• Tidak ada hasil yang ditemukan

on G TiC-Ni

N/A
N/A
Protected

Academic year: 2024

Membagikan "on G TiC-Ni"

Copied!
7
0
0

Teks penuh

(1)

on G TiC-Ni

3

Al Cermet

Ji Heon Kim and Wan Jae Lee

Department of Metallurgy and Materials Science Engineering Hanyang University Ansan, 425-791, Korea (Received 24 September 2002 ; Accepted form 16 October 2002)

Abstract The effects of boron or manganese added as B4C, Mn, TiB2, B on TiC-30vol.%Ni3Al cermet sintered at 1380 and 1400oC for 1 hour, were examined in relation with shrinkage, relative density, microstructure, lattice parameter, hardness and fracture toughness (KIC). The results are summarized as follows: 1) The highest shrink- age showed about 30.5% in the specimen added B4C and the maximum relative density was about 99% in the specimen added TiB2; 2) The grains of TiC were grown during sintering and made the surrounding structure by adding boron and manganese. The largest grain size showed about 2.8µm in the specimen with boron sintered at 1400oC; 3) The lattice parameter of TiC was about 4.325Å and Ni3Al about 3.592Å by adding other elements; 4) The highest hardness was about 1100 kgf/mm2 in the specimen with B4C; 5) The fracture toughness (KIC) showed about 15 MNm-3/2 in the specimen added TiB2.

Keywords : Cermet, Ni3Al, TiB2, Microstructure, Hardness.

1. B †

TiCê Žš WCê .ã.ö j~ .ÓW"

ÚÖzWf Ö>~æò “.K" žWš ÔjB "

‚ .Ó ’Ïb‚ ‚;>Ú ÒÏ> ®j ö, Ú îÎÒò ~ æ ª¢ö ÒÏ>æ á~º 6j B F~¶ Öçž Ni 6º Ni-Co¢ &چ bî‚

B NÒòž Ni3Al .³*zbš &ˆ ©b‚

6>î. &¶ f TiC-Ni3Al Ž~ ֏ç ï,

²Ö Nêf *, Ò ê² 5 Mo2C Î& ö

&‚ ’¢ >¯~, Ûç~ ‡ç ²Ö‚ ~&‚

²ÖÚ¢ B–† > ®b–, ßWê Vš~ TiC- Niêf F҂ Ö"¢ áî1,2).

Ni3Al .³*zbf L12 Ö;’–š– ;ê&

800oCræ Nê ~šWb‚ Ã&~, NöB Ú ÖzW, ڒãW, ÚÏÏW š Ö>~–, Wf

Ž«; ö²‚ Bj, ~~; ö²‚ Mnj ²ï Î&

~š BFB rJ^ ®3,4).

’öBº TiC-Ni3Al Ž~ W" žWj BF† Ï'b‚ »²(B)¢ '' ž ;ž TiB2, B4C, Bf *(Mn)j ²ï Î&~ .~ ^–

ç" Vê' ßWö ~º 'Ëj –Ò~&.

2. þ O»

öòªö‚º TiC(Herman Stark Co., «ê £ 1.4 µm), Ni3Al(X-form Co., 44µm š~), B4C(Herman Stark Co., 1.5µm), TiB2(Herman Stark Co., 1.5~

2.5µm), B(Herman Stark Co., 4~8µm), Mn(Kanto Chem. Co. £ 2µm) ªöj ÒÏ~, TiC-30vol.%- Ni3Al~ ¢;‚ –Wb‚ ~ Ni3Al ïö &~

0.3 wt%~ B4C, TiB2, B 5 7.5wt%Mnj Î&~

(2)

V~&. Fig. 1f *Ú þ";j BÛ'b‚ ‚

~&.

' –W~ ªöj FW"&V(Planetary Mill)öB 10* ÿn Û"&j ‚ ê ê J6öB š–

~&. š–B ªöj 100 MPa~ {Kb‚ W;~

, £ 5Ü10-2Torr~ ê 7öB 1380oCf 1400

oCöB 1* ÿn ²Ö~&. š ' –W~ ²Ö Úö &~ š' >»†" &ê(ASTM B 328)¢

G;~&. ' ²ÖÚ~ ^–çf šjÒ F

" ¾Êނ î‚ ê FE-SEM(JEOL Co. JSM- 6330F)j ÒÏ~ &V~&. Ò TiC «¶’V º Image Analyzer¢ ÒÏ~ ’~&. 6‚, XRD(Philips Co. PW1730)‚ –ç 7ö î‚Ú ç

~ Â*¦f TiCf Ni3Al~ ϶;>¢ G;~&

. Vê' W jÊãê¢ ~7 50 kgb‚

G;~&b–, žWf Palmqvist Toughness Test O

»5)b‚ ãê {z F~ crack ^š¢ G;~

2ZžW(KIC)j ’~&.

3. þÖ" 5 V

ÖF Fig. 2ö TiC-30vol.%Ni3Alö æWª(B4C, Mn, TiB2, B)j Î&‚ ²ÖÚ >»†" ç&&êf

~ &ê¢ ¾æÚî. Fig. 2öº jv¢ *~ æ Wªj Î&~æ pf Þ~ Ö"ê ÷V~&. ¢

>'b‚ >»†f æWªš Î&>æ pf Þö Bº 1380oCöB £ 27.6%, 1400oCöB 29.6%‚

²ÖNê& ¸bš çß~&. ¾ B4C, Mn, TiB2, Bj ²ï Î&‚ ãÖöº ²ÖNê~ Nšö

~‚ >»†~ Nšº Ö 'îb–, '' £ 31,

29.8, 29.3, 27%‚ š 7öB B4C¢ Î&‚ ãÖ

&Ë ¸² ¾æÒ. ²ÖÚ~ ç&&êº Mnj Î

&‚ ãÖö jv' Ô² ¾æÒb–, TiB2¢ Î&‚

ãÖö &Ë ¸² ¾æÒ. &Ë ¸f ç&&ê¢

¾æÚº ©f TiB2¢ Î&~ 1380oCöB ²Ö‚

ãÖö £ 99%‚ ¾æÒ. TiB2¢ Î&~&j r Î&~æ pf Þ ç&&ê& ¸jæº ©j r > ®î.

rb‚ æWª Î&ö Vž .~ SEMö ~‚

^–çj Fig. 3ö ²ÖNêf~ &ê‚ ¾æÚî . æWªš Î&>Úê TiC «¶º ;çš ';b

‚ ·f «¶f – «¶š b>Ú ®b–, – «

¶~ ãÖº ²Ö 7ö WË~ «¶ 7¦f ž

¦öB «z~ Nš‚ ¾æÒ. š‚ *çf Mn j Î&‚ ãÖö z× F«~² ¾æÒ. ÿ¢ – W~ .öBº ²ÖNê~ Nšö ~‚ ^–ç ç~ æzº «{® ’ª>æ p~.

Fig. 3~ ^–çöB Image Analyzerf Fullman

~ 6)j ÒÏ~ TiC «¶~ ï ’V¢ G;‚

Ö"¢ Fig. 4ö ‚~&. TiC «¶~ ï ’V º æWªj Î&~æ pf .(â 7 Free)"

B4C, Mn, TiB2, B¢ Î&‚ .~ ãÖö 1380oC

²ÖöB '' £ 1.2, 1.65, 1.9, 1.85, 1.6µmb‚

MnÎ& .öB ‚&‚ ¾æÒ, 1400oC ²Öö Bº '' £ 1.58, 2.1, 2.4, 2.5, 2.8µmb‚ BÎ

& .öB ‚&‚ ¾æÒ. ÿ¢ ²ÖNêöB æ Wªš Î&>æ pf .ö j~ æWªš Î&

Fig. 1. Flow chart of experimental procedure.

Fig. 2. Relative density and shrinkage of TiC-30vol.%- Ni3Al cermets in relation with other components and sin- tering temperature.

(3)

Fig. 3. SEM microstructures of TiC-30vol.%Ni3Al cermets in relation with other components and sintering temperature.

(4)

>š TiC «¶~ ï ’V& Ã&~&. 6‚ ÿ

¢ . –WöBº ²ÖNê& ¸bš «¶W˚

¢Ú¾ ï TiC «¶~ ’Vº Ã&~&. ¢>' b‚ TiC-Mo2C-Ni ŽöB~ «¶WËf ²Ö 7 ö TiC«¶ "*ö "æ–ç(surrounding structure) j ;W~šB ¢ÚÂ. TiC-Ni3Al ŽöBê æW ª Î&öB "æ–çš &V> ®bæ‚ «¶W Ë V’º TiC-Mo2C-Ni Ž~ ãÖf ÿ¢ † © b‚ ÒòB. ¯, æWª Î&ö ~~ ‡ç Â*

Nê~ æz, ‡ç" TiC «¶ êšöB~ C V

’f ‡çöB~ {Ö ³ê š TiC «¶~ Ϛ- CÂö ~‚ Ostwald WËö 'Ëj V r^š

¢ 'B. »²& ŽFB B4C, TiB2, B& Î&

B .~ ãÖöº ²Ö ‡ç Â* Nê& Ô~

V r^š¢ ºGB. šº ²Ö ßN ";öB Î& bî 7ö Bö¶& ‚š {Öö ~~ Ni3Al

«¶ ‚šöB Ni" B ö¶& ֏>š Ni-B ç ê7)öB r > ®º :f ?š ‡çš jv' Ôf NêöB W>šB Ni3Al «¶~ Ϛ& Ô f NêöB ¢ÚÒV r^š¢ 'B. 6‚

Mn Î&~ ãÖê çVf FÒ~² Ni-Mn çê7) öB Ni 7ö Mnš Ã&>š [6š Ôjææ‚, Mn ê Ni3Al~ ϚNê¢ ÔºV r^š¢ ' B. Ò š Î& Wªš ‡ç 7ö Ϛ>Ú

®bš TiC «¶~ Ostwald WËö ÚÊ ;‚

&®j ©b‚ Òò>– ;ï'ž ï&º Ö Ú [. 1400oCöB TiB2f B Î&ö ~~ TiC «

¶ W˚ 1380oCö j~ *&~² Ã&‚ ©f

‡ç" TiC «¶ êšöB ‡ç 7ö Ϛ>Ú ®º Ti, C, B ö¶~ ‚zK" ‡ç 7~ {Ö ³ê&

Ã&®V r^š¢ 'B.

rb‚ æWª Î&‚ ²Ö 7ö B2ç~ Â*

¦¢ –Ò~V *~ Cu Kαö ~‚ X-F ².

þ Ö"¢ Fig. 5ö ‚~&. ' ²ÖNêöB

².NZf æWªj Î&‚ .š¾ Î&~æ p f .(â 7 Free)öB ÿ¢~² ¾æÒ. V¢

B .ö Î&‚ æWªf ²Ö 7ö TiC¾ Ni3Al 7ö *¦ Ï>î 6B.

Fig. 6ö æWª Î&ö ~‚ TiCf Ni3Al~ ϶

;>¢ ’~ ‚~&. Fig. 6(a)öB TiC~ Ï Fig. 4. TiC particle size of TiC-30vol.%Ni3Al cermets in

relation with other components and sintering tempera- ture.

Fig. 5. X-ray diffraction patterns of TiC-30vol.%Ni3Al cermets in relation with other components and sintering temperature. (a) sintering at 1380oC and (b) sintering at 1400oC.

(5)

¶;>º 1380oC ²Ö~ ãÖ æWª Î&~æ pf

.~ ãÖ £ 4.334ÅöB æWª B4C, Mn, TiB2, Bš Î&>š £ 4.327çb‚ Ôjr. ¾ 1400oC ²Ö~ ãÖº Î&~æ pf .~ ãÖ

£ 4.318çöB B4C Î&~ ãÖº £ 4.320çb‚

£* Ã&>, Mn, TiB2, B Î&~ ãÖº £ 4.325çb‚ –~ FÒ~&. VB æWªš Î&

>æ pf .öB TiC~ ϶;>& ²ÖNê æ zö ~~ – N𢠾æÚ ®. ¢>'b‚

TiC~ ϶;>º ϶ 7~ ê²ö¶~ Žê" î êö ~~ æz‚. 1380oC ²Ö~ ãÖº TiC

«¶ 7~ ê²ö¶& Ni3Al ֏çb‚ {֚ ' îV r^š–, 1400oC ²Ö~ ãÖº {֚ ¢Ú

¾ îêš >ÚB ϶;>~ æz& ¢ÚÒ 'B. æWª Î&‚ ãÖö TiC~ ϶;>& ² ÖNêf ç&ìš –~ ¢;~² ¾æÂ ©f, Î&

ËçÎ ~ ®3). V¢B B& ŽFB Wªf Ni3Al~ ϶;> æzö ’² V~æ á

~&V r^ö –~ ¢;~² ¾æÒ 'B.

¾ Mn Î&~ ãÖº ²ÖNê 1380oCöB £ 3.597çš, 1400oCöB £ 3.578çb‚ – Nš¢

š ®. Mnš Ni3Al ֏çö ~~;b‚ Ï

>æ‚, L12 Ö;’–ž Ni3Alf šö Niö¶&, Sæ6ö Alö¶& *~~ ®ÚB, Mnö¶& ÚÊ ö¶f~ ~~ &ËWf ö¶ ’Vf &ê ®j ©

š. ö¶>ãf Mn, Ni, Alš '' 1.37, 1.25, 1.43çšæ‚, Ni3Al~ ϶;>º Mnš Ni" ~~

>š Ã&~ Al" ~~~š 6²† ©b‚ 6B . V¢B Ni3Al~ ϶;>& 1380oC ²ÖöB Ã

&‚ ©f Mnš Ni" ~~>, 1400oC ²ÖöB 6²‚ ©f Mnš Al" ~~~&V r^š¢

'B. ¾ 1380oCöB Mnš Ni" ~~ ¦º 6~V ÚJ֖ .êö ҦƢ º‚.

rö Vê' Wî‚ TiC-30vol.%Ni3Al Ž~

ãêö ~º æWª Î& 5 ²ÖNêf~ &ê‚

Fig. 7ö ‚~&. .~ ãêº 1400oC ²Ö~

ãÖ æWª Î&~æ pf ., B4C, Mn, TiB2, B Î&.öB '' £ 985, 1103, 1080, 1070, 1095 kgf/mm2b‚ æWª Î&~ ãÖö ¸² ¾æ Òb–, ß® B4C Î&~ ãÖ& ‚ 8j ¾æî . 1380oC ²Ö~ ãÖº ãËf FÒ~¾ £* Ô

² ¾æÒ, Mn" TiB2 Î&¢ Bž~š ²ÖNê Nšö Vž ãê~ Nšº –~ ìî. Mn"

TiB2~ ãÖº Mn" Tiš Ni3Al 7~ Al" ~~~

Ï>Ú ;z>îV r^ö ²ÖNê& ¸j>

ƒ Ïïš Ã&~ ãê& ¸jr 'B.

. ãê& B4Cf B¢ Î&‚ ãÖö jv' ¸²

¾æÂ ©f Cö¶~ Ni3Alö Ž«; Ïö ~‚

Ï;zf Bö¶~ «ê ;zö ~‚ ©b‚ ºG Fig. 6. Lattice parameter of TiC-30vol.%Ni3Al cermets in

relation with other components and sintering tempera- ture. (a) TiC lattice parameter and (b) Ni3Al lattice para- meter.

(6)

B.

TiC-30vol.%Ni3Al Ž~ 2ZžW(KIC)j Palmqvist Toughness Test O»5)b‚ ãêG; ê {z F~

crack ^š¢ G;~ r b‚ 2ZžWj ’~

&.

(1)

VB, Aº ç>(0.0028), Hº ãê(N/mm2), P º ~7(N), Σlf ãê {z F~ ’¿^š~  (mm)š.

Fig. 8ö TiC-30vol.%Ni3Al Žö æWª Î&f

2ZžW(KIC)"~ &ê¢ ¾æÚî. ¢>'b‚

KIC 8š ¸j>ƒ .~ žWš ¸f ©j ¾æÞ . Mnj Bž~º æWª Î&‚ žWš Ëç>

î. ‚~ žW8f TiB2¢ Î&‚ ãÖö ²ÖN êö ç&ìš KIC 8š 14~15 MNm-3/2& áÚr.

Bf Ni3Al~ žWj ËçÊæ‚ Bš ŽFB TiB2

º TiCf Ni3Al~ êš~ ֏j ;z~ ~

*2¢ ÛB~&V r^ö 2ZžW𠏲 ¾æÒ 'B.

4. Ö †

TiC-30vol.%Ni3Alö æWªb‚ B4C, Mn, TiB2, Bj ²ï Î&~ 'Ëj ²ÖNêf~ &ê‚

–Ò~ r" ?f Ö"¢ áî.

1. ²ÖÚ~ š' >»†f B4C¢ Î&~

1380oCöB ²Ö®j r £ 30.5%‚ &Ë ¸~b–, ç&&êº TiB2¢ Î&~ 1380oC‚ ²Ö~&j r £ 99%‚ &Ë ¸² ¾æÒ.

2. ^–çöB TiC «¶º ';š–, ²Ö 7ö

«¶W˚ ¢Ú¾B «¶"*f 7¦º «z~ N

š& ¾æÒ. «¶WËf ²ÖNê& ¸bš z×

«{® &V>îb–, TiC~ ï«êº 1400oC ² Ö~ ãÖ æWªj Î&~æ pf ãÖ,

B4C, Mn, TiB2, B Î&BB‚ '' £ 1.58, 2.1, 2.4, 2.5, 2.8µmb‚ B Î&~ ãÖ& &Ë –

&~&.

3. æWª Î&ö ~‚ –ççö B2ç~ Âf

&V>æ p~b–, XRD ².NZöBê TiCf Ni3Al ç~ ².b’ò ¾æÒ. æWª Î&ö ~

‚ TiC~ ϶;>º 1400oCöB £ 4.325çb‚

FÒ~&b–, Ni3Al~ ϶;>ê Mn Î&~ ãÖ

¢ Bž~ £ 3.592ç‚ FÒ~&.

4. ãêº B4C¢ Î&~ 1400oCöB ²Ö~&j ãÖö ‚& £ 1100 kgf/mm2& áÚr.

5. 2ZžW(KIC)f Mnj Bž‚ æWª Î&‚

Ëç>îb–, ‚~ žWf TiB2¢ Î&‚ ãÖö

²ÖNêö ç&ìš £ 14~15 MNm-3/2& áÚr.

^^ò

1.¶^", šjÒ: ‚“ªö¢.²æ, 5 (1998) 286.

Kpj A H P Σl ---

=

Fig. 7. Vickers hardness of TiC-30vol.%Ni3Al cermets in relation with other components and sintering tempera- ture.

Fig. 8. Toughness values of TiC-30vol.%Ni3Al cermets in relation with other components and sintering temperature.

(7)

Referensi

Dokumen terkait

The steel changes its structure fro a body-centered cubic lattice (ferrite) to a face- centered cubic lattice(austenite) at about 720 o C.Austenite is capable of dissolving carbon.

We concluded that there are, at least, two roles of boron addition to CVD-Co/MoS 2 /Al 2 O 3 that is boron weakens the interaction between Mo oxides and Al 2 O 3 surface, promoting

Analytical models of specimen type 3/II, 4/II, and 2/III using SAP2000 Analytical model consists of main reinforced concrete frame, infill wall shell elements, and gap between main

Exchange mechanisms The complex magnetic structures of the lanthanide elements and their alloys derive from the interplay of band structure, crystal field, lattice strain, and the

INTRODUCTION Indonesia has the largest national population in the east equator, but no study about pancreatico-duodenal and pyloric preserving pancreaticoduodenal resections has been

Images of the tetra collapse ratio of 3d mesh elements of a original surface mesh smoothed surface mesh of grain boundaries before quality enhancement, b 3d mesh elements generated

From AFM results, the average grain size of all samples decreases from 158.74 nm to 62.87 nm with the increase of Gd3+ doping ratio, which is attributed to the reduction lattice due to

"The effect of grain mass variations on drying time by adding a pipe heat exchanger to a fluidized bed dryer", AIP Publishing, 2019 1% match Internet from 29-Aug-2022