f f r ’7 fl 7’- ___—E— .——e _ W, 7 _ 47 , _ ,7 7 7, .. | 1 h I i H \ 1‘ \E __I N (D A STUDY OF THE PHYSICAL PROPERTIES OF MEDIUM CARBON STEELS Thesis for the Degree of M. 5. Kenneth J Trigger I935 \ 0 o w: tum/1 63 Y ..", (lazy h 1",,“ ‘-.%“< ‘xpi-wr‘": “‘5 " "‘f -' ow? {1:115}; “ ‘ 1:14.): .\II :(‘I‘ .’_‘ -‘ .9" “ 'n’fi-M‘V‘. .. n"? - ".’ '3‘.“- 4...! "5 t “ .tg'fi-‘TI ‘ div-<1”): r‘ H.‘ '- v ‘. ’ $.d“‘.‘..‘z D . .I l' h" \ . r. .. » " I‘,""o)f “fil‘ '(:$c;‘ 3"; ' .f “r; «.W H141, L: 3.» WWW“. r. "Haw“! 3W! ’V . .‘ .- m “’: 1‘ “.1 . a? "3‘ ‘ " 5" v9“? it". {iii}? 1'}. g‘%¢}$ w 4. as. 3H i a M?" my gig ‘9 I . .. ~ '3}.- .‘é‘i WW ~. ""1".“ ’4 j "- h.‘ '§~‘{- ' ‘ A. I. '“’1"'\’1-’r&' n . «.239 1"}. - ~ ‘, . . .. ‘ 1*t‘ ‘K'g ‘. H at: b 9 1“» In”. '- 10"th EEL'F’ have“ L} A i Nusa=kuv ‘ ”I. . _‘ A STUDY OF THE PHYSICAL PROPERTIES OF HEDIUH CARBON STEELS A Thesis submitted to the Faculty of Kichigan State College in Partial Fulfillment of the Requirements for the Degree of Easter of Science Kenneth J; Trigger 1955 \leH 11 I ‘ n tying-v. ,uIy m0..v.m.l:.h flu 1‘! THESIS ACE’EIOE’EEDGI‘JIEIIT r“he writer wishes to express his sincere appreciation for the kindly assistance given by Professor F. G. Sefing during the progress of this work. 98?}??20 TABLE OF CONTENTS Page 1. INTRODUCTION . . . . . . . . . . . . . . . . . l 2. SCOPE 13.23) PUKPOSE o o o o o o o o o o o o o o 5 5. EQUIPMENT USE . . . . . . . . . . . . . . . . 4 4. FUEUACE ATHOSPHERE & IT EFFECT ON THE SCALE TIT I 01:13.2 8 S o o o o o o o o o o o o o o o o 5 5 . 3.1.4.}; JJLS EVIL; STIGELTED o o o o o o o o o o o o o 9 6. GRAIN SIZE SPECIFICATIONS & PHOTOEICROGRAPHS . 10 8. TESTS ON THE IIPACT SPECIIEE . . . . . . . . 28 9. TESTS ON THE SMALL CYLINDERS . . . . o . . . . 51 10 . COIICLUESIOIIS o o o o o o o o o o o o o o o o 55 11 . BIBLIOGRJ‘LP}IY o O O O o o o o o o o o o o o o o 56 {‘1 It], . 1ygflru nfiiuvvfir.‘ IHTEODUCTION It has often been observed that while two steels may meet the same chemical Specifications they may show vastly different physical prOperties, particularly with reSpect to toughness, depth of hardness, distortion, forging properties, and susceptability to heat treatment. This variation of steel has caused a great deal of trouble to the users of plain carbon steels. O In view of such differences in steel, metallurgists have come to the conclusion that the chemical analysis of steel is not the only important factor determining its prOperties but that the grain size must also be considered. With such large quantities of steel required by present day production methods it becomes imperative that the steel mills manufacture a product which can be relied upon to give uniform results. At present the study of grain size control in carbon steel and its effect upon the physical prOperties is one of the most important and most widely discussed phases of steel metallurgy. T'It is generally believed that it is grain size or perhaps some still more fundamental condition which is responsible for the variations in physical prOperties of steels with the same chemical analysis. With reSpect to the factors controlling the causes of inherent differences in steel, the following is quoted from ”Deoxidation of Steel" by C. H. Herty, Jr.(l) "In the steel entering the mold and the reactions which take place during solidification it will be noted particularly 5111 h ‘II .L 1L. 1. v. ‘b.s'lp £533.. . hi?” 1.3%,!“ Ewifl“ .Io that, aside from chemical composition, there are non-metallic elements in solution and in suSpension and that the amounts of material in solution and the type of suspension are due largely to the deoxidation methods employed. One of the prOperties of steel that might be affected by these solutions and suspensions is that of grain size. "It is the general concept at this time that fine-grained steels are the result of the presence of a fine suSpension which furnishes nuclei for recrystallization during heating .through the critical range. Steels of the same grade will vary in grain size as a result of the type of fine suspension present. For example, if a steel is deoxidized with silicon alone it will always tend to be coarse grained and will show a marked coarsening of grain when overheated. Aluminum killed steels on the other hand, are almost always fine grained and will not coarsen until a higher overheating termcrature is applied than was the case in the original coarse-grained steel.” From the above statements it is evident that the final quality of steel is largely determined by the deoxidizer and the method of deoxidation. Steel manufacturers are now making use of the knowledge gained through recent experiments and are "grain size controlled steels” by preper manipulation producing of the various deoxidizers during the steel making process, and at present grain size is a very important Specification. l C»! I SCOPE AND PURPOSE In view of the present interest in the grain size of steel, this study was undertaken for the purpose of investi- gating medium carbon steels with respect to the relationship existing between grain size and volume changes on hardening and tempering; grain size and impact strength; and grain size and cracking tendency of the heat treated steels. T iI.l‘L ..l. ‘.s . . .tr». ,. . : 4.4.3.5.. .fl...,sn.[,_m..¢ iré‘ - . EQUIPL’IE IT SED s were used to obtain the dimensions "S micrometer calipe of the test cylinders. The same micrometers were used throughout the work and all measurements were made at 20°C. An electric muffle furnace equipped with an automatic termerature controller was used for all the heat treatment work. A gas burner was installed in the furnace to give the preper atmosphere for the prevention of scaling. The chemical analysis of the gas atmosphere was obtained by use of an Orsat gas analyzer. A standard metallurgical microscope was used to deter- mine the grain size of the steel. A Brinell hardness tester was used to determine the hardness on the large cylinders, a Rockwell tester being used to measure the hardness of the small cylinders and impact bars. The impact strength of the various steels was determined by use of an Izod impact testing machine. This machine has a range of 120 foot pounds and can be accurately read to my foot pound. A small power hammer was used for the forging work. T TT’IV T I .T ‘ fidVTTHO..fl T ..I‘ I PURE-L". E lei-IOSPIITIRLS AI-TD ITS EEl-L‘ICT 017 THE SC:‘.LE TIEICI‘QIESS Since an important phase of this study involved volume changes it was imperative that the depth of scaling during the heat treating operations be reduced to as small a value as possible. This was accomplished by using a controlled gas atmOSphere within the furnace by the use of a burner placed just inside the furnace door. Local city gas was used in the furnace. The composition of the gas varies and the following analysis is given as being tyyical: 002 02 CO CZH4 H2 CH4 N2 H20(vapor) J n /’ r-‘I’ r: P? r- " f, (1 I O 4.53 . fl 17.0fi 4.5; 05» 2 p 9p remalnder A series of tests were performed to determine the scaling effects in the various atmospheres obtainable with the furnace set-up. The results of the tests are shown in Table I. From these results it is evident that there was always some oxygen in the furnace atmosphere, the most favor- able conditions showing .Sfl oxygen present. According to Table I, two furnace atmospheres may have the same oxygen content and yet show quite different degrees of seali 3. For example, consider tests A and F. Both had the same oxygen content, but test A had a higher 002 content and a lower CO content than test F. 002 is known to be an active scaling agent‘Z) and probably does play an important part in the scaling, as is brought out in the tests just mentioned. TABLE I REST: TS OF PRELITIITIAT'ZZ' 'OTC OI? FURNACE ATTIOSPHEIES. *“ *---.~-o . u. u. -. -.... -- -.--~.—-.--.-.m-.--.~--.—.w—‘n “-H ~o.—.—-O-- -—-—‘ — Edfiace Gas Test Analysis Ratio of Temp. 002 02 co 002 e co 0 v— = ’-".“.' 0 Remarks ~—' g... -'~ A 7.4 .4 8.8 .842 595 Woticeable scaling B 6.2 1.5 6.9 .90 650 Uoticeable scaling C 6.8 .4 12.5 .548 595 Very slight scaling D 5.6 .6 15.2 .424 815 Very slight scaling E 4.9 .5 16.0 .506 595 Exceedingly thin scale *r 4.9 .4 12.6 .333 595 Average depth of scale calcula ed to be l.5x10“0 in. **G 4.1 .4 17.5 .257 850 Avg. depth of scale calculated to be 2.6 x 10’0 inch. * Tenpering Temperature *rQuenching Temperature ,L figwfql Chiba-J..- TI‘ A. From the test data it appears that the ratio of 002 to CO is an important factor. Referring to Table I, it is seen that if this ratio is about .8 or higher the steel invari- / ably shows appreciable sealing. However, if the ratio is around .5 or lower it is possible to heat the steel with but slight scaling. A C02 to CO ratio of about .5 was found to give very satisfactory results, provided the oxygen was kept as low as possible with the present equipment. Tests were performed to determine the thiekress of the scale under the different heat treatments used. In the test at the tempering heat, (Test F - Table I), 12 bright cylin- drical sanples were used, 6 of which had been coated with quenching oil. The samples were weighed on an analytical balance before heat treatment. They were then given the tempering treatment, 59500 for 1% hours, in the furnace atmOSphere, and after furnace cooling, were again weighed. The increase in the weight of the samples was due to oxygen combining with Fe to form an iron oxide. Under the conditions of this test it appears that the particular oxide f v, 3A 1" (V l 0"- (5) .9 H. 1' Q .(‘j J. r. r- r~e~ olmCa Mao argcly FeO . KnowinQ tae weight of oxygen going to form FeO, the weight of FeO formed was calculated. The specific gravity-of FeO is reported in the International Critical Tables to be 5.99 and since the dimensions of the cylinders were known, the thickness of the FeO film was calculated, assuming uniform distribution over the surface of the cylinders. The preportion of Fe in the FeO was determined and the ’{I Hum .. ~ v. flunk 5A .hllp.‘ ‘ thickness of the Fe film entering into the FeO was calculated. ‘0 The difference between the thickness of the FeO film and the fl 1' Fe film represents tie increase in dimensions due to scaling .1. during heat treatment. The scale thickness produced in ttst \D F was found to be 1.5 x 10'5 inch for the cylinders coated with oil. It was found that the presence of an oil film on the samples reduced the thickness of the scale to about half of that on the samples which were not coated with oil. As a result of this observation, all of the steel used in this study was dipped in oil prior to heat treatnent. A test similar to the one previously described was i I 7 performed to determine the scale thicgness under hardening conditions, 850°C for one hour, followed by water quench. (Test G - Table I). The thickness of the scale formed under these conditions was found to be 2.6 x 10—5 inch, slightly more than was formed under the tempering treatment. Since the f nest measurement in this study is of the i order of l X 10-4 inch, the results of the two scaling tests were considered as sufficient proof that the scale thickness formed under the two heat treatments used was so small as to be entirely neglected. With the previous results on scale thickness capable of being duplicated by preper adjustment of the furnace atmos- phere, it was concluded that the scale produced would cause no appreciable error in the volume determinations to be made later. I dial 441*- L Giuliani ....nlraI: In?!" AL ANALYSIS OF DIWTERCIT UAITUFAC TURERS STEJLS TABLE II C‘ WT‘T" L.) .l._J 4...! IEVBSTIGATED C0 A8 HEP OWTED BY exp. Heat \teel io._‘f No._fi Co. _.C Kn. Phos. SUl' 811' 51 - D .4?-.44 - - - - 54 90,185 B .42 .70 .016 .055 .21 56 81,112 B .48 .41 .015 .028 .21 57 55,254 C .44-.48 .77-.80 .014 .024 - 58 51,544 C .49-.55 .75-.76 .012 .022 - 59 29,101 C .55-.57 .79-.81 .014 .024 - 40 89,011 B .48-.51 .72-.74 .010 .025 - 41 59,045 B .45-.48 .71-.75 .050 .052 - 42 89,114 B .46-.50 .74 .014 .021 - 45 29,095 B .47-.50 .68-.70 .014 .028 - 44 62,480 C .42-.46 .64-.36 .011 .021 - 45 2J,189 D .45-.47 .65-.65 .028 .017 - 46 9-9215 A .49-.52 .64-.66 .018 .028 - - 10 _ GRAIN SIZE SPECIFICATIONS ND PHOTOHICYOGRAPHS The grain size of the steel was determined according to standards of the A.S.T.H. Designation E19-55 (carburized at 927°C (17000F) for 8 hours and furnace cooled). The grain size classifications run from No. l with about 1% grains per square inch up to E0. 8 with 96 or more grains per square inch. According to this standard those steels showing grain size Nos. 1 to 5 are considered as "coarse grained" and the steels that show grain size Nos. 5 to 8 are considered as "fine grained". A steel of U0. 5 grain size may be either "coarse” or "fine grained", d.pending on whether the other grains present are mostly coarser or finer than No. 5, e.g., a steel showing a grain size of mostly Ho. 5 but with some No. 6 present would be considered a "fine grained" steel. A steel which the writer refers to as having a "duplex" grain size is one in which the grain size classification shows it to contain both coarse and fine grains. For example, a No. 2 to No. 6 grain size would indicate a "duplex" grain structure in the steel. The discussion brought out later in this paper will frequently refer to coarse and fine grained steels. A series of photomicrographs are therefore included here in order that the reader may have a clear picture of the differences in grain size and microstructure of typical examples of coarse and fine grained steels. .....fl.’ «J The steels selected as being representative of the two classes are No. 57 and No. 42. The chemical analysis of these two steels is essentially the same. Some of the physical preperties are shown in Table III. TABLE III PROPERTIES OF A CORRSE & A :IIE GRAINED STEE Steel Grain Brinell Increase ERIKQEEEG Izod Cracking in No. Size Hardness Hardened” Tempered Impact Large Impact Cuenched (5950C) value Cyl. bar _ :23 130.. fans. _ v 57 612% 565 .0756 .044 94.5 No No 42 .2- 514 .1590 -.0504 69.6 Yes Yes (severely) *A bar under the grain siz, number indicates predominate size. The photomicrographs and the notes appearing with them are, in general, self-explanatory, but there are a few facts brought out that merit further discussion. It will be noted that throughout the series of photomicrbgraphs, steel No. 57 shows a consistently finer structure than does steel No. 42 when both have been treated under identical conditions. An interesting feature is brought out by comparing Figs. 5 and 11 and 6 and 12. Figs. 5 and 6 show the hyper- "as entectoid zone of steels 42 and 57 respectively when the received" pieces are carburized and rated for grain size. Figs. 11 and 12 show the same zone of steels 42 and 57 respectively when carburized after being forged. It will be noted that both Figs. 5 and 11 show He. 2 grain size and both , Figs. 6 and 12 show Ho. 7. Several other steels given the carburizing treatment were examined under the_nicrosc0pe and in all cases the grain size was the same before and alter the steel was forged. This would indicate that the grain size as determined by the A.S.T.I. method may be regarded as the ”inherent" grain size of the steel as it is not altered ’ by severe plastic deformation at forging temperatures. A cohparison of Figs. 1 and 5 shows the coarse grained steel to be of about the same grain size in "as received" condition and after being carburized. Similarly Figs. 1 and 7 reveal that the coarse steel exhibits much the same grain size "as received" and after forging. The same thing is evident to a lesser degree in Figs. 8 and 2. In forging the hot work was stepped and the piece allowed to air cool from about 875°C. Fig. 15 is included to show what may be an inclusion in the steel. The photomicrograph was taken as representing the beginning or "root" of a crack in one of the impact specimens machined from a forged bar of steel No. 42. Several other cracked impact bars were examined in the same region and Fig. 15 is typical of the microstructure in that area. Different polishing methods were resorted to in an attempt to ascertain whether the slag-like appearance was due to polishing compound lodged in the crack. The appearance was the same regardless of the polishing method used. The writer has no positive proof that the "inclusion" was slag, but it had the same appearance as the inclusion (ferrous silicate) in Fig. 5 of a recent paper by Urban and Chipman.(4) at)“. z .1 4. w! s . L . . v 4 . D‘ A .7 . K flI‘EI‘,’-i!.oi.lu.j~l|vu4r:§i‘v .. 4 4. v . a r‘ v_ j 0 q , o I _~ k}. a k) l N, i190]. "13 3‘ 100x 7 .’"‘.": '3 7'1 {A L 12 ‘1; n 1 OF - —\_’I -- '1 Y’ steel ‘13 1(3Ct: x? 1.791 'I " 1,3 ‘1‘? J -n 'I ..L .g ,4. "'q "‘. (1" (I , . E, f U f1 1 ‘ \ A V‘. v a o 91 - r o < . , . ‘ II A -.f, , - :m' . -, x .1, v3 d" 0.1“ nnfiOn gl\>_’ , ' a p '5 p '._) _ l N ( .. li" r ( U -/ a d..- )JJL 10 t ". "-3, I" C .' fi — treat «p -I- 00» 5.4 I n10, 1:13;- 1‘ Q Jv L.) ~-’. 5 "I. O H , I“ . k . f» I ~, ‘.- V I . I LJ V‘ - \ ' .1 \ --rv‘ ‘4 \ I; ._ . r l V " I 1 O I ‘0 I ‘ V (J ‘ t. < ".4 a. Q j 'I . 011‘. r v“ ;p_ 'Q r) f- ‘>. f‘ .1 'fi 1 " I1. I . 'J a, ", . ‘. fi'lr)!’ J. P . J . 3 :1.) .__“: I‘ ‘ r r\ .'~ ,k L '. LI _ -L ' i". It‘wo - V17 .-. 3 J 9f! - a \ .- . ‘4 I 'Q “.~ f." ..,.~.. 2 .1" L Hut-3 f-‘f'.3l_L 1 (“”111 \__t 1- .L J. I-- "‘ \_0 1575 L. . LI trea 1_ o o v.1].‘3‘ss‘, "w-fir- '-- ‘,‘_A- _._l-.__.- C q (‘1 8.. Id. .‘ I .1 . c . .10 “(1‘ on a‘b 100~ J. J L. fix .Qs .u a... o. r n). . . .. r.» I; C '. a. f r. o ... ..q .. 0'. \z . Fl “a 'l) I. A . _ D I I n. O . .\ If .(\ a b I". ‘- r 1 ,- “ff ..( air cooled fro» 10o— - c 5 00. u?» ~ . r '3 s {31‘11('t':.“.?‘£‘- for‘el 79.011“: .... o . A 3') ‘41. ‘V v br- ~- _ -.O. sued. :. 1‘» 0.“ Air cooled 140w Coupare sURWCiwi #p“|fl K 1 9 }‘_I f I ~ a ...4‘5 .. b L \'. ( r: «w . fl .'* {\v 3. IL- . I (I1 H . f .7 ..H a; a v I. u”\ . . Ow. Or 7 .. OI”. _ . H \— J ‘3‘! ‘C’Li'g: “ , . it I-.. .r. “I \l: 1 w‘. ‘ff"(‘\ 1.. "r fr?! ‘»'0 ‘1 .7- 4- IL- 0 ‘J C 03 r3 ar 3 O 0". / ’—/ -.L . " l' I v (7 ‘1' . ‘ - _“ -‘ L ‘0""\ n.‘ '1 _ !.\, ~fi. J6 -. . c 1. or 'ml ... s ." v.‘ VJ w ‘ " r ‘. .‘lj ..-' _' ‘, -"o_ .‘ ‘1 _:- " a (-3 "."{,t _ . \J_ L “O" ‘0 ]( I I ' _/‘.J . Li-.. 1.,11L, .° '4 ‘ ’7 o M Ll-i: ;‘ l m n \ ' l i A ( ' \. ..L ,3 \l __ ,. r‘ 5"rflt f‘k‘x.‘ L47- ‘:_J h v, .1 3 J .i 'T’r.’ o) 1' TN .'-\. fl" ‘ —’ ‘~-' on L m .fi. r. r l . , .L , 7! .‘ o O " ‘ I ‘ Pi ‘ ... v '- b _ W} - - rt’ "'5 -. ..L 4 L1 L,- . _-_ I, . (W _ . ‘ . .. .. o o r r: - (.r , \ . L; - A :1. r. . r ” 9 .0 _ . u_' '1 o' - r' u. t . '1 .... ,. .'. ..L l ’I O .1~'—‘ ~’\) (.1 . x.‘ - .n t (W: )1 ,4 " ('5 I r. ._ \ L.-.L. (jft'f' (\f,’ ‘0.) 5. K - I p ‘ 4‘ I flew .“ «I ’ *( f . r, ’- .' -?"K~Y\‘" ‘5 :ég .' - I i . - -.. . ‘ fiv—e — —L, 0 .Lu 1 .~. - -. .. "10 ‘-)“LIjs-\‘J.‘~Y_’\ ‘I ’ ”'1 'f . I ..k (J (3“)'I (‘mfi eon ‘— 3 . Ca. MC :AL ‘9'!“— '; , '. (-3.9. (‘V‘ . _ ‘ a: a) )PCHL -1‘1 7‘" I )0}: Q. r J, ~‘Ot(3 U"_’.? a“ r; ‘_1 i7..-_) ... ”“e t ” “PP9arance of‘ :1 ~ .- J ‘ {Tani}? area 43. i 14 O ’1" ‘ - - "\ ~ ‘-1 (JIM; 0 .llf‘t ln “—1- ) J " () (‘1'1 ' ‘ _ / ,u__ 1‘W1L.)pg 1n. . x.’ "1 " “'- M.u'3 dra'cwn‘ “no - - H, A ,‘1 - o l' . -3 r 3- .. , rr ._ -. _l_ ... .- _ ..TH .43: . ‘ 3: 7'1) J‘fi ,‘ 1' r4!“ IJ (~0(‘\|"'m . \J utJC') ' F ".-'1‘ J‘L'v’l‘. TESTS ON THE LARGE CYLIHDERS Procedure: Bars of medium carbon steel from the heats shown in Table II were obtained from various steel mills in order to introduce the variables, due to different heats, met with in industrial practice. Samples were cut from each of these bars to be used for metallographic specimens and to be sub- jected to the various heat treatments used during this study. Two four-inch lengths were cut from each bar and the remainder was forged to about a 2 inch round bar. The four- inch lengths were normalized at 900°C for 1% hours after which the ends were machined parallel, with a very fine finish cut, and the diameters were machined to within 1/10000 of an inch of being perfectly round. These pieces will hereinafter be referred to as the large cylinders. They were accurately measured by four independent read- ings taken of both length and diameter at approx'mately 90O intervals. Two such sets of readings were taken on each cylinder at different times prior to any heat treatment. After the observer acquired the technique, the dimensions could easily be read within l/10000 inch of a previous reading. The Brinell hardness was taken of each cylinder. The large cylinders were heated to 850°C and held for 1% hours in the controlled atmosphere electric furnace. After being prOperly heated, the cylinders were quenched at the rate of |.| .H‘ 40.. one a minute, in water kept at nearly constant temperature (16°C) by a steady stream of fresh water. The dimensions of the quenched cylinders were obtained as soon as the steel had reached room temperature, about 20°C, at which temperature all of the volume measurements were made. The dimensions were measured to the degree of accuracy previously described. The Brinell hardness was read on each cylinder. Within 1 hour after quenching each cylinder had been measured and heated to about 260°C to relieve the stresses set up in quenching. The cylinders were tempered at 595°C for 1% hours in a controlled atmosphere electric furnace and allowed to furnace cool in this atmOSphere to about 150°C. The dimensions of the tempered cylinders were obtained as before, two complete sets of readings having been taken. The Brinell hardness was read on each cylinder. Discussion of Results: The volume changes referred to in this work are eXpressed in per cent of the original volume, and are all positive unless otherwise indicated. Table IV shows the results of the tests on the la ge cylinders when hardened and tempered, and the results of the impact tests on the same steels forged and machined to impact specimens and subjected to the sane heat treatment as the large cylinders received. ..- 0 III 316‘14 .um DRIVE. . - v LIL. TAB 3 IV RESULES 0T TESTS 0] LARGJ CYLINDERS ND IXPACT BARS Steel Grain Brinell Increase in Volume Izod Cracking_in No. 813 Hardness Hardefied' Tempered Impact Large ImpaEt Quenched (595°C) Value Cyl. Bar __. _ 53 .11 % ft.1bs. 51 2-5 555 .181 .058 71.6 Yes 'Yes 42 '2-4 514 .150 -.0504 69.6 Yes Yes 45 1-5 555 .150 .0518 58.9 Yes Yes 59 2-5 555 .175 .154 75.5 Yes Yes 41 5-5 555 .181 .077 77.1 Yes Yes 46 £15 514 .174 .058 55.5 Yes Yes 40 Efé 413 .0718 .055 75.1 Ves Yes 58 4f§~6 444 .104 .072 75.0 Yes yes 54 4-gr6 477 .152 .067 84.3 To 33 44 5-6 565 .004 .048 85.4 ho NO 45 512 555 .0658 .055 81.5 Ho Ho 56 .2‘7 565 .081 .020 84.9 No No 57 641 err .0756 .044 94.5 Ho No All steels normalizaiat 900°C for 1% hours. All steels tempered to a hardness of 212 to 229 Brinell. Original hardness on all steels about 179 Brinell. Cylinders 2.2 to 2.4 inches in diameter and about 4 inches lone. " U .....PCAV p . a .fill a... .0 V5! ... . .. I .3: I .1I‘ . .1; I! I. \I Lvn. I'lIo‘. . .0 .ll « .... Classifying the steels with respect to grain size, steels Nos. 51, 42, 45, 59, 41 and 46 are considered as coarse grained. Steels Nos. 40, 58 and 54 all exhiiit a duplex grain size, but of the th ee mentioned ho. 40 seems to have a more truly duplex structure than do the other two. No. 40 had both Ho. 2 and No. 6 grains present, while Nos. 58 and 54 both show mostly No. 5 with some No. 4 and No. 6 present in each. Steels hos. 58 and 54 might be considered as being on the borderline between corase ahi fine grained steels. Steels hos. 44, 45, 56 and 57 are all fine grained U Considering the relationship existing between grain size and increase in volume on hardening, it is seen that the coarser grain size is associated with the greater increase in L volume. The per cent expansion is of the same order of L ..4. magnitude for all of the coaese grained steels. The f’ne ! grained steels show a lower percentage increase in volume on hardening.. Steels having a duplex grain size, as steel I0. 40 with grain size No. 2 to to. 6, may show the eXpansion 1‘ characteristics 01 either a coarse or fine grained steel. Those steels, Nos. 54 and 58, which lie midway between coarse and fine grain classification show a smaller increase in volume than do the trul* c arse grained steels. The preceding observations are clearly indicative of the greater tendency of the coars- grained steels to eXpand on hardening the degree of eXpansion increasing with the increase in grain size, excepting, of course, those steels diich shov e characteil.t°cs and.which may act as either N duplex grain si coarse or fine rained steels in some of their preperties. The tendency of coarse grained steels to mlow a hiCh de cgiee of eXpansion indicates that they are much more subject to warpage and distortion upon hardening than are the fine grained steels. Likewise, there is a definite relation hip between grain size and surface Brinell hardness of the steel in the hardened condition. From Table IV it is evident that a coarse grained steel is associated with the hi her Brinell hardnesses, (514 to 555) and the fine graized steel with Brinell hardness of 565. Here again the d.uplex grain steels e: {hibit hardne values betw en those of the coarse and the fine grain steels. Davenport and Bain(5) and others have shown that coarse grained steels possess greater hardenability than steels hav- ing a fine grain. The hardening power s directly measured by the Brinell reading and also by the eXpansion. Bain and V.'aring(6) make the following statements concern win the densi- ties of the various constituents in steel. "Carbides are the most dense, austenite somewhat less dense, and martensite the most voluminous. Ordinary ferrite lies between austenite and martensite as does also the mixture of ferrite and carbide found in annealed steels." Steels which have the grea ater ha rdenability would show a greater preportion of martensite when hardened and since martensite is the most voluminous constituent produced in quenching it is logical that the coarse grained steels, which show the higher Brinell hardnesses, should also show a greater degree of eXpansion than the fine grained steels. The per cent volume change in the tempered condition did not seem to have any relationship to the grain size. The greatest inconsistencies were found in the coarse grained steels in the tempered condition, Ho. 42 showing a decrease in volume of .OSOdfi over the volume in the normalized condi- tion. It may also be observed that fine grained steels show greater consistency in volume changes than do coarse grained steels, the variation being from .029% to .055% Another interesting relationship may be pointed out between grain size and the tendency toward cracking when the steels are hardened and tempered. The various steels were all heated at 850°C and quenched into water at about 16°C as previously described. Table IV shows a definite relationship between the grain size and cracking tendency. All of the large coarse grained cylinders showed varying degrees of cracking when quenched. Steel Ho. 40 with a duplex grain showed decided cracking and in this respect is typical of a coarse grained steel whereas its volume change and Brinell hardness were more like that of a fine grained steel. Steels 58 and 54, both coming under the duplex classification, again exhibited the preperties of steels on the "borderline”. Ho. 58 cracked decidedly while Ho. 54 showed no visible cracking whatever. This emphasizes the point that steels showing a duplex grain size are inconsistent in their preperties and may act either as typically coarse or typically fine grained steels. I [O C) I None of the fine grained steels showed any tendency toward cracking. This observation suggests that coarse grained steels are either more sensitive to heat treatment or that they have inherent characteristics which give rise to quenching cracks. Herty(l) claims that coarse grained steels have a lower transformation termerature and a relatively lower transform- ation rate than do fine grained steels. It is therefore necessary that they be treated in a limited temperature range. It may be that the hardening temperature used in this study was not suited to the coarse grained steels. 'It is worthy of note to state that those steels which cracked most severely were Nos. 51 and 42 in which the smallest grain size was No. 4. The cracks in the large cylinders were all circumferential and of about the same intensity with the two exceptions just mentioned. A typical crack is shown in Fig. 14, page 19 of this paper. The tendency of the coarse grained steels toward cracking was not confined to the large cylinders, but was also observed in the impact specimens. It is interesting to note that ‘gll of those steels which cracked in the large cylinders also cracked in the impact bars; and those steels which did.22§ crack as cylinders showed no signs of cracking as impact Specimens. The agreement in this reSpect was perfect. The impact bars and cylinders were all quenched from the same temperature. This seems to be positive proof that the tendency to crack on quenching is inherently in the steel Q for it is not altered oy the forging Operation. §pmmary of Tests on Large Cylinders: The preceding observations on the large cylinders may now'be smmnudzed.as follows: 1. When steels of practically the same chemiea analysis are hardened the coarse grained steels may be expected to show large volume changes and high surface Brinell hardness and to exhibit a marked tendency toward cracking or distortion. The fine grained steels when hard- ened may be ex acted to show small volume increase, lower surface hardness, and no cracking or distortion. 2. The grain size of the steel has little effect on the volume change in the tempered condition. Generally, the fine grained steels show greater consistency of volume change in the tempered condition than do coarse grained steels. 5. A steel having a duplex grain size is inconsistent in its behavior, and may exh bit the characteristics of either a coarse or a fine grained steel. Some of the preper- ties may be consistent with those of fine grained steels while other properties are characteristic of coa se grained steels. Steels having a grain size midway between the coarse and fine classification are quite consistent in their eXpansions and Brinell hardnesses, but may differ markedly with respect to cracking tendency and impact value. TESTS ON THE IKPACT SPECIKEH Procedure: The & inch forged bars were normalized at 900°C for one hour and two round Izod impact specimens were machined from each. The impact Specimens were heated at 850°C for one hour, water quenched and immediately tempered at 5950C for one hour. Rockwell hardness readings were taken in both quenched and tempered condition. The impact values, six in all, were obtained on an Izod impact tester. Discussion of Results: The Izod impact values are included in Table IV. It is doubtful if some of these values can be interpreted very well since a number of the specimens were cracked longitudinally, and the impact values determined on the cracked sections are apt to be in error. In steel Ho. 58 one of the impact Spec mens was cracked and the other was not, yet the impact values were the same on all of the six breaks obtained as is shown in Table V. 1 ES*LTS 0T IHPACT TFSTS OH STEEL N0. 58 - TEHPERED 5950C. Break Ho. 1 2 5 4 5 6 Avg. Impact value ft.lbs. 76 77 77 76.5 76.5 75.5 76.1 Breaks 1, 2 and 5 were on uncracked bar, while breaks 4, 5 and 6 were obtained on longitudinally cracked bar. ..l.‘ O 1'.’ to This may indicate that longitudinal racks do not materially affect the impact values, but it is better to interpret the values on the cracked pieces as being subject to error. The impact values of such specimens varied from 55 to 77 foot pounds, all of the steels being coarse grained. The impact values for the fine grained steels are reliable since no cracks were revealed in any specimen. Steel No. 57 with he. 7 grain size, showed the highest impact value, 94.5 foot pounds. The other fine grained steels, with mostly No. 6 grain, showed impact values of from 81.5 to 86.4 feet pounds. This indicates the higher impact value for the Smaller grain though the data is rather meager. Steel No. 40 with a duplex grain structure, showed cracks in the impact specimens and the impact values were consistent with those of the coarse grained steels. Steels hos. 54 and 58 again showed the peculiarities of a duplex structure. Ho. 54, which did not crack, gave an impact value of 84.5 foot pounds, while Ho. 58 showed consistent impact values of 76 foot pounds even though one Specimen cracked and the other did not. Summary of Tests on;the Impact Specimens: The results of the impact tests are summarized as follows: 1. Higher impact values are associated with the fine grained steels. 2. Cracking in the im act specimens is associated with coarse grain size. 5. Steels showing a duplex grain size may have impact values typical of either coarse O r fine grained steels. 4. In steel No. 58, at least, the impact values are consistent even though one specimen cracked longitudinally. m ("m lens 01: T1113 SInLL cmnmms 1 Procedure: The small test cylinders were machined from the forged stock remaining after.the impact Specimens were made. The small cylinders varied from .625 to .750 inch in diameter, and from 1.70 to 2.20 inches in length. They were measured in the same manner and heat treated under the same conditions as were the large cylinders. All hardness determinations were made with a Rockwell tester in order that the sample should not be made unfit for subsequent measurement. Discussion of esul s: Table VI shows the results of tests on the small cylinder. A survey of this table reveals that the increase in volume on hardening is much greater in the small cylinders than it was T in the larger samples. For example, steel Lo. 59 showed an increase of 1.545 in the small cylinders and.l75% in the large cylinders. Similarly steel ho. 41 expanded 1.1265 in the small cylinders and .181% in the larger pieces. Both of the steels just mentioned are coarse grained and as such would possess good hardening preperties. The small cylinders would harden more completely because of the reduced cross section, and a greater prOportion of martensite would ’- .9 Ho . .L. . mar t0 [1 S (D be produced than in the larger sections. Sine is the most voluminous constituent(6) in the structure it is reasonable to eXpect a higher percentage of volume increase in the smaller cylinders. Genera‘lv, the fine grained steels showed the lower volume increase, but several inconsistencies are apparent. TABLE VI RESL.TS OF TESTS Oh SHALL CYLINDERS Test Grain Rockwell Diam. Volume Charges, per cent Steel Size Hardness inches -T§fiifi§i§i‘ Tempered” 1'10 - “wheels-Casi“... .. 1-.-- *N51 ‘2-5 59 .750 .852 .595 N42 {2-4 59 .687 .800 .561 N52 5 54-57 .688 .555 .581 52 5 55 .662 .700 .425 N45 1-5 58 .750 .608 .162 N59 2-5 61 .750 1.540 .504 N41 [5:5 58 .750 1.126 .527 N40 [216 55-60 .687 .016 .519 N58 475-6 49—58 .688 .996 .505 N54 412-6 55-57 .750 .644 . 55 T45 516 60 .750 .906 .507 N56 6-7 57-60 .625 .667 .236 56 6-7 57-61 .685 .651 .552 4A _‘ A O ‘«_W. *”N” indicates samples normalized at 900°C for one hour. Rockwell Hardness as tempered - C22 to 28. The results in Table VI on volume increase in the hard- ened condition is not of much value. The diameters of the cylinders varied from .625 to .750 inch, depending on the diameter of the forged piece. It is common knowledge among steel treaters that a sample in this diameter range is on the borderline between complete and partial hardening throu3h the section. Such being the case, it is not advisable to rely upon the volume chan3es .iven in Taole VI, because some. of tile sections may have hardened CONlpthGl y throu3h the section, while others were only partially hardened. The variations in diameter, and this particular diameter intro- duce what mi3ht be termed a "dimensional problem", vfhich has not oeen inves i3ate1 in this work. There was no apparent relationship existing between grain size and Rockwell "C" hardness, probably because all of the steels hardened thoroughly at the surface regardlw of the grain size Likewise, there is no relationship between grain size and volume change in the temp red steels. Both cylinders of steel No. 42 showed H1i3“ cracking when water quenched from 850°C, being the only steel to show crackin3 under three conditions. Sunmarv of Results on .——.—.!L._._.. A .r *-—.— *H-u- 1. The per cent volume increase on hardening is much greater in the small cylinders than in the larger sections. 2. The lar 3est ex pansions, (1.545 and 1.1265) occur in coarse grained steels. 5. Grain size bears no relationship to Rockwell "C" Q hardness in the Lardened cylinders of the diameters used. 4. The diameter of cylindzrs used in this study was such as to introduce a ”dimensional problem” and leads to inconsistencies in the results obtained. 5. There is apparently no relationship between the grain size and the volume changes in hardened or tempered conditions (in the chosen diameter ran3e). CONCLUS IONS 1. Fine grained steels may be expected to show high impact values, low volume changes on quenching (which are indicative of a low degree of warping or distortion) and no cracking on quenching and tempering. 2. Coarse grained steels may be GXpOCted to show lower impact values, a decided cracking tendency on quenching and tempering, high surface hardness and large Xpansion on hardenins indicating that they are subject to warpage or distortion. 5. Duplex grain steels are inconsistent in their prOp- erties and may exhibit the characteristics of either coarse or fine grained steels. 4. The Specifications for a particular part, based on the results of this study may be stated as follows: If the part were required to have consistently good toughness, as is indicated by impact value, a low degree of eXpansion or distortion, no cracking tendency when quenched, and/or good 5 forging prOperties, a steel of grain size greater than No. ioult be Specified. 5. All steels showing a duplex structure or grain size below No. 5 should be rejected. 6. If high surface hardness is most desired, without regard for distortion or cracking, a steel of a larger grain than No. 5 should be specified. Duplex structures should not be accepted. 4. BIBLIOGRAPHY Deoxidation of Steel - C. H. Herty, Jr. Transactions A.S.H., Vol. XXIII, Narch, 1955. The Effect of Furnace Atmospheres on Steel - R. G. Guthrie Transactions A.S.S.T., Vol. XV, January, 1929. U. S. Bureau of Nines Bulletin #296, pp. 7, 55, 81-2, 95-6 Iron Oxide Reducation unlibria A critique from the standpoint of the phase rule and thermodynamics. Inclusions in Steel - Urban & CLipnan Transactions A.S.N., Vol. XXIII, March, 1955. General Relations Between Grain Size & Hardenability & he Normality of Steels - E. S. Davenport & E. C. Bain Transactions A.S.N., Vol. XXII, December, 1954. Austenite Decomposition & Length Changes in Steel - E. C. Bain and W. S. N. Waring Transactions A.S.M., Vol. XV, Januawv 1929. "d’ m1|milHamlinIgutguljlflluliltltmlilillnu1