. PART I. THE EFFECT OF HYDROGEN AND. HEL-IUM ON PLAIN CARBON STEBL’_ ' ' PART; 11 ‘ sous PHYSICAL PROPERTIES. or . "CARBURIZED - mans , . Thai; for the Degree gf-M.‘ S. MlCHIGAN STATE COLLEGE Eldon H. Shotwell - 179.41 V V . n .' ¢ 1 5 | a ‘ J -.-‘-LA PART I THE EFFECT OF HYDROGEN AND HELIUM ON PLAIN CARBON STEEL PART II S ME PHYSICAL PROPERTIES OF CARBURIZED STEELS By ELDON HQ SHOTWELL .- ' 1:: a! KYiflM“ A THESIS Submitted to the Graduate School of Michigan State College of Agriculture and Applied Science in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE Department of Chemical Engineering 1941 q- ’\ up“ '5 '3 H A C K N O W L.E D G M E N T S The author wishes to express his gratitude for the cooperation and guidance received from the late Professor H. E. Publow. He also wishes to express his thanks to Professor R. L. Sweet under whose guidance the work was continued. The assistance in X—Ray analysis, giVbn by Professor J. C. Clark of the Physics Department, is greatly appre- ciated. 5-32666 I. II. III. IV. I. II. III. IV. T A B L E O F C O N T E N T S Part I Introduction Experimental Work and Results Conclusions Bibliography Part II Introduction Experimental Work and Results Conclusions Bibliography Page 22 25 Part I The Effect of Hydrogen and Helium on Plain Carbon Steel -1- INTRODUCTION The primary purpose of this experiment was to design and construct an electric furnace capable of heat-treating metals under controlled conditions of atmosphere. Plain carbon steel was to be the subject of study, using atmospheres of helium and hydrogen. Particular attention was to be paid to the macroscopic appearance of the surface scale and the microscopic appearance of the heat—treated specimens. At the outset it was hOped that an atmOSphere could be ob- tained which would be inert to the metallic surfaces. This, however, proved to be an impossibility with the experimental methods used. Pos- sible causes for this failure will be discussed later. "Bright annealing" is a term used in industry for annealing in relatively inert gases. However, it should be noted here that most of the successful "bright annealing" is at present carried on with metals or alloys whose recrystallization temperatures are in a relatively low range. Metals and alloys, such as aluminum, copper, brass, etc., are annealed at temperatures usually not exceeding llOOOF. and are fairly aptable to a "bright annealing" treatment. Steel, however, recrystal— lizes at temperatures ranging from 15400F. to 1650°F., thereby present- ing a more difficult problem. ‘The only advantage seen in "bright an- nealing" steel or ferrous alloys at the present time is to reduce the scale formation to a minimum and thereby shorten the pickling, sanding, or cleaning operation. It might also be pointed out at this time that metals having heavy cross-sections would require prolonged time for an- nealing, thus introducing a problem of greater scope in the so-called "bright annealing" process. In this problem a time of five hours was _ 2 - selected and a temperature of l700°F., which is well above the recrys- tallization range of all hypo-eutectoid steels. The samples were all placed in the furnace before the temperature was raised, and were re- moved from the furnace at room temperature. EXPERIMENTAL WORK AND RESULTS The first problem to be confronted was the construction of the furnace. It was desired to have a furnace that would heat to a max- imum temperature of lBOOOF. in one hour. Actual tests proved that the furnace would heat to l700°F. in one hour. It was decided to construct a simple electric resistance furnace using Chromel "A” wire for the heating element. The wire was “close wound" on to the center section of a silica furnace tube. The winding was about 10 inches in overall length. Asbestos sheet was wrapped around the tube between the winding and the furnace tube. Silica was chosen for the furnace tube because of its high refractory properties and its relative imperviousness to gases, as compared to other refrac- tory materials. A round tube was chosen having an inside diameter of 1-7/8 inches, a length of 24 inches, and a wall thickness of 5/16 inch. The tube was open at both ends for purposes of adapting fittings for control purposes. The furnace tube and winding were supported between two asbestos board supports. The furnace body or frame was a cylindri- cal sheet steel cylinder 10 inches in diameter and 10 inches long. The body, which was packed with asbestos and fire brick insulation material, was supported between the two upright asbestos board ends. The des- cription of the furnace may be clarified by observing its construction in figure 1.. .wnfiammunm oponamospw cmaaonpaoo new con: mspwpmmm< H oadmwm - 4 _ As stated before, the ends of the furnace tube were both open. A threaded steel tube with a cap to fit was designed to fit over each of the ends. The caps were made removable to allow for the introduction of the samples, thermocouple replacements, adjustments of various sorts, and cleaning. Three holes were drilled in each cap, into which copper tubes one inch in length and 1/4 inch in diameter were inserted and soldered into position. The purpose of the tubes was to serve as an in- let for the thermocouple wires and as an inlet and exhaust for the gases. A manometer and a vacuum pump were connected to these tubes as well. Figure 2 is a blueprint of the designed threaded tube and cap. The means of fastening the steel tube onto the silica tube afforded a serious problem. Furnace cement was first tried with little success. It was found that the cement after being subjected to the heat conducted down the silica tube soon lost its coherent properties and crumbled with the slightest torque placed on the tube. This in turn broke the air- tight seal of the furnace. A "steam fitters" cement was then tried. The cement was composed of litharge (PbO) in a glycerine base. It is essential that the PbO be in the yellow form. It was obtained in this form by heating the red Pb304 to a temperature of lSSOoF. for 50 minutes. Enough glycerine was added to the litharge to make a pasty mass. After thorough mixing it was quickly applied to the tube joint and allowed to "set.” This joint had excellent strength and did not crumble through- out the entire eXperiment. Hydrogen was used first as an atmosphere for the furnace. The gen- erator first selected was a Hoffman electrolysis unit. Connected in series with the generator in the order named were: (1) An ascarite .572n51. 7zxsur 42 IWEGLD 12 rub: PER m CAP CLEARANCE S 7551. 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L. pl nCQMZM 0;.Nan 00 20 U¢m - 26 _ The reactions generally assumed as occurring during a carburization process are as follows: 2 co 002 + C H 11 C + 5 Fe F950 2 CO + 5 Fe :1 Fesc + 002 It may be seen that the reactions are all reversible and therefore require "energizers" to keep the equilibrium shifted toward the forma- tion of the FesC. Common energizers used for this purpose are BaCOg and NagCOs. The samples which were cut to 55 millimeter lengths were then tested on the dilatometer for thermal effects due to different depths of carbur- ization. The dilatometer used for this eXperiment is shown in figure 25. The first sample tested on the instrument was an S.A.E. 1020 steel to find the normal thermal changes occurring when no carburization had taken place. Results of this test may be seen in figure 26. It may be noticed when comparing the critical temperatures obtained to the iron- carbon equilibrium diagram in figure 24 that the steel reacts normally. A general expansion is experienced from room temperature up to 730°C., which is the A01 point. At this temperature the pearlite transformed to austenite and the ferrite gradually dissolved in this austenite until the AC5 temperature was reached. In the case of the S.A.E. 1020 steel, A05 point is 83000., which again checks with the equilibrium diagram very Well. It may be noticed that a general contraction occurs through the austenite-ferrite zone. Upon reaching AC5 an expansion again occurs. When the alloy is cooled, the reverse effects are encountered. The upper and lower criticals being termed Ars and Arl respectively. It may also . Figure 25 Photograph of Chevenard Dilatometer -23.. . . . . a . ~ . .. ..H . ... .. . ...: l . ... . N.. ...... .... _ n c . o . . . o . . . H . . . . .. ..‘v enof . n .. .u.. 0.. . . . . . . - . o . v . ... .. A..~ .711 . M . 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N .. . u . o . . . . . . . . .. . . . . . 0 . . . . n'm . .. .. . ... .. . H. . . .....,.. . . . H . . . o . .. . . . fl .. .. . , h ole. . o ..000 OIDI It-...|1 Qt- ... o O DuaA 011.10- 1.10... .I .o. . o.» I. IOO‘IIII‘OAHOO $3.1.dnile¢1t‘.|fll§5n$.l¢.91fiw'0%llv‘.+TWI..J.'.!‘.9-.. .. o. . . . . . h n . — m . . m.. . .. _. . o . . . ... o. . .... u . . h . . .. . o. . . ... ... . ....A O. . .. .- . m fi 0 h... .... ... . P.... ... ....L 67..- cool‘ . . L [>1 .— . V V .... Sc ... .. .> . Eamzm Emzomz no 20. vi be noticed that the Arg point was depressed to 775°C. and the Arl point to 700°C. In figure 27 we may see the reactions occurring in a sample carbur— ized for 1 hour. It may be seen that the shape of the normal dilation curve has been altered extensively. The Arl point is found to be raised slightly to 740°C. However, the austenite-ferrite transformation line has changed its slope considerably. This is thought to be due to the fact that the sample has undergone complete transformation according to zones in the steel. That is, the case being of eutectoid composition has undergone its complete transformation at one temperature, the Arl point. Due to the fact that there is no excess ferrite or cementite to be dissolved in this newly fonned austenite, the case again tends to expand with an increase in temperature. The core, however, being of hypoeutectoid composition has not undergone complete austenite-ferrite transformation and will continue to contract through this zone. This will set up an internal shear within the zones and the resulting expan- sion or contraction will be a resultant of the forces set up within the zones. Two zones were selected for descriptive purposes, but in reality there would be many zones of decreasing carbon content extending from the case to well within the core. The same is true for the hypereutec- toid zones which extend in the other direction (toward the surface). The A03 point, for the reason given above, is very difficult to define. Apparently from the curve the A05 point is about 8100C., which is a de- pression of some 20°C. when compared to the non-carburized sample. The cooling criticals are apparently 805°C. and 660°C. for the Arg and Arl respectively. The occurrence of the change at 805°C. is not obvious at --4A. ..-.— ' V I Y ' f I -..-Q.--“ -... -....- —. cu. h r627 t Qn,of s.A.E 1020 s 0:01.1«0a.. v ...-p--.. -o— ma 1 0 . . O o w . o " .oll“t|co I -- ; --..-a t . . . . . . 'I'O-OII o 0 ¢ vO'TQIIIJ . . ...-,.-..- .---..-.- O I . A -.-.Jr-_.- - ‘0 b n--§v--.. . v~.9s~rru.$- 5d, mcmmzm quNOmz no 20. U+M - 31 - present. It is apparently higher than the Arg point for the 1020 steel. The Arl point was depressed to 665°C. and occurs in the same relative posi- tion for all of the carburized samples. It is quite logical, however, that the Arl point will vary that much over the range of compositions re- sulting from carburization. The lepe of the austenite-ferrite transfor— mation line may be seen to be quite different than in the non-carburized sample. The same explanation may be given here that was given for the transformation during heating. Figures 28 to 34 inclusive are dilation curves derived from samples carburized from 2 to 8 hours. The same general effects in the critical zone may be noticed in all of these samples as was noticed in the sam- ples carburized for 1 hour. The tendency is, however, for the case of approximately eutectoid composition to become the predominating zone in the transformations as shown by dilation. This is quite lOgical, however, due to the increase in the depth of case with a longer carburizing time. In the samples carburized five hours or more it will be noticed that the apparent transformation zone is narrowed down to some 30°C. which is fur- ther indication of the predominating character of the eutectoid or slight- ly hypereutectoid case. Continuous photomicrOgraphs were taken of each of the carburized sam- ples. They may be seen in figures 35 to 42 inclusive. The increase in carburization depth may be noticed with the increase in time. These re- sults may be more plainly seen from the graph in figure 45. The depth of the case in each photomicrograph was measured to the zone containing about an S.A.E. 1040 composition. It may be seen that the carburization rate decreases after about a 6 hour period. The cause for fluctuation -52.. . . . * .... .... + . . . . .»4 . u H.. .+ .. A..." ...M ...v a... 0.... o... o . .. M H ... .... ”Hm. . . . . . . _ . .. ..-. . . .k... . ... .:.1 '9‘. .... ... . . o . . k . . . . . M... . .W..¢4. . v...... _ .. .... .... ... H. . 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ITid-XL -. _ _ .e. _ . 4 - - .m. E. 4 4¢4- LI-..;w.«‘ . 4 4 wipe 07. ,3. . ..T._- 4 -. --- _. --“__....- *-.4r_ .... - ----,. - .-.-.. --..-.» H- - I ._._._ -1>-———--o——4 _-‘-. . 4 . 4 H 4 * ‘ . . . m .1 - ..- .. -- .- . H . .. II -Illlllllbllly .‘ 4 _ If. . . . _-__,’., - r --‘7L..V. ,__.___.&.- _- -.4 . .._._.._.__.._- - 4 —. . . ,_- -4 - . -4 _-........._ 4 4 . _. -ixérva. ,-.1...-ii-i?-4I-u--+l- 4.. 4 , fl _ a H 4 * . ‘ w m . u _ n . _. 4 _ m .- - c Q _ - . t .lh‘lo‘xlvlrtv' ’3 I1 \ _ . . m _ W . — . . 4. 4 . 4 ..... . u 4 4 4 L45 _ . _ 4 _ . - _ .. u - . + . . . _ _ 4 __ 1 4 4 4 .. 4 ‘ ., ., dew -. M . ' _ 4 4 I I Inf- I '14.1 «II If: ~11: . ... it. laii-l Al . _ 4 _ 4 _ _ - _ 4 q H . h 4 4 4 ,. .-.“... -. - ...—n l ——.+ y-—- ....-—- 4- . .A-‘ .. .... 4 .yl. W 1.. 4 4w 4 _ . _ ... w. .4 .- 4, .. u 4 4 . 4: m . 4g 4 .4: .4 ":4:-2m ...:Zma2 00. 2.0-. -————L - _-._._+ -—--—— . , . Fv—4..¢7- . . K" c '1.“ ' ';.“|~‘r‘ k“ '* ': " ‘ i ' ‘K‘K .~ K \" wit -'K‘-K‘~§\=»‘v 's': trt‘mflmw'fi‘ 135’ “K "’5’?“- D ‘ - . '. " -'|-. .'. ' | ' " ‘ a ‘ ""‘I'l ' ‘S - - 4‘s”? 'd“1.“.’”-.if-"<3 m1 ~ WYA'fhxhK i 3,13 $16K") 4"“- m-JK... K. . :5"? K ., ' ' a I. ‘ ‘ \' L‘ J‘ . ‘ ' ' '.- "Ff! ' s c " . “d“; r" 5’- 5?» .‘K‘?! .13.: ‘ "' ‘1: ‘ L '-“$r ya”: ". “,.Y:,"\‘:0 K ; -.\'.‘~‘K~K.- ‘x ‘K‘f— KK w- 8 .15 N.- ..z-Iz- ’3“- .' ..K.’}.‘-.-- - ' D ‘_ .' ' ' J ' ' ‘ ’ ' v. “a“ i ‘ ‘ 3’7}... . ' ‘. l t _ ‘ ‘ . . ..:.‘”%'J_-}:£;I“x’3lv ‘7"? A: ,II - 2‘ vi! ,'\ ‘) " ‘ -f' ‘ . . . (r .lil, - .. ‘-V '3. I fill} ;‘.:;hI 1 WVFK’X (3'1“! "H‘N-r 2-"? ..' _ . . . K. \v 'Pr . \. M1”: l.’ ._ Jr.“ 3 . - I - ..'.i - “ g l ~5 38 ‘ -\ . L! - . . \ . . . . . a . . . 3 ‘ K_' .. . .~ 1- “ . v .‘ ‘ -\ . " -.'.d- \ __ ‘ ‘.‘ - ‘ \ - ' I o " . *1 n ’ . ‘5 Figure 35 ' S.A.E. 1020 Steel Carburized 1 Hour at 17oo°1r. Mag. 1sz from Edge of Sample. .... o a) K063 8) 0 ON HO Sir-c no «4 0 rum 0 <3: 0 U) Carburized 2 Hours at 170003. Continuous Photomicrograph from Edge of Sample. Meg. 1601 -41... N03 .3: 638% no mwcm Eon.“ Amwhwonoaoponm 96:34:80 ..moooS 95 990m m 33.39.30 floopm Omoa #4546 en oaswam , ... ...... fifif? ORJ. - . r 0.. O I n t n‘. . . . .0. . ...t.& . F n . I ... I » . I ; .‘l l A O \\ .- O - 42 - . I .... ' I .. L‘a ITEN {be 1' r 54-14%" ‘. p_ . I" .. '4. -- ......» Q #1451 N‘ 6‘ .. ~ 43.:- _, "o ' . ‘Qtf"m .\ ,Y_ .N' - - .' .' p- " c fl.‘ ’ ‘ ,- ”‘4‘; I :: ~53, '¥.V.,f’ )'?- Figure 38 S.A.E. 1020 Steel Carburized 4 Hours at 1700°F. Mag. 1601: Continuous Photomicrograph from Edge of Sample. -43- Noma .wwz .oamewm uo mmwm Eomm nmemOHOHEoponm wdoddwpcoo .moooua pm mhdom m comfihdnpwo Hoopm omoa .w.¢.m mm oksmfih . n... 5.‘ . . / “‘43 n+3 {Haj ....... .. 4 .. . .l » Mgdfi .on‘v...s+ I H ‘H-«LIoo . .H . . 4 ... . .. . I . 0?..Io». .. . :oo.4~fi[. .I ..m .. . . . u .4 . H . 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I. 4 I A 4 g H . . . . . ~ . o . g I a . ‘I . . . ~ . . - .. . n . o o I o o . I . H . . . o . . . . k . B 4 . .. . . . u u _ _ . I I '1 I-I.: In C IIIII II ... I 0.0 IIIAIIoolhII'III TIIIYI IL .IIIFI'IIIIIIIIIIYIIIIII liti’llilolol' v .A. II .II .fII oII IIIoIII I.. I I III. I. 4' Io I I III; :II ... V. IH .. v u i q:g . . ... .I . 7.! . H . . . 4 . n I I . . o a o . . . . . . M . . c 1. 4 u . ... . . . a _ . . _ . _ H . _ . o a z o . _ . . F III I J < 4 I n 1.1 I o H h . . . I H . II I H . . . . .I I . o . v a . . . . . . - . . . . I . . . . . . _ . _ . . . . . . . .I n . . . . . I II. a I. Ir'I II'.’ III OI OIIYII 3‘. III- ''''' £II- IIII‘IIOIOAII‘O'J II...II II ..III. I... ... .II..I.II.4 IIIIIIII I ...... .II..4. ....... I... III II . :IAI.:I.4I-I : III I 4 In” . M a 4 w .. I . D 4 . . . . H . . r e o. n . . o a 9:. . . H I n . . . . . I. . a a. . H .I no . . . . > . H . II 4 4 I 0 I I . h . ..1 . m . I I.. . . . . . o n . “I! — o ... o. . . a . . . _ . . . . I _ _ n . .. . o. . . _ . . _ . o 1 . . o . .. L w w u - II III- IIlB I I IIII| 9IIIII7 Clo-Ito! :.II.|0II|IIIIII'I III’IIHII IIOI TI'II I‘II : I I N I I . I: III I I I I “I . I. c I l I I I A III I e uOI A o It. I II II I . I I III I o I: I I III I” II J o ”IV I . . 4w . . . IIIIH. . _ . . . v . 1 I t . . o _ I . a c 4 w . . _ _ _ fl 8 u“ . o . 4 . I” . H . o 4 L qr . . . 4 d o . . 4 fl . I.- . . . 1 . . 4 . ..V . .. . . . . . . . . H . _P . . . . - H .4 . . . . . I ._ — I H . . . . . H H I . . . III I lIL IOIIOII II'IO‘I .IOIIIII IITIIIJI'I'II*.'II IIIIII. IIIIL IIIIO IIIIIOII . I I 4 o It I I I . II. a II I II I I I a u l I I4 o I I III II I IIIIIIA I I I, II II. . g . . _ . .u . fl . . . . . _ . . 4 T . _ . . . 4 . . . . . 4 4 . . . . . . . 4 . . . . . . . . . . . _ . _ 4 . . . . I I . I ’* pl _ _ . - . - . I . . o _ _ . + . . I. H . . . . . . — a . I . . . . . . . h . . I . . H . . . . p . . _ ... ..- 4 . . . . . . . o . . - . .- . 1 .. .. . I I L I! I7.“ I‘ I H I b I. II .III I. To III I III IYIII: ..I..III.-I IlIIkoIoIoIIL IIIIIIIIIIIL I IYIII- VIIIoorIIII HIIIIIIIIIIIIIJwIIIIIOIWIIII; II “I‘lIIIIIIIIwJII t H I“. III 0 I I III . . . . . . . u u 0 I. I I. . H _ . . . . . . . . . .. .m H I 4 P . . r HII . r I” I: I I a I. I . .I . J. . ., . A... .I. ..m .4 . - .- . . .. .. . . . . .k . . . v . . . _ 4 4 . . . _ . . .-.: .. 4 . 4 ~ u v u * < . I 4 n O . o n.. a Q o . . . . 9|: IIIIQIIIIIIAVIIIIQIIII VIIIIIOIIIIIIATIIIII‘IIIIIIFIIII ..III. IIOIIIII'IIIIIIII.III;IIaI1I9IIQI¢IIIIIIIIHTIIIIIIQIoiII‘l10IIII IIOII III OIII III OI II. I I I; OYIII I II IO‘O .VIuOon‘O I IIIO7 A .I . o . .. .I a c o . . . . . . I . . .I . . . . . 4. m . ~ . o . . . o H . H _ ...C . o o. . . . I a .. . . . . . — . . . . . .. . H . . . I .. 4 4 4 1 I 4 o o 4 . a .I o ... . . . . 4 . 4 4 . . . . 4. . _. . . - .. < 4 . . a . o . a a . .... I . . . . . . . o . .. . . . . . H . .. . . I . . . ~ . . . . . .. I . . 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IO- QIII' vICIOlOOIOIIII . . . .I a I . o ..I._ 9‘ _. ..III 0. ~ _ o _ o . I.4I<. ... .... 9‘ III a. 4. _ .~ . . _ . .I o L . - . .4 ...I.. I . . a .. . o . . .. I. M. I . .III . I. . .. . .. . _. . . . m J I I .. o. u . . . «- . I. . . . .H. .. v . . 4 . . .. . . .I . . . . h . . . . . . . .9 . I I. . . . . . . .. I . . . .. . . . . . . . . III- -IIIIIII IIIIIIIIIII-IIILI . I I Iv I IIOIOIA : I I I I 0.. o I. I I l V O . u I 4v. 5 II. 7):, ..- . I 4 II 0‘ I I I It. I I I A-- IIC‘II. I1 . u e . n _ . . s . o I. o. .. . . . . . . . . .. . o I I” .¢ . o o _ . . . . H4. . . M . . . . . . L 3 - . 4 - I r . ; .. . .. . . . . . . _ . p ....o . v I». .0 n . o . e o o a H. . II . r. o . v .4 . _ . c . H . o H . a I H . H. . . . _ ... v: I_< 1' I'II. QIOOI IV I. all 'lII. . 7 o. I III... I. .Ivlo II. . ”I. .I‘ ‘IOIOI 'll'..-‘ . .. . . . _ o o .I e I . . M . . ” H . I HIMI . u. JII. .. o .I _ . . . . . . . 41.. u... 9; . . e To... I+Io 4 .I S w u c...c.rr..z ... b. “4. . :9- e... m I - 48 - in the shorter carburization periods may be explained by the fact that the carbon did not diffuse at an even rate. In some instances the car- bon content reached full eutectoid composition before any further appre- ciable diffusion would occur. This may be noticed especially in the sample carburized for a one hour period. ‘Very little diffusion has oc- curred past the eutectoid zone. In the sample carburized for two hours, it will be noticed that the diffusion depth is greater, yet the carbon concentration in the case is much lower. This may be due somewhat to the nature of the carburizer, the quantity of carburizer in the bomb, or to the surface conditions of the steel. Figures 44, 45 and 46 show the hyper eutectoid, eutectoid and hypo eutectoid compositions of the sample carburized for eight hours. The ex- cess cementite can be seen in the grain boundaries of the hypereutectoid zone very plainly at this higher magnification used. This is not appar- ent in the photomicrosraphs taken at lGOX. The pearlite may also be seen to be a distinct lamellar aggregate of ferrite and cementite. The pear- lite in the hypo-eutectoid photo, however, shows that the pearlite is tending more toward the sorbitic form. Figures 47 and 48 show the eutec- toid and hypo-eutectoid structure of the sample carburized for 3 hours. These photomicrographs are likewise taken at a magnification of lOOOX. The pearlite is again well defined in the eutectoid zone, but is in more Of a sorbitic nature in the hypo-eutectoid zone. Figure 49 is a photo- Inicrograph taken at lSOOX of the sample carburized for 1 hour. In this Case the pearlite tends toward a sorbitic form. - 49 - I; A} V. ‘.-. ‘ l/ '4 )HW'" Figure 44 HyperbEutectoid Zone Case Carburized 8 Hours at IVOOOF. I ‘\l "L1. “\ F" 1:31.313. {1"} ' ‘3 ,§\\\\x§‘x;fm\\) 9: L ' - ' Figure 45 “V'-:fi(j$33 (2,5; f"z- ‘ Eutectoid Zone _ }»”»»w&LC ;..£;'J1 3] Case Carburized 8 Hours a 4 w at 173331;- r "\'|\ \. :-_- v .3. \v"\).\ . \‘n .- x3: Figure 46 Hypo-Eutectoid Zone Case Carburized 8 Hours at lVOOoF. Mag. lOOOX "7"?" ‘5“.5. - .... , ‘ ' 3' '3’" I r I ~ .1 -50... Figure 47 Eutectoid Zone Carburized 3 Hours at lVOOOF. Meg. lOOOX Figure 48 Hypo-Eutectoid Zone Carburizec 3 Hours at l700°F. Mag. lOOOX Figure 49 Eutectoid Zone Carburized 1 Hour at lVOOOF. Mag. 1500K l. 2. COJCLUSIONS The effect of carburization on the critical thermal range as measured with a dilatometer, is a resultant dilation effected from the zones present. The great- er the depth of case, the greater is the tendency to- ward a single eutectoid type transformation. Carbur- ization periods of 6, 7 and 8 hours reduce the trans- formation range to a minimum of 30°C. The normal range for the non-carburized sample being 100°C. (S.A.E. 1020). The rate of carburization is retarded appreciably after a 6 hour period. Non-uniformity in carbon content of steels may cause erroneous critical point measurements when measured with the dilatometer. BIBLIOGRAPHY l. "Metals Handbook": American Society for Metals,« 1939 Edition, Cleveland, Ohio. 2. Sauveur: "The Metallography and Heat Treatment of Iron and Steel," Fourth Edition, The Univer- sity Press, Cambridge, Mass. 1955. 3. H. E. Publow and W. P. Fitzéfiandolph: "The Micro- structure of Hardened Carbon Steel," Bulletin No. 45, Michigan Engineering Experiment Sta— ]“77‘13‘41 Té:m. ”-92 a .' ' r tion, April, 1932. . U . . u . .. . 1.. IA . - ‘ «...-r0 . 1...: .. .. w ...... 4-4...\.IS-J.VM . \an .....Bu...’ . ... lute. fi_rw...‘. .. .1.“ . -..: . y . . 1.. it- .1. 1 a \Ql. fi‘VF' . k u. 2 .. u y ‘ In . 1:. 11‘ . . “8'4..m.k . .. . ‘ r...($\ NJ? I. l, .I‘ . if? . h. ah~ . h. . , I. . . . . . do ‘ ... . . . . ‘ . 0.10 .h .. A ‘t’ _ ...—”Che“ ..e .w. \ at h, ,H . -. v . i V 1 , , "—M‘-‘ V,‘ . . L. 4 d‘ " {Oi-.‘ol .......... o. SJ. ..7: 1...... 0 I I v'QJ t n; - ,\_- .- P I . I r ' _ .j'fgx." l O .I _‘ .‘ 5" vv - ' 1' 'l- - '5 ~ - ‘ ‘U;y' A I ‘ l A . ...... _. I - ' IARI’4 .‘A. 3 don”t): I . ”A ' ' +wa "xii 1;er D l “A. q —. 11"“ . " d» a 4 .6‘ 2“; . 2": ‘ . _ . A Mfg ' -¥ _ g - ' . of: -t (g- ... V I ..v 3,, 4 :-'-. {”539 " f... .- A3 ' ...-1'11”“ -. " I -‘ ‘ --.; 3" ‘Vm' ' - _. ' ' ’ . 7.. ' h. ._ ' ..' . .' o ..f V‘ ‘ I “ I '. ‘ 3". 4 ‘h. I ‘ . ' "r l' *3 J A' a.) ,." ' I C. " ' : ‘ . i .‘ . . - .- , _ ... v' 3 ._ ... . T ‘ nr_.‘.v_ « - , . . II .V. ’ ... ‘, ‘ . :: .‘- ‘ ‘ '. J ‘ A" II’.‘ ‘ ' ..' '.'."'“ > ' ‘ ; ' "... J' u ._ ." ' ' .1 3' " ...! I, ', . . I. o-‘ a ‘ y ' ' ..‘I ‘ ', ‘. f , .‘l': ‘ - - ' 4 ‘ ' '. 1. _.‘. ' ' I- ‘41 "' . V f A '_ . . . ‘ - 2 '0 - '-‘.‘ ' ' ' .- ' ' ' .'.' . ."' o _ .' ' ‘ ' o -. ' 2 I, - ' i L'. ' ‘V -‘ ' ‘ . . i.“ ' ‘ ~ .‘ . -- p ' ' u ‘ '. »' . ‘- 4’._ u ‘ ; - . .. 1 _ . . ' . ' ' ., .- ; _- — -_ ‘ 4‘ ‘ 0-. V . . A o -. __ J. _' ' Ld': ‘ ‘V ' ' I ' . J O ‘ . I *2: 4 .-,Ar ' +‘lr.\: 'I. "VI... .‘ .. ’ '9‘ $5435 51" . . c - -- .. M“ sac “ I ‘3 . m; _ } .7 l- . IQ. LS}, f h .9! _ a .141'3ANSTATF LerFRSITV 1111'? ‘fF‘S ll ‘ 0 1 I 174 572