A N N A L E S
81,9(56,7$7,60$5,$(&85,(6.à2'2:6.$
/8%/,1±32/21,$
92//;9,,, 6(&7,2$$$ 2013
ABSTRACT
Comparison of numerical simulation and experimental data for nanoindentation studies of QDQRVWUXFWXUDOFDUERQDFHRXVSDOODGLXPILOPV&3GLVSUHVHQWHG
)LQLWH(OHPHQW0HWKRG)(0DQG$16<6SURJUDP$QV\V,QFZHUHXVHG7UDGLWLRQDO2OL- ver–Pharr method for cone and spherical shaped indenter were applied for FEM modelling of nano- LQGHQWDWLRQH[SHULPHQW)(0VLPXODWLRQVVKRZHGWKDW3GQDQRJUDLQVDUHPRYHGLQFDUERQPDWUL[
WRZDUGWKHILOPVXUIDFHGXHWRDQH[WHUQDOVWUHVV'LVWULEXWLRQRISDOODGLXPJUDLQVLQWKHILOPYROXPH
LQIOXHQFHRQWKH<RXQJPRGXOXVDQGQDQRKDUGQHVVZDVDOVRIRXQG
,1752'8&7,21
Mechanical properties of new nanomaterials are particularly interesting due WRWKHSRVVLELOLW\LQQRYDWLYHDSSOLFDWLRQV3URSHUWLHVRIVXFKPDWHULDOVRQWKHQD- QRPHWHUVFDOHPLJKWGLIIHUIURPWKRVHRIDEXONPDWHULDORIWKHVDPHFRPSRVLWLRQ
Nanoindentation investigations of films containing Pd nanograins are difficult be- FDXVHWRSRJUDSK\DQGRUVWUXFWXUHRIILOPVDQGFRQWHQWVRI3GLQWKHILOPVVLJQLIL- FDQWO\DIIHFWWKHLUQDQRPHFKDQLFDOSURSHUWLHV6XFKILOPVFRXOGEHDSSOLHGDVDQ
DFWLYHOD\HULQPDQ\W\SHVRIVHQVRUV&3GILOPVFKHPLFDOPHFKDQLFDODQGSK\VL- cal properties depend on palladium nanograins and carbonaceous matrix structure
> @ 2QH RI QHZ PHWKRGV RI LQYHVWLJDWLRQV RI QDQRPHFKDQLFDO SURSHUWLHV LV
QDQRLQGHQWDWLRQPHWKRG7KLVPHWKRGLVGHVLJQHGWRPHDVXUHWKHQDQRPDWHULDO¶V
mechanical properties such as nanohardness and reduced modulus of elasticity
>@,QWKLVWHFKQLTXHWKHLQGHQWHULVSODFHGRQYHU\VPDOOGHSWKLQWRPDWHUDO
)(0DSSOLFDWLRQLQVWXGLHVRIPHFKDQLFDOSURSHUWLHVRIWKH&3G¿OP
-2$11$5<0$5&=<.
7HOH 5DGLR5HVHDUFK,QVWLWXWH5DWXV]RZD:DUVDZ3RODQG (PDLODGGUHVVMRDQQDU\PDUF]\N#LWURUJSO
)LQLWH(OHPHQW0HWKRG)(0LVXVHIXOWRDQDO\]HPHFKDQLFDOEHKDYLRURI
QDQRFRPSRVLWHVWKLQILOPVDQGELRPDWHULDOV,QWKLVSDSHUDVWUXFWXUDOPRGHORI
film composed of palladium nanograins embedded in carbonaceous matrix is pre- VHQWHG7KHPRGHODOORZVSUHGLFWLQJVRPHPHFKDQLFDOSURSHUWLHVRIWKHILOP7KH
preliminary FEM studies demonstrated that this method can be applied to simula- tion of nanoindentation experiment and is used to fit experimental load-displace- PHQWGDWDIRUQDQRLQGHQWDWLRQWHVW
6$03/(35(3$5$7,21
&RPSRVLWH&3GILOPVZHUHREWDLQHGE\3K\VLFDO9DSRXU'HSRVLWLRQSURFHVV
39'7KLVSURFHVVZDVSHUIRUPHGIURPWZRVHSDUDWHGVRXUFHVRQHFRQWDLQLQJ
C60IXOOHUHQHVDQGRWKHUFRQWDLQLQJSDOODGLXPDFHWDWH39'SURFHVVZDVFDUULHG
out in a dynamic vacuum of ~ 10-5 PEDU7KHGHSRVLWLRQUDWHZDVDERXWQPPLQ
and the temperature of the substrate was 180o&>@)LJSUHVHQWVW\SLFDO7(0
LPDJHRI&3GILOP3DOODGLXPQDQRJUDLQVKDYHDQRYDOVKDSHZLWKDGLDPHWHU
WRQP7KHWKLFNQHVVRIWKHILOPLVaQP3GQDQRJUDLQVDUHRIIFFW\SH,Q
)LJE3G!SODQHVIRUVXFKIFFVWUXFWXUHDUHYLVLEOH
)LJD7(0LPDJHRI&3GILOPEKLJKUHVROXWLRQLPDJHRI3GJUDLQ
7+(1$12,1'(17$7,217(&+1,48(
Nanoindentation experiments were performed using the electrostatic trans- ducer of the Hysitron Nanoindentor Triboscope attached to a scanning force mi- FURVFRSH6)07KHLQGHQWHUFDQEHXVHGIRUVFDQQLQJRYHUWKHVDPSOHVXUIDFH
IRULPDJLQJ,IQDQRLQGHQWDWLRQLVFRPELQHGZLWKVXUIDFHLPDJLQJWKHQQDQRPH- FKDQLFDOSURSHUWLHVFDQEHORFDOO\GHWHUPLQHG7UDGLWLRQDOO\WKHORDGRILQGHQWHUWLS
FDXVHVSHQHWUDWLRQLQWRDVSHFLPHQDQGLQWKLVZD\WLSUHDFKHVDGHVLUHGGHSWK$W
WKLVSRLQWWKHORDGRIWLSFRXOGEHVWDELOL]HGIRUDPRPHQWRUUHPRYHG,QQDQRLQ- GHQWDWLRQVPDOOORDGVYDOXHDQGVPDOOVL]HVRIWLSDUHXVHG7KHQWKHLQGHQWDWLRQ
DUHDPD\KDYHDIHZVTXDUHPLFURPHWUHVRUHYHQQDQRPHWUHV7KHGHSWKRISHQ- etration versus a force is obtained and then the area of the indent is determined with WKHNQRZQJHRPHWU\RIWKHLQGHQWHUWLS$UHFRUGRIWKHVHYDOXHVFDQEHSORWWHGRQ
DJUDSKWRFUHDWHDIRUFHGHSWKFXUYH7KHVKDSHRIWKHFXUYHSURYLGHVLQIRUPDWLRQ
RQPHFKDQLFDOSURSHUWLHVRIPDWHULDOQDQRKDUGQHVVHODVWLFPRGXOXVHWF
The indenter tip is made of diamond and has 90oS\UDPLGVKDSH6FKHPDWLF
JHRPHWU\RIWKHLQGHQWHUWLSLVVKRZQLQ)LJ7KHDQJOHEHWZHHQDQG SODQHVLVo¶¶¶>@
)LJ6FKHPDWLFJHRPHWU\RIWKHLQGHQWHUWLS
,QWKLVFDVHWKHFURVVVHFWLRQDUHDSODQH$('LQ)LJLVJLYHQE\
2 2 2598 2
3
3 K K
$F
)RUFHYHUVXVGHSWKFXUYH)LJSURYLGHVPXFKPRUHLQIRUPDWLRQWKDQDPL- FURVFRSLFLPDJHHODVWLFDQGSODVWLFGHIRUPDWLRQZLWKLQFUHDVLQJDQGGHFUHDVLQJ
ORDGDQGSHUPLWVWRFDOFXODWHQDQRKDUGQHVVDQGUHGXFHGPRGXOXVDVDIXQFWLRQRI
SHQHWUDWLRQGHSWK>@
)URPWKH)'SORWRQHREWDLQIROORZLQJSDUDPHWHUVPD[LPXPLQGHQWDWLRQ
GHSWKKPD[ZKLFKLQFOXGHVHODVWLFDQGSODVWLFGHIRUPDWLRQGHSWKRIWKHUHPDLQLQJ
LPSUHVVLRQDIWHUFRPSOHWHXQORDGLQJKIDQGPD[LPDODSSOLHGIRUFH)PD[%DVHG
RQWKLVGDWDDQG2OLYHU±3KDUUWKHRU\LWLVSRVVLEOHWRGHWHUPLQHWKHQDQRKDUGQHVV
1+DQGUHGXFHWKHPRGXOXVRIHODVWLF(U>@
)LJ3ORWRIIRUFHGHSWK)'SORWGHSHQGHQFH
7KHQDQRKDUGQHVVRIWKHVDPSOH1+LVREWDLQHGIURPWKHIRUPXOD>@
max F F K
$ 1+ )
where )PD[ is the maximum applied force and AF is the cross-sectional area cor- responding to the contact depth KF7KHFRQWDFWGHSWKKFLVJLYHQE\
6 K )
KF max 075 max
where 6LVWKHFRQWDFWVWLIIQHVV
GK 6 G)
with G)GK being the slope of the unloading curve at the initial point of unload- LQJ
The reduced modulus (U is a measure of the elastic properties of the tip- sample system and can be calculated from the force-depth curves according to the IRUPXOD
GK G) K
$
(U 12 S C C
NH
G) GK
G) GK
5(68/76
)RUQXPHULFDOPRGHOOLQJQDQRLQGHQWDWLRQH[SHULPHQW)(0DQG$16<6SUR- JUDP$QV\V,QFZHUHDSSOLHG,QRXUPRGHO&3GILOPLVGHSRVLWHGRQDJODVV
VXEVWUDWHDQGLWLVLQGHQWHGE\PHDQVRIDGLDPRQGLQGHQWHUDVVKRZQLQ)LJ
,QWKHFDUERQOD\HUVSKHULFDOREMHFWVUHSUHVHQWLQJ3GQDQRJUDLQVZHUHORFDWHG
)LJ$[LV\PPHWULFPRGHORIWKH&3GILOPDQGWLS
7KHWKLFNQHVVIRUWKHPRGHORI&3GILOPLVȝPDQGWKHJODVVVXEVWUDWHLV
ȝP7KLVWKLFNQHVVZDVPXFKKLJKHUWKDQIRUUHDO&3GILOPEXWLWZDVQHFHVVDU\
IRURXUPRGHOWRHOLPLQDWHWKHLQIOXHQFHRIVXEVWUDWHHIIHFWVRQUHVXOWV,QRUGHUWR
SURSHUO\VLPXODWHWKHQDQRLQGHQWDWLRQH[SHULPHQWDFRQWDFWDQDO\VLVZDVDSSOLHG
)RUWKLVSXUSRVHFRQWDFWHOHPHQWVZHUHSODFHGDORQJWKHWRSVXUIDFHRIWKHILOP
DQGWDUJHWHOHPHQWVZHUHXVHGDORQJWKHERWWRPVXUIDFHRIWKHWLS7KHFRQWDFWLV
DVVXPHGWREHIULFWLRQOHVV7KHLQGHQWDWLRQH[SHULPHQWZDVVLPXODWHGE\DSSO\LQJ
displacement boundary conditions in the y-direction to the nodes along the upper VXUIDFHRIWKHWLS7KHWRSVXUIDFHRIWKHWLSZDVFRQVWUDLQHGLQDOOGLUHFWLRQV6LQFH
WKHSUREOHPSRVVHVVHV\D[LVV\PPHWU\WKHQWKHPRGHOZDVDQDO\]HGLQRIWKH
JHRPHWU\'LVSODFHPHQWVDORQJWKHV\PPHWU\SODQHVZHUHFRQVWUDLQHG
5DWLRRIQDQRJUDLQVVL]HDQGWLSGLDPHWHUGHWHUPLQHVDVFDOHRIWKHSUREOHP
The plastic deformation after unloading for the model of C-Pd film is shown in )LJD,Q)LJEWKHGLVSODFHPHQWRISDOODGLXPQDQRJUDLQVGXHWRWLSUHDFWLRQLV
SUHVHQWHG7KHFRORUIXOVSKHULFDOVKDSHVVKRZSDOODGLXPQDQRJUDLQVSRVLWLRQDIWHU
WKLVUHDFWLRQ2EMHFWZLWKDJULGGLQJVKRZVWKHSRVLWLRQRI3GJUDLQVEHIRUHWKH
UHDFWLRQLQGHQWHUSUHOLPLQDU\SRVLWLRQ
)LJ0RGHORI&3GILOPDGLVSODFHPHQWYHFWRUVXPIRUWKHZKROHILOPEGLVSODFHPHQW
YHFWRUVXP3GQDQRJUDLQV
Spherical shape of the tip becomes important when one wishes to perform QDQRLQGHQWDWLRQVRQWKLQILOPVZLWKDWKLFNQHVVRIOHVVWKDQQPDQGZKHQWKH
PD[LPXPGHSWKRISHQHWUDWLRQRIWLSLVaQP>@$UHDOLQGHQWHUFDQWKHUHIRUH
EHPRGHOOHGDVDVSKHULFDOLQGHQWHU7KHVFKHPHRIWKHVSKHULFDOVKDSHGWLSLQWKH
VLPXODWHGQDQRLQGHQWDWLRQH[SHULPHQWLVVKRZQLQ)LJ
)LJ6FKHPHRIVSKHULFDOVKDSHGWLSLQWKHVLPXODWHGQDQRLQGHQWDWLRQH[SHULPHQW
In nanoindentation experiment the SFM is used to give the contact area of the WLSZLWKWKHVXUIDFHXVLQJWKHEHDULQJIXQFWLRQPRGH,QWKHFDVHRIa FRQHindenter with a perfect VSKHULFDOWLS the total cross-section area $FLVJLYHQE\
$F
S
K2 2S
UKFor U!!K$F |2SUK DFFRUGLQJWR>@
,Q )(0 PRGH WKH VSKHUHFRQLFDO WLS ZDV UHSODFHG E\ D VSKHUH 7KH ORFD- WLRQRI3GJUDLQVLQWKHFDUERQDFHRXVOD\HULVQRWV\PPHWULF7KHGHIRUPDWLRQRI
the C-Pd film model in the FEM simulated nano-indentation experiment with the VSKHULFDOO\VKDSHGWLSLVVKRZQLQ)LJ
)LJ3ODVWLFGHIRUPDWLRQRI&3GILOPLQWLPH
)LJVKRZVWKDWWKHGHIRUPDWLRQIRUDFDUERQDFHRXVSDOODGLXPILOPLVQRW
V\PPHWULFDO1DQRJUDLQVDUHPRYHGLQWKHFDUERQDFHRXVPDWUL[WRZDUGWKHILOP¶V
surface and create piling-up on the surface of the film in a contact area of the tip’s SHQHWUDWLRQUHJLRQ'HIRUPDWLRQLQVLGHWKHILOP¶VGHSHQGVRQWKHGLVWULEXWLRQRI
JUDLQVLQWKLVILOP
)LJ)RUFHGHSWKFXUYHD)(0VLPXODWLRQEH[SHULPHQWDOWHVW
1DQRLQGHQWDWLRQDQDO\VLVUHVXOWVIRU&3GILOPDUHSUHVHQWHGLQ)LJ)'
SORWVZHUHREWDLQHGDVDUHVXOWRIWKH)(0VLPXODWLRQ)LJDDQGQDQRLQGHQWD- WLRQH[SHULPHQW)LJE7KHFDOFXODWHGSORWUHIOHFWVH[SHULPHQWDOFXUYH7KH
DQDO\VLVRIWKHVHFXUYHVVKRZVWKDWKDUGQHVVRI&3GILOPLVa*3DDQGUHGXFHG
PRGXOXVLVa*3D
This compatibility of experimental and simulated data allow to predict of Pd QDQRJUDLQV EHKDYLRU LQVLGH WKH &3G ILOP SDOODGLXP GLVSODFHPHQW LQ FDUERQD- FHRXVPDWUL[VWUHVVGXULQJWKHQDQRLQGHQWDWLRQWHVW
&21&/86,216
:HFDQGHGXFHIURPRXUPRGHOLQJH[SHULPHQWWKDWWKHPHFKDQLFDOSURSHU- WLHVRIREWDLQHG&3GILOPVDUHFRQQHFWHGWRWKHQDQRVWUXFWXUHRIWKHVHILOPV7KH
C-Pd carbonaceous film has completely different mechanical properties in com- parison to pure C60ILOPVDVZHOODVWRSXUHSDOODGLXPILOP)URP)(0UHVXOWVRQH
can conclude that Pd nanocrystals are moving in carbon matrix toward the film VXUIDFHGXHWRDQH[WHUQDOVWUHVV
FEM simulation also shows that deformation of the model of the C-Pd film LVQRWV\PPHWULFDO3GQDQRJUDLQVPRYHWRZDUGWKHILOP¶VVXUIDFHLQWKHFDUER- QDFHRXVPDWUL[7KH\DOVRFUHDWHSLOLQJXSRQWKHVXUIDFHRIWKHILOPLQDFRQWDFW
DUHDRIWKHSHQHWUDWLRQUHJLRQ&KDQJHVLQWKHIRUPRIILOPXQGHUJRLQJLQWKHILOP
YROXPHGHSHQGRQWKHGLVWULEXWLRQRIJUDLQVLQWKLVILOP
2EVHUYHGHIIHFWVDUHLPSRUWDQWEHFDXVHRISUDFWLFDODSSOLFDWLRQVRIILOPVDV
0(06GHYLFHV9DULRXVPHFKDQLFDOSURSHUWLHVDUHFRQQHFWHGWRGLIIHUHQFHVLQWKH
VWUXFWXUHDQGWKHFRPSRVLWLRQRIREWDLQHGILOPV
$&.12:/('*(0(176
7KH DXWKRU ZLVKHV WR WKDQN ( &]HUZRV]$ 5LFKWHU DQG 3 'áXĪHZVNL IRU
WKHLUKHOSLQSHUIRUPLQJWKHPHDVXUHPHQWV filmThis research was co-financed by the (XURSHDQ 5HJLRQDO 'HYHORSPHQW )XQG ZLWKLQ WKH ,QQRYDWLYH (FRQRP\ 2SHUD- WLRQDO 3URJUDPPH WLWOH RI WKH SURMHFW ³'HYHORSPHQW RI WHFKQRORJ\
for a new generation of the hydrogen and hydrogen compounds sensor for appli- FDWLRQVLQDERYHQRUPDWLYHFRQGLWLRQV´1R8'$32,*
REFERENCES
>@ 0.R]áRZVNL5'LGXV]NR.2OV]HZVND+:URQND(&]HUZRV]1DQRVWUXFWXUDOSDO- ODGLXPILOPVIRUVHQVRUDSSOLFDWLRQV9DFXXP82
>@ , 3DYORYVN\ 36RXQGDUUDMDQ =<DQLY 3DOODGLXP QDQRSDUWLFOH K\GURJHQ VHQVRU 6HQVRUV 7UDQVGXFHUV-RXUQDO73,
>@ :&2OLYHUDQG*03KDUU$QLPSURYHGWHFKQLTXHIRUGHWHUPLQLQJKDUGQHVVDQGHODVWLF
PRGXOXVXVLQJORDGDQGGLVSODFHPHQWVHQVLQJLQGHQWDWLRQH[SHULPHQWV-0DWHU5HV7
>@$5LFKWHU55LHV56PLWK0+HQNHO%:ROI1DQRLQGHQWDWLRQRIGLDPRQGJUDSKLWHDQG
IXOOHUHQHILOPV'LDPRQGDQG5HODWHG0DWHULDOV9
>@*7LPS1DQRWHFKQRORJ\6SULQJHU1HZ<RUN
>@$&)LVFKHU&ULSSV1DQRLQGHQWDWLRQ6SULQJHU9HUODJ1HZ<RUN
>@(0DGHQFL,*XYHQ7KHILQLWHHOHPHQWPHWKRGDQGDSSOLFDWLRQVLQHQJLQHHULQJXVLQJ $16<6
6SULQJHU6FLHQFH%XVLQHVV0HGLD
>@01RZLFNL$5LFKWHU%:ROI+.DF]PDUHN1DQRVFDOHPHFKDQLFDOSURSHUWLHVRISRO\PHUV
LUUDGLDWHGE\893RO\PHU