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$B:G=*99?7F|;~!'(B2021-08-21 18:44:01

$B$3$NJ,N`$G$h$/;H$o$l(B
$B$F$$$k%-!<%o!<%I(B		$B%-!<%o!<%I(B$B
Solubility4$B7o(B*
molecular dynamics simulation2$B7o(B
carbon dioxide2$B7o(B
multicomponent system2$B7o(B
Supercritical CO22$B7o(B
interaction number parameter2$B7o(B
excess molar enthalpy1$B7o(B

$B$BHV9f(B$B9V1iBjL\!?H/I=$B%-!<%o!<%I(B$BH/I=7A<0(B
89$B?7$7$$3hNL78?t<0$N=cJ*
($B6eBg9)(B) ($B@5(B)$B4d0f(B $BK'IW(B		interaction number parameter
new activity coefficient equation
multicomponent system
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102303.2K$B$N6Q0l1UAjNN0h$K$*$1$k(BHFO-1234ze(E)+$B%"%;%H%s:.9g7O$NL)EYB,Dj(B
($BF|Bg@8;:9)(B) ($B3X(B)$B!{8M:"(B $B5~$B!&(B ($BF|BgM}9)(B) ($B@5(B)$B2,ED(B $B??5*(B$B!&(B ($BF|Bg@8;:9)(B) ($B@5(B)$BJ]2J(B $B5.N<(B$B!&(B ($B%^%l!<%7%"9)Bg(B) ($B@5(B)$BDT(B $BCRLi(B$B!&(B ($B;:Am8&(B) ($B@5(B)$B8E20(B $BIp(B		density
hydrofluoroolefin
binary mixture
P
120$BD6NW3&Fs;@2=C:AGJ70O5$2<$K$*$1$k%]%j%a%?%/%j%k;@%a%A%kCf$N%"%s%H%i%-%N%s$N3H;678?t$NB,Dj$*$h$SJ,;RF0NO3X%7%_%e%l!<%7%g%s(B
($B6eBg9)(B) ($B3X(B)$B!{@>;3(B $B3+(B$B!&(B ($B@5(B)$B4d0f(B $BK'IW(B		Diffusion coefficient
Supercritical impregnation
Molecular dynamics simulation
P
137ASOG-ThermConduct$B%b%G%k$K$h$k1U:.9gJ*G.EAF3N($N;;=P(B
($BF|BgM}9)(B) ($B@5(B)$B!{FJLZ(B $B>!8J(B$B!&(B ($B@5(B)$B>>ED(B $B909,(B$B!&(B ($B@5(B)$B7*86(B $B@6J8(B$B!&(B ($BCf1{BgM}9)(B) ($B@5(B)$BA%B$(B $B=S9'(B$B!&(B (GNAU U.) V. K. Rattan		Thermal Conductivity
ASOG-ThermConduct model
Prediction
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140$BAjJ,N%7?5[<}%2%k$NFs;@2=C:AG5[<}2aDx$K$*$1$kJ*
($BEl9)BgJ*$B!&(B ($B@5(B)$B?%ED(B $B9LI'(B$B!&(B ($B@5(B)$B2<;3(B $BM52p(B		CO2 absorption
phase-separated gel
mass transfer analysis
P
141$B2D;k8w%l!<%6!<$rMxMQ$7$?0eLtJ*
($BEl9)BgJ*$B!&(B ($B@5(B)$B?%ED(B $B9LI'(B$B!&(B ($B@5(B)$B2<;3(B $BM52p(B		rapid measurement
solubility
visible light laser
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164$BD62;GHN.B.J,I[7WB,$K$h$k2aEOE*%l%*%m%8!2A(B
($BKLBg(B) ($B@5(B)$B!{ED:d(B $BM5;J(B$B!&(B $BK'ED(B $BBY4p(B$B!&(B ($B3X(B)$BBg2H(B $B9-J?(B$B!&(B $BB<0f(B $BM40l(B		Rheometry
Transient properties
Ultrasonic wave
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168$B%^%$%/%mGHHsJ?9U6I=j2CG.$K$h$k1U1U3&LL$NI=LL2~
($BJ<8K8)Bg9)(B) $B1rIt(B $BCR;K(B$B!&(B $B$B!&(B ($B@5(B)$B!{D+7'(B $BM52p(B$B!&(B (Curtin U.) Hyde Anita$B!&(B Phan Chi		Microwave
Interfacial modification
Interfacial tension
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183$BFs;@2=C:AG(B/$B%H%k%(%s(B/$B%]%j%a%?%/%j%k;@%a%A%k;0@.J,7O$NAjJ?9U(B
($BElM}Bg(B) ($B3X(B)$B!{5L(B $BBn8+(B$B!&(B ($B@5(B)$B>>@n(B $BGnN<(B$B!&(B ($B@5(B)$BB<>e(B $BM5:H(B$B!&(B ($B@5(B)$B>1Ln(B $B8|(B$B!&(B ($B@5(B)$BBgC](B $B>!?M(B		Phase equilibrium
Carbon dioxide
Polymethyl methacrylate
P
184$B2~NI$7$??7$7$$3hNL78?t<0$rMQ$$$?(B2,3$B$*$h$S(B4$B@.J,7O5$1UJ?9U$NAj4X(B
($B6eBg1!9)(B) ($B3X(B)$B!{>>ED(B $BM*4u(B$B!&(B ($B@5(B)$B4d0f(B $BK'IW(B		interaction number parameter
new activity coefficient model
multicomponent system
P
198$B0eLtIJ(B+$B%7%/%m%G%-%9%H%j%s(B+$B?e7O8G1UJ?9U$N3hNL78?t<0$K$h$k;;=P(B
($BF|BgM}9)(B) ($B@5(B)$B!{FJLZ(B $B>!8J(B$B!&(B ($B@5(B)$B>>ED(B $B909,(B$B!&(B ($B3X(B)$B:45W4V(B $BM*?M(B$B!&(B ($B@5(B)$B7*86(B $B@6J8(B		Solid-Liquid Equilibria
Drug Containing System
Activity Coefficient Equation
O
214$B%l%*%m%8!<%^%C%W$K$h$k9bJ,;RMO1U$NB?3QE*G4CF@-I>2A(B
($BKLBg9)(B) ($B3X(B)$B!{Bg2H(B $B9-J?(B$B!&(B $BK'ED(B $BBY4p(B$B!&(B $BKQ(B $BzuDA(B$B!&(B ($B@5(B)$BED:d(B $BM5;J(B$B!&(B $BB<0f(B $BM40l(B		viscoelasticity
polymer solution
ultrasonic spinning rheometry
P
351$BJ,;R%7%_%e%l!<%7%g%s$rMQ$$$?<+8JAH?%2=%$%*%s1U>=$N%J%N%A%c%M%k$K$*$1$k?eOBMMBV2r@O(B
($BJ<8K8)Bg1!%7%_%e(B) ($B@5(B)$B!{@P0f(B $BNI$B!&(B ($B:eBg1!4p9)(B) ($B@5(B)$B>>NS(B $B?-9,(B$B!&(B ($BKLN$BgM}(B) $BEOJU(B $B9k(B$B!&(B ($BElBg1!J*@-(B) $B86ED(B $B;|5W(B$B!&(B ($BElBg1!9)(B) $B2CF#(B $BN4;K(B$B!&(B ($BJ<8K8)Bg1!%7%_%e(B) $BOIDE(B $B?N;V(B		Ionic Liquid Crystal
Self-Assembly
Nanochannels
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358Wilson$B<0Dj?t$N29EYJQ2=(B
($BElM}Bg(B) ($B@5(B)$BBg9>(B $B=$B$(B		vapor-liquid equilibria
Wilson parameter
temperature dependence
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360$B=cJ*x5$05$N?d;;K!(B
($BElM}BgM}(B) ($B@5(B)$BBg9>(B $B=$B$(B		vapor pressure
boiling point
organic compound
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389$B9b050hD6NW3&Fs;@2=C:AG$KBP$9$kFqMO2r@-J*
($B6bBtBg1!<+(B) ($B3X(B)$B!{FgB<(B $BM45.(B$B!&(B $BF#Bt(B $B$B!&(B ($B6bBtBgM}9)(B) ($B@5(B)$BEDB<(B $BOB90(B		solubility
supercritical CO2
elevated pressure
P
429$BM-5!=$>~6bB0;@2=J*%J%NN3;RJ,;61U$NG4@-5sF0$NG;EY!&29EY0MB8@-(B
($BElKLBg(B/$BF|K\@=9]=j(B) ($B@5(B)$B!{?70f(B $BM5;R(B$B!&(B ($BElKLBgB?858&(B) ($B@5(B)$Bcx5o(B $B9bL@(B$B!&(B ($BElKLBg(BWPI) ($B@5(B)$B2#(B $BE/(B$B!&(B ($B@5(B)$B0$?,(B $B2mJ8(B		nanoparticle
viscosity
P
432$B7k>=2=EY$*$h$SAH@.$N0[$J$k%4%`>u%W%m%T%l%s6&=E9gBN$KBP$9$k(B1-$B%V%F%sMO2rEY!&3H;678?t$NB,Dj$H?d;;(B
($BElKLBg1!9)(B) ($B3X(B)$B@D;3(B $BM55*(B$B!&(B ($BElKL9)Bg9)(B) ($B@5(B)$B!{:4F#(B $BA1G7(B$B!&(B ($BElKLBg1!9)(B) ($B@5(B)$BCv8T(B $B9((B		Crystallinity
Solubility
Diffusivity
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472$B%,%9J,N%@-1UBN$r;V8~$7$?%$%*%s1UBN(B/$BJ,;R@-1UBN:.9g;~$NJ,;R4VAj8_:nMQ$K4X$9$kNL;R2=3XE*9M;!(B
($BCf1{BgM}9)(B/JST ACT-X) ($B@5(B)$B!{9uLZ(B $B:ZJ];R(B$B!&(B ($BCf1{BgM}9)(B) ($B3X(B)$BEOIt(B $B>0BAO:(B$B!&(B ($BCf1{BgM}9)(B/$BJ,;R8&(B) ($B@5(B)$B?9(B $B42IR(B		non aqueous solutions of ionic liquids
ab initio simulations
intermolecular interaction
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557$B%a%?%N!<%k$N(BCO2$B2a>j%(%s%?%k%T!
($BF|Bg1!9)(B) ($B3X(B)$B!{@P@n(B $B@F(B$B!&(B ($BF|Bg9)(B) ($B@5(B)$B;y6L(B $BBgJe(B		excess molar enthalpy
methanol
carbon dioxide
P
629$B?eAG7k9g%M%C%H%o!<%/$K4p$E$/%1!<%8!&%8%c%s%W%b%G%k$N3+H/$H$=$N2aNd5Q?e$K$*$1$k3H;6%@%$%J%_%/%9$X$N1~MQ(B
($B:eBg1!4p9)(B) ($B3X(B)$B!{5FDT(B $BBn??(B$B!&(B ($B@5(B)$B6b(B $B9](B$B!&(B ($B@5(B)$B>>NS(B $B?-9,(B		hydrogen bonding
molecular dynamics simulation
supercooled liquid
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630UV$B$rMQ$$$?K0OBMO2r05NOC5:wK!$K$h$kD6NW3&(BCO2$B$KBP$9$k%k%V%l%s$NMO2rEY$NB,Dj$HAj4X(B
($B6bBtBg1!<+A3(B) ($B3X(B)$B!{A0ED(B $BD>:H(B$B!&(B ($B6bBtBgM}9)(B) ($B@5(B)$BFbED(B $BGn5W(B		Supercritical CO2
Solubility
Rubrene
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(C) 2021 $B8x1W
Most recent update: 2021-08-21 18:44:01
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