 ppm moved to 2.98 and 2.86 ppm. Addition of tris(2,2,6,6-tetramethyl-3,5-heptandionato)europium reagent to the mixture of indanols in CDC13 caused the following downfield shifts: Z-lJ-Dimethyl—Z-indanol: methyl doublet signal at 1.30 ppm moved to 1.33 ppm, methyl singlet signal at 1.47 ppm moved to 1.52 ppm. The other peaks could not be identified due to peak broadening. E-lJ-Dimethyl-Z-indanol: methyl doublet signal at 1.19 ppm moved to 1.23 ppm, methyl singlet signal at 1.27 ppm moved to 1.34 ppm. The other peaks could not be identified due to peak broadening. NOe Experiments: Z-lJ-Dimethyl-Z-indanol: Irradiation of the signal at 1.30 ppm (CDC13) caused the following enhancements: 2.96-3.05 ppm (3%), 7.1-7 .3 ppm (3.1%) Irradiation of the signal at 1.47 ppm caused the following enhancements: 2.96-3.05 ppm (4%), 7.1-7.3 ppm (1.6%) E-l,2-Dimethyl-2-indanol: Irradiation of the signal at 2.73 ppm (C6D6) caused the following enhancements: 1.0-1.05 ppm (1.0%), 1.6 ppm (0.4%), 6.9-7.1 ppm (1.7 %) Irradiation of the signal at 2.88 ppm caused the following enhancements: 1.0-1.05 (0.8%), 1.6ppm (0.6%), 6.9-7.1 ppm (2%) 206 lg-Dii2’-ethylphenyl)ethane lH NMR(CDC13): 5 1.22 (t, J=7.5 Hz, 6H, 2CH3CH2), 2.67 (q, J= 7.6 Hz, 4H, 2CH2CH3), 2.8 (s, 4H, 2CH2). 7.1-7.2 (m, 8H, Ar) ”C NMR(CDC13): 5 15.4, 25.5, 34.3, 125.9, 126.3, 128.5, 129.1 Products from a—Mesitylacetone (11) a-Mesitylacetone (0.002 g) in deuterated benzene was irradiated until starting material could not be observed by NMR. Two products were detected in the NMR spectrum of the mixture and were identified as an indanol and a diarylethane. The effect of temperature and phase on product ratios was also investigated by conducting the photochemistry in acetone/ethanol and silicon oil (110°C) baths and in solid. Product ratios were determined by NMR integration of the methylene signals of the indanol (AB quartet) and the diarylethane (singlet). Large scale irradiation using 0.20 g of or— mesitylacetone in 100 mL of benzene was performed until 100% conversion by GC. Solvent was removed to leave a yellow oil which was chromatographed by PTLC using 3% ethyl acetate in hexane to separate the products. The indanol was eluted after the diarylethane and was recovered as an oil. 1 1 l lind 1 lcleav Scheme 72. Photoproducts of ot-Mesitylacetone 207 OE'I SZ'I OZ'I A ‘4- --—1 In! 00'! .—H SI'I 1.104 L >. Low onr 15 cams mun) 00 m Figure 42. 1H NMR of the Methyl Region of the Indanol Mixture from 01-(2- Ethylphenyl)-acetone in Benzene 'I SO 0! 1 0‘0 r——L—fi 00.1 OT 1 1 1 1 1 1 1 1 1 1 1 4L4} 1 J 1,L 1 J, 1 1 1 1 1 1 1 1 1 1 1 J .Lml 1 1 1 1 1 1, 1 1 1 1 1 141 J 1 1 1 1 '9 56'0 '0 06 v 90'0 208 . 8. + at o _ to sos'z——— N tzs'z < . tn __ so a: =— Lmt— _ N Iu'z , ’ii‘;— 9 4 r " _ N ItL'Z >- < P- L no «we __ p. P N a: rust oIL'z—r——-——-— * 1- o __ a to": . _ N 1.. P ‘3 250': *‘ . L N ”r: 000': ~ sort 0 _. at _ N Figure 43. 1H NMR of the Methylene Region of the Indanol Mixture from 01-(2- Ethylpheny1)acetone in Benzene 209 lH NMR(C6D6): 5 1.30 (s, 3H, CH3), 2.05 (s, 3H, CH3Ar), 2.20 (s, 3H, CH3Ar), 2.65 (AB quartet, J: 16.6 Hz, 2H, CH2), 2.80 (AB quartet, J: 16.5 Hz. 2H, CH2), 6.72 (s, 1H, Ar), 6.73 (s, 1H, Ar) IH NMR(CDC13): 5 1.63 (s, 3H, CH3), 2.13 (s, 3H, CH3Ar), 2.33 (s, 3H, CH3Ar), 3.0 (Half of an AB quartet, J=16.6 Hz, 1H, CH2), 3.1 (Half of an AB quartet, J=16.5 Hz, 1H, CH2), 3.25 (Half of an AB quartet, J= 16.6 Hz, 1H, CH2), 3.35 (Half of an AB quartet, J: 16.5 Hz, 1H, CH2), 6.79 (s, 1H, Ar), 6.81 (s, 1H, Ar) l3C NMR(C6D6): 5 19.0, 21.3, 28.0, 47.0, 48.9, 79.3, 123.3, 128.5, 133.7, 136.1, 137.9, 141.9 IR(CCl4): 3443, 2968.8, 2926.4, 1469.9, 1448.7, 1230.7, 1076.4, 895, 873.8, 850.7, 702.2 LZL-Difimesitylethane lH NMR(CDC13): 5 2.3 (s, 6H, 2CH3), 2.4 (12H, s, 4 CH3), 2.8 (s, 4H, 2CH2), 6.9 (s, 4H, Ar) 13C NMR(CDC13): 5 20.1, 20.8, 28.9, 129.1, 135.2, 135.7, 136.3 Products from a—(2,4,6-Triethylphenyl)acetone (12) a—(2,4,6-Triethylphenyl)acetone (0.004 g) in deuterated toluene was irradiated until starting material could not be observed by NMR. The signals for several products were detected in the NMR spectrum of the mixture. These products included two isomeric indanols and a diarylethane. The peaks for the two isomeric indanols overlap 210 and separation is difficult. The Z-stereochemistry for the major indanol was based on the comparison of the peaks to that of the Z-indanol of a—(2-ethylphenyl)acetone. Product ratios were determined by NMR integration of methyl doublet signals of indanols and the methylene singlet signal of the diarylethane. Large scale irradiation using 0.30 g of or- (2,4,6-triethylphenyl)acetone in 100 mL of benzene was performed until 100% conversion by GC. Solvent was removed to leave a yellow oil which was chromatographed by PTLC using 5% ethyl acetate in hexane to separate the products. The indanols had a lower rfvalue than the diarylethane which had moved with the solvent line. 12 12indZ 12indE 12cleav Scheme 73. Photoproducts of a-(2,4,6-Triethylphenyl)acetone 4 6-Dieth M Z -dimeth 1-2-indanol lH NMR(C,D,): 5 1.12 (t, J= 7.5 Hz, 3H, CH3CH2). 1.19 (d, J: 7 Hz, 3H, CH3CH), 1.20 (t, J: 7.5 Hz, 3H, CH3CH2), 1.26 (s, 3H, CH3), 2.44 (q, J= 7.5 Hz, 2H, CHZCHg), 2.56 (q, .1: 7.5 Hz, 2H, C CH2H3), 2.62 (Half ofAB quartet, J: 16 Hz, 1H, CH2), 2.72 (1H, q, 1: 7.5 Hz, 1H, CHCH3), 2.74 (Half of AB quartet, J= 16 Hz, 1H, CH2). 6.85 (s, 2H, Ar) 13 C NMR(C6D6): 5 11.6, 14.9, 16.5, 25.4, 26.8, 29.4, 45.6, 49.3, 80.9, 121.1, 125.9, 143.3, 146.9 211 IR(CC14): 3440, 2968, 2930, 1470, 1076.4, 895, 704.2 4 6—Dieth l-l -dimeth l-2-indanol lH NMR(C6D6): 5 1.11 (d, J: 7.5 Hz, 3H, CH3CH), 1.13 (s, 3H, CH3). 1.15 (t, J=7.5 Hz, 3H, CH3CH2), 1.20 (t, J=7.5 Hz, 3H, CH3CH2), 2.43 (AB quartet, J: 14 Hz, 2H, CH2), 2.48 (q, J: 7.5 Hz, 2H, CH2CH3), 2.56 (q, J= 7.5 Hz, 1H, CHCH3), 2.62 (q, J= 7.5 Hz, 2H, CHZCH3). 6.81 (s, 1H, Ar), 7.05 (s, 1H, Ar) l,2-Di(2,4,6-triethylphenyl)ethane IH NMR(C,D,): 5 1.15 (t, J: 7.5 Hz, 12H, 4CH3CH2), 1.2 (t, J: 7.5 Hz, 6H, 2CH3CH2), 2.5 (q, 1: 7.5 Hz, 4H, CHZCH3), 2.7 (q, I: 7.5 Hz, 8H, 2CH2CH3), 2.85 (s, 4H, Ar), 6.9 (s, 4H, Ar) Products from a—(2,4,6-Triisopropylphenyl)acetone (13) 01—(2,4,6-Triisopropylphenyl)acetone (0.005 g) in deuterated benzene was irradiated. The signals for three products were detected in the NMR spectrum of the mixture. One of these products, the enol, disappears as the irradiation time (percent conversion) increases. The signals for two products were detected at 100% conversion in the NMR spectrum of the photolysis mixture. These products included an indanol and a diarylethane. The indanol/diarylethane ratio was determined by NMR integration of the methyl singlet signal of the indanol and the methylene singlet signal of the diarylethane. Large scale irradiation using 0.30 g of a—(2,4,6-triisopropylphenyl)acetone in 100 mL of toluene was performed until 100% conversion (GC). Solvent was removed to leave a 212 yellow oil which was chromatographed by preparative scale tlc using hexane to separate the products. The indanol was the second fraction eluted and was recovered as an oil. . \ CH3 H H CH3 \ 1 / O hV .‘CHa + — CH C D 6 6 H3O ”CH3 13 13ind 13enl 13cleav Scheme 74. Photoproducts of 01-(2,4,6-Triisopropy1pheny1)acetone 4 6-Diiso ro 1-11 -trimeth l-2-indanol lH NMR(CDC13): 5 1.10 (s, 3H, CH3), 1.25 (6H, t, J= 6.84 Hz, 6H, (CH3)2CH), 1.27 (d, I: 6.84 Hz, 6H, (CH3)2CH), 1.30 (s, 3H, CH3), 1.36 (s, 3H, CH3), 1.8 (broad s, 1H, 0H), 2.8-3.0 (m, 2H, 2CH(CH3)2), 2.95, 2.99 (AB quartet, 1: 16 Hz, 2H, CH2), 6.88 (d, 1: 1.59 Hz, 1H, Ar), 6.95 (d, J= 1.59 Hz, 1H, Ar) ”C NMR(CDC1,); 5 19.9, 20.6, 22.6, 23.9, 26.1, 30.6, 33.9, 43.4, 49.4, 83.1, 117.8, 120.9, 133.6, 1442,1477, 150.6 IR(CC14): 3448, 2966, 2930, 1448.7, 1076, 802.4 1Ztl-Methyl-2-(2,4,6-triisopropylphenyl)ethenol lH NMR(C6D6): 5 1.1-1.3 (d, J: 6.84 Hz, 18H, 3 (CH3)2CH), 1.8 (s, 3H, allylic CH3), 2.7-3.0 (3H, septet, .1: 6.84 Hz, 3H, 3CH(CH3)2), 4.4 (broad s, 1H, OH), 5.2 (s, 1H, vinylic CH), 6.9 (s, 1H, Ar), 7.05 (s, 1H, Ar) L1l+ll AlAAIAPlLLLlAA Zl0 h Figure 44. 1H NMR of a-(2,4,6-Triisopropylphenyl)acetone after Irradiation in 213 ’ O O E r-o ‘ 1 11 1-0 g: I 1 t O r E + a O I l . g} + a I M Toluene (A > 290 nm, T= 297 K) 214 1,z-Dif2,4,6-triisopropylphenyl)ethane lH NMR(CDC13): 5 1.20 (d, J= 6.84 Hz, 24H, 4 (CH3)2CH), 1.24 (d, J=6.84 Hz, 12H, 2 (CH3)2CH), 2.90 (s, 4H, 2CH2), 3.25 (septet, J= 6.84 Hz, 6H, 6CH(CH3)2), 6.98 (s, 4H, Ar) Products from o-ten-Buo’ltrifluroacetophenone (14) o-tert-Butyltrifluroacetophenone (0.003 g) in 0.8 mL of deuterated benzene was irradiated until no trace of starting material could be observed by NMR. The signals for two products were detected upon analysis of the NMR spectrum of the photolysis mixture. The products were identified to be an unsaturated alcohol and an indanol. The product ratios were determined by NMR integration of the methyl singlet signal of the alcohol and indanol. Products were separated by performing large scale irradiation using 0.30 g of o-tert-Butyltrifluroacetophenone in 100 mL of benzene. Solvent was evaporated to leave a yellow oil which was chromatographed by PTLC using 30% ethyl acetate in hexane solution. The indanol eluted before the unsaturated alcohol. 14 Mind 14alc Scheme 75. Photoproducts of o-tert-Butyltrifluroacetophenone 215 1-{2’-(3-(2”-Methyl)propargyuphenylitriflouromethylethanol lH NMR(CDC1,): 5 1.8 (s, 3H, allylic CH3), 2.42 (d, J= 4.88 Hz, 1H, 0H), 3.40 (AB quartet, 1: 16.5 Hz, 2H, CH2), 4.5 (dq, J=1.4, 0.83 Hz, 1H, vinylic CH), 4.88 (dq, J=1.4, 1.5 Hz, 1H, vinylic CH), 5.3 (dq, J= 4.8, 6.7 Hz, 1H, CHOH), 7.2 (m, 1H, Ar), 7.35 (m, 2H, Ar), 7.65 (m, 1H, Ar) ”C NMR(CDC13): 5 22.3, 41.6, 69 (q, 1= 34 Hz), 112.5, 124.5 (q, J=290 Hz), 127, 127.4, 129, 131, 133, 138, 144.8 l9F NMR(CDC13): 5 -2.0 (d, J= 6.7 Hz, 3F, CF 3) reference: ethyl trifuroacetate IR(CC14): 3618.9, 2937.9, 1453.5, 1272.2, 1169.1, 1132.4, 1061.9, 898.9, 803.4, 701.2 3,_3_-Dimethyl-l-trifluromethyl-l-indanol lH NMR(CDC13): 5 1.37 (s, 3H, CH3), 1.42 (s, 3H, CH3), 2.20 (1H, q and half of an AB quartet, J=1.16, 14.4 Hz, 1H, CH2), 2.45 (half of an AB quartet, J= 14.2 Hz, 1H, CH2), 7.0 (m, 1H, Ar), 7.35 (m, 2H, Ar), 7.55 (d, 1H, Ar) Products from o-tert-Amylbenzophenone o-tert-Amylbenzophenone 0.4 g in 100 mL of benzene was irradiated until no trace of starting material could be observed by GC. The signals for two pairs of isomeric indanols were detected upon analysis of the NMR spectrum of the photolysis mixture. The products were separated by liquid chromatography using 5% ethyl acetate in hexane. NOe experiments were performed to determine the stereochemistry of the isomers. 216 Scheme 76. Photoproducts of o-tert-Amylbenzophenone E 2 -Trimeth l-l- hen l-l-indanol lH NMR(CDC13): 5 0.82 (d, J= 7.3 Hz, 3H, CH3CH), 0.89 (s, 3H, CH3), 1.36 (s, 3H, CH3), 2.41 (q. =7.3 Hz, 1H, CHCHs), 7.09 (m, 2H, Ar), 7.2-7.5 (m, 7H, Ar) Noe(CDC13): Irradiation at 5 0.82 ppm produced the following enhancements 5 1.36 ppm (2.5%), 5 2.4 ppm (2.5%), 5 7.2-7.5 ppm (3.8%) (Z)-2,3_,§-Trimethyl-l-phenyl-1-indanol IH NMR(CDC13): 5 1.01 (d, J= 7.3 Hz, 3H, CH,CH), 1.30 (s, 3H, CH3), 1.39 (s, 3H, CH3), 2.22 (q, J=7.3 Hz, 1H, CHCH3), 6.98 (d, 1H, Ar), 7.2-7.5 (m, 8H, Ar) Noe(CDC13): Irradiation at 5 1.01 ppm produced the following enhancements 5 2.22 ppm (4.5%), and 5 1.39 ppm (2.5%) (E)- 3-Met_1_1vl-3-e_tl_1yl-l-phenyl-l-indanol lH NMR(CDC13): 5 0.96 (t, J= 7.4 Hz, 3H, CH3CH2), 1.27 (s, 3H, CH3), 1.80 (q, J=7.4 Hz, 2H, CHZCH3), 2.29-2.56 (AB quartet, J= 14.1 Hz, 2H, CH2), 7.07 (d, 1H, Ar), 7.2-7.5 (m, 8H, Ar) 217 Noe(CDCl3): Irradiation at 5 1.27 ppm produced the following enhancements 5 1.80 ppm (1.7%), and 5 2.29 ppm (1.9%), and 5 7.07 ppm (2.9%) (Z)- 3-Methvl-3-ethyl-l-phenyl-1-indanol lH NMR(CDC13): 5 0.81 (t, J= 7.4 Hz, 3H, CH3CH2). 1.42 (s, 3H, CH3), 1.58-1.72 (m, 2H), 2.26-2.45 (AB quartet, J= 14.1 Hz, 2H, CH2), 7.01 (d, 1H, Ar), 7.2-7.5 (m, 8H, Ar) Noe(CDC13): Irradiation at 5 1.42 ppm produced the following enhancements 5 2.26 ppm (0.8%), and 5 2.56 ppm (0.9%), and 5 7.0 ppm (0.8%). Products from 2 '-(2,3-Dirnethyl-2-butyl)benzophenone (I 5) 2'-(2,3-Dimethyl-2-buty1)benzophenone (0.004 g) in 0.8 mL of deuterated benzene was irradiated until no trace of starting material could be observed by NMR. The signals for four isomeric products were detected upon analysis of the NMR spectrum of the photolysis mixture. The products were identified as indanols and an unsaturated alcohol. The product ratios were determined by NMR integration of the methyl singlet signals of indanols and the isopropyl doublet signal of the alcohol. The effect of temperature and phase on product ratios was also investigated by conducting the photochemistry in acetone/ethanol, ice-water and silicon oil (110°C) baths and in solid. The products were difficult to isolate because of a rapid dehydration on silica gel. The spectroscopic data given are from the NMR mixtures of photoproducts in benzene. 218 15 lSindmZ lSinde 15alc Scheme 77. Photoproducts of 2-(2'-(2',3'-Dimethyl)butyl)benzophenone Z-3-lsopropyl-3-methyl-lphenyl-1-indanol 1H NMR(C6D6): 5 0.62 (d, .1: 6.84 Hz, 3H, (CH3)2CH), 0.78 (d, J= 6.84 Hz, 3H, (CH3)2CH), 1.40 (s, 3H, CH3), 1.91 (septet, J= 6.8 Hz, 1H, CH(CH3)2), 2.05 (Half of an AB quartet, J= 14.1 Hz, 1H, CH2), 2.38 (Half of an AB quartet, J= 14.1 Hz, 1H, CH2), 6.8-7.2 (m, 7H, Ar), 7.5 (d, J=6.9 Hz, 2H, Ar) E-3-lsopropyl-3-methyl-lphenyl-1-indanol 1H NMR(C,D,): 5 0.76 (d, J: 6.81 Hz, 3H, (CH3)2CH), 0.85 (d, I: 6.78 Hz, 3H, (CI-13)2CH), 1.10 (s, 3H, CH3), 1.91 (septet, J: 6.8 Hz, 1H, CH(CH3)2), 2.08 (Half of an AB quartet, J= 14.5 Hz, 1H, CH2), 2.58 (Half of an AB quartet, J= 14.5 Hz, 1H, CH2), 6.8-7.2 (m, 7H, Ar), 7.4 (d, J=6.9 Hz, 2H, Ar) 219 3,3,4,4-tetramethyl-lphenyl-1-indanol lH NMR(C6D6): 5 1.11 (s, 3H, CH3). 1.16 (s, 3H, CH3). 1.18 (s, 3H, CH3). 1.45 (s, 3H, CH3), 6.8-7.3 (m, 9H, Ar) 1- 2’- 3- 2”-Iso r0 1 r0 a l hen lbe lalcohol IH NMR(C6D6): 5 0.92 (d, J= 6.96 Hz, 3H, (CH3)2CH), 0.95 (d, J= 6.85 Hz, 3H, (CH3)2CH), 1.91 (septet, J= 6.8 Hz, 1H, CH(CH3)2), 3.26 (Collapsed AB quartet, J= 1.14 Hz, 2H, CH2), 4.47 (dd, J=1.53 Hz, 1H, vinylic CH), 4.84 (m, 1H, vinylic CH), 5.92 (s, 1H, CHOH), 6.8—7.2 (m, 7H, Ar), 7.4 (d, J=6.9 Hz, 2H, Ar) 3-Iso ro l-3-meth l-l- hen lindene lH NMR(C6D6): 5 0.64 (d, J= 6.75 Hz, 3H, (CH3)2CH), 0.94 (d, J= 6.81 Hz, 3H, (CH3)2CH), 1.25 (s, 3H, CH3). 1.97 (septet, J= 6.8 Hz, 1H, CH(CH3)2), 6.22 (s, 1H, vinylic CH), 7.15-7.30 (m, 6H, Ar), 7.5 (m, 1H, Ar), 7.5 (d, J=6.8 Hz, 2H, Ar) D. Quantitative Measurements I. Semiempirical and Molecular Mechanics Calculations All calculations were performed on a 7100/80 Power Macintosh computer equiped with the Cache program. MOPAC, a version of MOPAC6 written by James J. P. Stewartl '2 , was used for semiempirical calculations. The calculations were generally done by creating a structural input which was minimized first by molecuar mechanics and then by semiempirical calculations at AMI level of theory. The purpose of this. procedure was to provide MOPAC with a better input structure. 220 Global minimizations (semiempirical-AMI) with dihedral drivers around bonds a and b were performed on the minimized structures to obtain the conformations of other minima. R2 a R1= Me, Et, i-Pr, CHzPh R2=H, Me, Et, i-Pr R3: H, MC R4: Ph, Me Figure 45 For R1=Et and CHzPh only conformations with the methyl and phenyl trans to the hemipinacol radical moiety were considered, since the syn isomer was found to lie 4 kcal/mole above the trans. The lowest energy rotational maps for interconversion of various minima were constructed by locating the lowest energy path between the minima in the global minimization maps, minimizing the geometries in the path (semiempirical- AMI) and plotting the energies. The details of global minimizations for all compounds studied are listed in Tables 28 and 29. Tables 30-38 contain energies from double dihedral minimizations about bonds a and b (Figure 45), calculated by MOPAC, for several compounds. Table 28. Details of Global Minimizations for Compounds 1-9 221 Compound State Calculation Level # of Increments Key Drivers' Words° 1 Ground Semiempirical AM] 2 36°, 36° NOANCI GEO-OK l Triplet Br. Semiempirical AMI-UHF 2 10°, 10° // 2 Ground Mechanics MM2 2 36°, 36° // 2 Triplet Br. Semiempirical AMl-UHF 2 20°, 20° // 3 Triplet Br. Semiempirical AMl-UHF 2 24°, 24° // 4 Ground Semiempirical AMl 2 10°, 10° // 4 Triplet Br. Semiempirical AMI-UHF 2 36°, 36° // 5 Ground Semiempirical AM] 2 15°, 15° // 5 Triplet Br. Semiempirical AMl-UHF 2 30°, 30° // 6 Ground Semiempirical AM] 2 36°, 36° // 6 Triplet Br. Semiempirical AMl-UHF 2 15°, 15° // 7 Ground Mechanics MM2 2 36°, 36° // 8 Ground Semiempirical AM] 2 36°, 10° // 8 Triplet Br. Semiempirical AMl-UHF 2 22°, 22° // 9 Triplet Br. Semiempirical AMI-UHF 2 15°, 15° // a) Dihedral rotations about bonds a and b, respectively. b) NOANCI= no analytical configuration interaction was used, GEO-OK= will allow the calculation to continue if a high energy (non convergent) geometry is reached. 222 Table 29. Details of Global Minimizations for Compounds 10-15 Compound State Calculation Level # of Drivers' Increments Key Words° 10 Ground Semiempirical AM] 2 16°, 16° NOANCl GEO-OK 10 Triplet Br. Semiempirical AMl-UHF 2 30°, 30° // 11 Ground Mechanics MM2 2 36°, 36° // 12 Ground Mechanics MM2 2 36°, 36° // 12 Triplet Br. Semiempirical AMl-UHF 2 36°, 36° // 13 Triplet Br. Semiempirical AMI-UHF 2 15°, 30° // 14 Ground Mechanics MM2 1 10° // 1 1 5 Ground Semiempirical AM 1 -UHF 1 36° // a) Dihedral rotations about bonds a and b, respectively. b) NOANCI= no analytical configuration interaction was used, GEO-OK= will allow the calculation to continue if a high energy (non convergent) geometry is reached. 223 Table 30. Grid of Energies (Real/mole) for The Ground State Optimization of or-(2- Ethylphenyl)acetophenone N“ 0° 36° 72° 108° 144° 180° 216° 252° 288° 324° 360° 1 0° 2.79 3.32 2.66 3.36 6.01 6.9 5.4 2.54 2.35 2.67 1.75 36° 1.4 2.04 2.03 1.13 4.4 7.31 6.48 2.14 1.62 2.71 1.44 72° 2.94 3.89 2.9 2.76 6.74 8.94 8.37 4.98 3.02 2.69 2.20 108° 2.53 2.88 2.44 3.03 6.27 8.08 7.39 4.59 2.51 2.88 2.52 144° 5.67 4.81 5.53 5.74 8 12.62 14.38 8.78 4.77 6.31 5.66 180° 5.56 6.94 6.98 8.22 12.83 17.55 12.32 6.71 6.53 7.13 6.84 216° 3.66 5.11 3.92 6.89 14.47 12.13 7.84 3.88 4.45 3.84 3.67 252° 1.89 2.13 2.07 5.14 7.53 8.53 5.74 2.49 1.65 2.31 1.90 288° 2.44 2.94 3.11 2.09 5.86 7.94 7.1 2.58 2.53 3.61 2.45 324° 3.02 4.18 4.24 3.87 7.54 8.76 5.88 2.8 3.62 3.56 3.03 360° 3.02 3.07 1.91 2.63 5.26 6.9 5.38 2.56 1.89 2.33 1.75 AMI NOMM MULLIK BONDS NOINTER PRECISE DENOUT ISOTOPE NODIIS NOANCI GEO-OK, oetpapsm, Optimized search (grid) TOTAL CPU TIME IN FLEPO : 89056.987 224 Table 31. Grid of Energies (Real/mole) for Global Minimization of The Triplet Biradical of or-(2,4,6-Triethy1phenyl)acetophenone N__. 0° 30° 60° 90° 120° 150° 180° 210° 240° 270° 300° 330° 360° 1 0° 19.35 13.7 10.98 12.1 18.43 28.69 29.16 20.17 13.5 10.73 12.44 17.36 24.72 30° 9.71 8.18 8.85 13.37 22.22 22.28 17.12 12.42 9.5 10.64 18.93 14.3 9.83 60° 5.95 ' 6.25 7.17 11.83 17.83 13.64 11.14 9.41 8.67 10.31 15.08 7.47 5.94 90° 5.42 5.35 6.25 12.63 10.1 1 9.71 10.08 13.78 12.86 10.67 5.9 5.22 5.25 120° 6.78 9.35 1 1.63 1 1.27 8.1 9.77 12.76 16.92 20.25 20.17 17.62 6.65 6.61 150° 11.79 16.94 17.49 11.35 10.37 13.99 33.52 28.03 19.34 14.37 9.64 9.06 11.65 180° 18.1 23.15 13.47 11.19 12.81 18.77 25.72 29.84 12.87 11.46 12.01 15.31 20.21 210° 13.96 11.51 11.12 13.92 20.14 22.81 17.71 12.12 8.71 10.96 14.64 21.14 24.37 240° 9.91 8.89 8.71 11.33 15.96 15.22 1 1.64 8.43 7.73 9.34 l 1.89 12.24 9.79! 270° 8.25 8.25 9.69 11.59 1 1.24 10.84 9.72 9.69 10.54 9.43 9.31 8.7 8.21 300° 9.06 11.17 10.89 8.26 7.81 8.57 10.6 12.77 15.75 17.81 9.5 9.3 9.43 330° 12.4 16.22 13.6 9.34 8.53 11.09 17.25 22.35 22.37 14.98 11.32 11.32 13.6 360° 17.84 19.76 13.49 9.76 1 1.32 16.75 24.15 29.94 16.23 11.89 11.82 13.97 17.86 UHF TRIPLET AMI NOMM MULLIK BONDS NOINTER DENOUT ISOTOPE NOANCI, GEO-OK, tetpap.br, Optimized search (grid), TOTAL CPU TIME IN FLEPO : 63458.344 225 Table 32. Grid of Energies (kcal/mole) for Global Minimization of The Triplet Biradical of a-(Z-Tolyl)propiopbenone IN 00 240 48° 72° 96° 120° 144° 168° 192° 216° 240° 264° 288° 312° 336° 360° 00 35115 41.78 331 32111 1252 29113 32313 21153 4128 34111 2911 22124 2R158 27219 21182 35111 24° .1287 31:48 30111 281N3 271" 29127 36117 21187 21196 2815 2R556 25141 2513 2715 3012 21183 430 32121 31.52 3017’ 28112 21154 29117 21222 38J6» 1586 22176 26(17 251" 2613 22176 28317 28155 72° 33111 .3188 21158 21108 31.16 .3108 21145 30113 23109 301" 281MB 26115 26151 271Mi 22187 28155 96° .1246 32115 3126 21185 27117 2154 2813 30317 32115 32315 3135 29115 27.17 273” 22175 2866 120° 21186 352” 21108 21193 2132 26115 22108 29113 1257 38117 21565 31.83 281MB 28112 28312 29117 1440 21163 38131 14188 34121 29113 28314 30121 34111 38115 4333 4M183 1556 31.72 21153 3133 3313 168° 46111 413” 21103 21168 31.56 321KB 35112 15109 41196 4217 36117 .1286 23167 32131 34131 39' 192° 21167 36114 21184 1256 32315 3554 21165 451” 50113 1167 23163 21132 32127 34(75 38123 4285' 216° 32117 .1288 32117 333” .1176 14184 21165 2H578 331” 29315 28 22198 3013 3415 1179 .1249 2400 29315 311" 3142 31.93 3234 35 37327 38111 363N5 273” 2638 2126 281”! 21155 21139 291” 264° 34313 3312 3124 3139 21153 333” 21278 341” 3213 32117 3011 29113 2815 29113 21108 30327 288° 36111 21559 21155 32117 3131 31.76 33111 1144 21183 1178 3513 21587 21182 23162 .3198 3312 312° 39111 21158 21143 33373 .3147 31.33 21253 3415 3613 21186 36113 21142 .1249 21123 21168 1526 336° 43377 43113 4311 21187 21158 21176 .1256 36117 4N156 11142 35117 3233 311” 3196 1292 36m39 360° 21109 34m43 321M 3033 2848 29L"? 3151 21585 361%) 1258 291 28Jéi 28J€i 28113 31.78 3532 UHF TRIPLET AMI NOMM MULLIK BONDS NOINTER DENOUT ISOTOPE NOANCI, GEO-OK, otolpp.br, Optimized search (grid), TOTAL CPU TIME IN FLEPO : 53680.500 226 Table 33. Grid of Energies (Real/mole) for Global Minimization of The Triplet Biradical of a-(2-Ethylphenyl)propiophenone Kfi 0° 360 720 108° 144° 180° 216° 252° 2880 3240 3600 1 0° 29.23 24.02 22.74 22.91 22.9 30 24.43 18.35 16.62 18.91 29.31 36° 22.62 19.57 18.66 19.71 26.35 22.82 19.03 15.9 16.47 23.63 19.72 72° 17.76 19.89 20.7 20.66 23.09 23.23 21.64 18.23 17.44 16.64 17.23 1080 21.99 23.81 22.06 18.43 18.17 26.78 28.39 23.73 17.11 15.40 16.89 144° 22.02 34.78 28.83 20.61 21.52 28.37 38.29 29.64 20.56 18.33 22.0 180° 34.28 25.93 23.64 23.57 29.3 38.89 30.55 22.21 20.89 22.37 32.54 216° 23.73 21.27 22.75 28.39 36.5 27.13 21.05 18.2 23.85 27.95 21.35 252° 21.29 20.32 27.03 27.97 24.99 21.83 19.72 17.94 20.28 18.60 17.71 288° 24.82 26.59 25.15 24.31 23.42 24.66 26.58 28.43 20.28 19.44 21.34 324° 32.69 37.11 27.14 23.57 25.02 29.32 35.17 26.89 22.66 22.01 26.24 360° 29.24 24.07 22.94 22.92 23.03 29.91 24.34 18.71 16.72 18.8 29.4 UHF TRIPLET AMI NOMM MULLIK BONDS NOINTER DENOUT ISOTOPE NOANCI, GEO-OK, oethylphenpph.br2, Optimized search (grid), TOTAL CPU TIME IN FLEPO : 34510.688 227 Table 34. Grid of Energies (Real/mole) for Global Minimization of The Triplet Biradical of a-(2,4,6-Trietbylpbeny1)propiopbenone Y__ 00 300 60° 900 1200 150° 180° 2100 2400 2700 3000 330° 360° 1 0° 22.31 34.49 17.39 15.23 17.41 23.88 32.96 28.28 18.88 13.67 13.44 17.5 24.33 30° 13.7 13.67 13.65 15.52 20.05 22.05 16.78 11.52 7.91 9.9 15.27 23.57 20.28 60° 11.35 12.57 13.04 14.36 17.88 20.4 12.29 9.33 7.75 8.92 12.48 12.02 10.83 90° 15.11 15.47 16.09 14.46 12.75 12.76 13.9 15.35 14.39 11.69 10.92 10.62 12.19 1200 21.68 24.25 20.57 15.36 13.62 14.05 17.98 22.58 25.76 25.67 15.22 15.2 17.14 150° 21.17 29.54 23.32 16.91 14.93 17.75 24.47 33.96 28.58 21.09 17.02 17.18 21.31 1800 22.84 28.75 22.13 20.13 15.41 21.41 28.32 33.84 24.95 17.01 15.21 17.74 22.92 210° 13.49 13.21 13.42 15.25 18.8 21 16.48 11.19 7.74 8.44 14.43 19.57 25.45 240° 9.95 11.34 11.37 12.23 15.83 18.2 18.03 9.01 7.37 9.24 13.3 11.41 9.84 270° 11.68 15.08 15.4 13.91 12.82 12.38 12.78 15.82 14.45 12.2 11.85 10.67 11.15 300° 15.04 19.72 20.27 19.21 12.91 13.07 16.12 19.97 24.2 17.87 13.9 13.91 15.12 330° 24.02 32.09 24.36 18.78 16.91 20.3 26.98 38.33 29.45 22.87 19.94 20.11 24.21 360° 36.07 21.86 19.75 17.28 15.51 21.38 29.84 24.63 17.14 12.63 12.82 16.36 22.91 UHF TRIPLET AMI NOMM MULLIK BONDS NOINTER DENOUT ISOTOPE GEO-OK, tetpph.br, Optimized search (grid), TOTAL CPU TIME IN FLEPO : 74793.797 228 Table 35. Grid of Energies (Real/mole) for Global Minimization of The Triplet Biradical of a-Mesitylpropiopbenone N 00 240 48° 720 960 1200 1680 1920 2160 2400 2640 2880 3120 336° 360o 00 2587 25527 2129 2937 1163 1935 35512 325%? 22195 24517 222M 235¥1 25357 2N129 36Jh1 2196 240 26557 22123 28514 29312 3181 32J13 2937 2151 22196 22185 22J4 21196 25u15 273” 26553 21595 48° 2N585 26517 21J7 275? 295%5 275" 26314 25313 255KB 24J1 23527 24527 25378 25337 24591 22189 72o 2H119 21189 29317 2137 26 265” 22153 295KB 305“ 2E182 285“ 25354 24521 2141 255M! 2N528 960 35J3 33.18 2M148 27J8 26524 26324 285KB IN172 21167 36J6> 21105 2N159 22198 22125 2737 29553 120O lH155 21119 32513 295y1 285¥1 28JM5 3L8 2M526 4“178 14185 21164 1122 2M138 295M 2fl184 33J4 1440 11183 3835 21185 2N188 28314 2N133 21183 l“106 11194 44577 383%? 1128 2M176 3052 3171 36J5 1680 1157 3L27 295%? 28314 3138 413” 43J 2%198 3538 2M164 2179 22165 22198 293KB 33.17 2fl155 1920 28557 2136 28J 29J7’ 32557 2M528 4132 41566 2737 24¢33 2131 22108 27J6 3036 3129 291x) 2160 2652 26JMS 265”! 28J9 1125 3L82 2931 2639 216 2L36 2L03 2121 2451 27 2597 25J 2400 2554 2592 SM528 2M582 2956 3114 3L77 2N165 2156 21105 2236 2353 2523 2503 25J1 2133 2640 28317 29AMZ 22198 22144 2126 22105 2123 27J2 28A”? 2933 265%? 24313 22162 2142 2189 2559 288° 21163 3216 29Jt3 275¥1 26J9 27x1 295IZ 3144 3103 21172 21592 29313 22125 2630 2123 285M5 312O 4L45 38J2 1193 2859 275? 2856 3L4 3527 395“ 45315 3933 1109 3L63 295MB 2M138 32315 3360 4539 40J2 1578 .1187 21167 1191 21184 46J 52313 45J7 3133 3172 2959 295%? 3146 3554 360° 3432 3038 22196 2139 21162 1199 383K! 1591 21163 33.11 2836 21585 265K! 28J1 21108 365M UHF TRIPLET AMI NOMM MULLIK BONDS NOINTER DENOUT ISOTOPE NOANCI GEO-OK, mespph.br, Optimized search (grid), TOTAL CPU TIME IN FLEPO : 70180.500 229 Table 36.Grid of Energies (Real/mole) for Global Minimization of The Triplet Biradical of a-(2-Ethy1pheny1)acetone N 00 300 60° 900 1200 150° 1800 2100 2400 2700 3000 330° 360° 1 00 -6.08 -9.62 40.68 41.47 41.43 -7.72 4.06 5.84 41.51 41.49 40.69 -9.66 -6.09 300 40.49 41.37 40.9 41.99 2.82 4.28 -5.97 -9.65 -11.63 41.73 -9.89 .654 -IO.61 60° 42 41.49 40.83 -11.76 -7.98 .051 4.49 -8.89 40.8 41.5 -9.08 40.15 42.08 900 -ll.46 40.67 40.19 40.86 -8.87 -7.8 -723 .497 -944 40.95 .991 41.14 -11.86 1200 40.4 -8.42 -947 40.66 40.6 -8.57 .557 -0.45 -7.86 40.34 -9.89 -10.61 40.4 1500 -7.52 -6.49 -9.21 40.36 40.03 -6.88 4.96 -0.84 -8.12 40.3 -9.41 -9.52 -7.49 1800 -6.03 -771 -9.36 40.39 -9.46 -3.79 3.55 6.95 .921 40.33 -941 -773 ~6.05 2100 .749 -954 -97 40.17 -8.16 5.25 -0.6 -6.95 40.46 40.36 -8.98 -6.6 .753 2400 40.52 40.48 -9.87 40.45 -7.86 4.56 1.63 -8.59 40.47 40.44 -93 -8.44 40.52 2700 41.8 41 40.22 40.92 -9.04 -5.86 .727 -754 -8.77 40.77 -9.66 40.64 -11.61 3000 41.99 40.19 -9.16 -ll.67 40.83 -8.93 .753 -5.62 -3.62 41.75 40.78 41.45 42.04 3300 -919 -8.02 -8.73 -912 -9.03 -6.57 -307 -2.99 40.13 41.93 40.69 41.52 40.6 360° -7.28 -7.96 ~8.26 -8.8 -8.23 -4.56 0.81 4.79 -8.25 -8.66 -8.18 -8.14 -6.92 UHF TRIPLET AMI NOMM MULLIK BONDS NOINTER DENOUT ISOTOPE NOANCI GEO-OK, oetphacetone.br2, Optimized search (grid), TOTAL CPU TIME IN FLEPO : 17316.492 230 Table 37. Grid of Energies (kcal/mole) for Global Minimization of The Singlet Biradical of a-(2-Ethylphenyl)acetone N 30° 120° 150° 180° 210° 240° 270° 300o 330° 360° 00 84.75 80.21 74.28 69.84 69.59 83.53 51.6 56.39 74.57 100.04 143.77 123.75 130.76 30° 83.73 92.96 109.3 107.29 108.21 96.28 113.29 86.86 77.56 78.54 87.65 111.12 107.14 60° 84.84 82.12 77.17 83.49 97.35 127.45 105.15 99.79 94.44 91.99 85.78 88.07 84.53 90° 87.05 85.14 80.65 77.18 75.48 83.91 87.53 87.86 97.67 97.43 85.36 87.8 86.3 120° 87.56 89.01 85.75 80.54 81.42 78.39 89.63 99.53 110.11 1 12.63 102.11 93.76 88.37 1500 96.63 94.05 84.07 89.93 102.76 108.62 105.88 147.2 121.69 88.6 86.18 89.06 95.13 1 80° 95.34 92.36 86.14 79.26 85.8 99.38 107.6 123.11 133.15 119.12 94.12 93.93 93.32 2100 105.77 95.69 94 104.8 115.46 118.36 92.43 102.12 79.9 81.16 86.16 87.91 95.35 240° 88.58 88.05 86.28 90.04 84.66 113.9 140.77 96.78 90.46 90.92 84.59 90.04 87.51 270° 92.73 94.96 99.74 99.58 91.79 82.07 84.8 80.67 70.65 74.12 81.95 84.65 84.93 3000 97.15 96.1 89.73 90.5 92.73 93.01 94.19 80.51 71.51 78 82.75 83.55 88.73 330° 96.13 97.2 88.89 89.17 104.09 148.62 129.76 96.37 71.62 75.57 78.77 81.82 88.06 360° 94.8 87.56 81.07 77.98 89.53 109.86 94.75 84.2 77.14 77.29 80.06 93.46 109.97 EXCITED SINGLET AMI NOMM MULLIK BONDS NOINTER DENOUT NOANCI GEO-OK, oetphacetonebr, Optimized search (grid), TOTAL CPU TIME IN FLEPO : 54177.381 231 Table 38. Grid of Energies (Real/mole) for Global Minimization of The Triplet Biradical of a-(2,4,6-Triisopropylphenyl)acetone by 0° 30° 60° 90° 120° 1 50° 1 80° 2 1 0° 240° 270° 300° 3 30° 360° 1 ~900 ~25.42 ~27.17 ~27.2 ~24.75 ~20.51 ~19.57 ~26.96 ~28.86 ~28.33 ~26.21 ~2 I .45 ~22.32 ~25.22 ~60° ~26.82 ~27.68 ~27.84 ~24.19 ~24.59 ~27 ~28.55 ~29.28 ~28.8 ~26.97 ~23.43 ~24.52 ~26.97 ~30° ~27.34 ~27.62 ~27.57 ~26.95 ~26. 18 ~28.51 ~28.75 ~28.97 ~28.33 ~27.38 ~25.93 ~26.46 ~27.25 0° ~26.66 ~27.09 ~26.92 ~27.34 ~27.69 ~28.52 ~28. 17 ~28.68 ~28.84 ~27.73 ~27.09 ~26.69 ~26.95 30° ~26.49 ~26.15 ~25.97 ~26.91 ~27.68 ~27.9 -27.53 ~27.99 ~27.71 ~27.97 ~26.84 ~26.52 ~26.46 60° ~26.01 ~23.61 ~23.88 ~25.68 ~26.28 ~27.1 ~26.99 ~26.19 ~24.66 ~25.46 ~25.46 ~26.34 ~25.88 90° ~24.42 ~22.26 ~20.07 ~23.49 ~25.14 ~26.37 ~25.47 ~23.46 ~22.09 ~22.57 ~24.26 ~25.46 ~24.29 UHF TRIPLET AMI RESTART NOMM MU LLIK BONDS NOINTER DENOUT NOANCI GEO-OK, tippacetone.br, Optimized search (grid), TOTAL CPU TIME IN FLEPO : 81761.70] 2. Quantum Yield Measurements Quantum yields for product formation were measured by irradiating solutions of desired precursor parallel to 0.1 M valerophenone samples in sealed, degassed tubes. Quantum yields were calculated from the following equation, .,,,,,,. "" 313 6 0.0065 0.35 - - 313 15 0.013 0.234 0.003 0.062 313 19 0.014 0.15 0.006 0.059 313 24 0.014 0.09 0.009 0.052 366 10 0.13 0.64 ' - - 366 18 0.18 0.64 0.024 0.085 366 25 0.24 0.64 0.034 0.085 a) Quantum yields were measured by NMR (b) Quantum yields were measured by GC [Ketone]= 0.0143 M (GC studies), [Ketone]= 0.0983 M (NMR studies) [VP]= 0.024 M (GC studies), [VP]= 0.1165 M (NMR studies) [C20]= 0.0033 M (GC studies), [Methyl benzoate]= 0.03 M (NMR studies) Rfl"°'“°'=1 .12, RfAP =1 .34, Irradiation Time=4 hrs, Irradiation Source= Mercury Arc 243 Quantum Yield Measurement for ajZ-Bengylphenyl[propiophenone in Benzene NMR analysis: Gemini 300 MHz Table 48. Product Quantum Yields of a-(Z-Benzylphenyl)propiophenone in Benzene Photoproduct A(product) A(std.) Concentration (D Z,Z~Indanol 0.57 1 1.05 0.0033 0.052 Z,Z~Indanol 0.51 9.36 0.0034 0.053 Z,Z~Indanol 0.54 9.34 0.0036 0.056 Z,E-Indanol 0.54 1 1.05 0.0031 0.049 Z,E-Indanol 0.42 9.36 0.0029 0.045 Z,E-Indanol 0.42 9.34 0.0029 0.045 [Ketone]= 0.0113 M, [VP]= 0.166 M, [Methyl benzoate]= 0.064 M Irradiation Time=8 hrs, l=313 nm Irradiation Source= Mercury Arc Lamp 244 Quantum Yield Measurement for 01:] 2,4,6-Triisopropylphenyl[acetone in Benzene GC analysis: 1400 Varian GC DB~225 Megabore column Initial column temp.: 100°C Initial col. hold time: 5 min. Final col. temp.: 185°C Rate: 8 oC/min., Hold time: 5 min. Table 49. Product Quantum Yields of a—(2,4,6~Triisopropylphenyl)acetone in Benzene Photoproduct A(product) A(std.) Concentration CD Indanol 2.69067 66.80157 0.0002 0.009 Indanol 2.64648 66.75248 0.0002 0.009 Indanol 2.68319 66.19910 0.0002 0.009 Diarylethane 2.03309 66.80157 0.00009 0.004 Diarylethane 1.85067 66.75248 0.00008 0.004 Diarylethane 2.06752 66.19910 0.00009 0.004. Enol 0.15 22.5 0.0036 0.028 Enol 0.18 231 0.0042 0.032 Enol 0.15 22.3 0.0036 0.028 [Ketone] = 0.0245 m, [VP]= 0.03 M, [C20]= 0.0035 M R,"‘“‘“°"=1 .0, sz'3'D‘W'°"""°‘=0.62, R,“’=2.9, Irradiation Time=20 hrs, 2:313 nm Irradiation Source= Mercury Arc Lamp 245 Quantum Yield Measurements for 2j2’j2’éhDimethyllbutyl[benzophenone NMR analysis: Gemini 300 MHz Table 50. Product Quantum Yields of 2-(2’~(2’,3’~Dimethyl)butyl))benzophenone Solvent Photoproduct A(product) A(std.) Concentration (D Benzene 151ndmZ 0.98 17.84 0.0021 0.026 Benzene 15indmZ 1.19 18.54 0.0024 0.028 Benzene 15inde 2.17 17.84 0.0046 0.052 Benzene 15inde 2.20 18.54 0.0045 0.052 Benzene 15indip 0.47 17.84 0.0010 0.01 Benzene 15indip 0.35 18.54 0.0008 0.009 Benzene 15alc 0.28 17.84 0.0006 0.006 Benzene 15alc 0.24 18.54 0.0005 0.005 Methanol 151ndmZ 3.26 12.3 0.0037 0.116 Methanol lSinde 3 .72 12.3 0.0042 0.132 Methanol 15indip 2.98 12.3 0.0034 0.107 Methanol 15alc 1.65 12.3 0.0019 0.06 [Ketone]= 0.0145 M, [VP]= 0.131 M, [MB]= 0.04 M Irradiation Time=8 hrs, 7t=313 nm, Irradiation Source= Mercury Arc Lamp 246 Table 51. Quenching of the Indanol Formation in a-(Z-Ethylphenyl)acetophenone with 2,5-Dimethyl-2,4~hexadiene at 313 nm in Benzene [Q] A(product)/A(std.) <1>°/ 0.00 0.145 1.00 0.0046 0.138 1.05 0.0092 0.135 1.07 0.0138 0.131 1.11 0.0184 0.127 1.14 [Ketone] = 0.032 M Table 52. Quenching of the Indanol Formation in a-(2,4,6-Triethylphenyl) acetophenone with 2,5-Dimethyl-2,4~hexadiene at 313 nm in Benzene [Q] A(product)/A(std.) °/ 0.00 0.056 1.00 0.00978 0.0422 1.32 0.0195 0.0393 1.42 0.0293 0.035 1.60 0.0391 0.034 1.7 [Ketone] = 0.064 M kq‘t = 17.4 248 Table 55. Quenching of the Indanol Formation in a-(2,4,6-Triethylphenyl) propiophenone with 2,5-Dimethyl-2,4~hexadiene at 313 nm in Benzene [Q] A(product)/A(std.) °/°/<1> 0.00 0.333 1 .00 0.0046 0.318 1.05 0.0092 0.315 1.06 0.0138 0.302 1.10 [Ketone] = 0.0075 M kqt = 6.7 Table 58. Quenching of the Diarylethane Formation in a-Mesitylacetone with 2,5- Dimethyl~2,4-hexadiene at 313 nm in Benzene [Q] A(product)/A(std.) 0.00 0.586 1 .00 0.0046 0.517 1.133 0.0092 0.4795 1 .222 0.0138 0.4035 1.452 [Ketone] = 0.0312 M kqt=31.4 250 Table 59. Quenching of the Diarylethane Formation in a-(2,4,6~Trisiopropylphenyl) acetone with 2,5-Dimethyl-2,4~hexadiene at 313 nm in Benzene [Q] A(product)/A(std.) 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