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$B:G=*99?7F|;~!'(B2021-03-04 21:47:01
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9:12$B!A(B 9:24A02$B%;%_%/%i%9%l!<%H%O%$%I%l!<%H$K$*$1$k(BCH4+CO2$B:.9g%,%9J,N%FC@-(B
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Smiclathrate hydrate
Gas separation properties
Ionic substances
1-a148
9:24$B!A(B 9:36A03$BDc(BGWP$B7O(B3$B@.J,7O:.9gNdG^$NG.NO3X%b%G%kI>2A$N$?$a$N5$1UJ?9U@-
($BIY;38)Bg(B) $B!{@>ED(B $BM}I'(B$B!&(B $B;3ED(B $BE/@?(B$B!&(B ($B@5(B)$B5\K\(B $BBY9T(B
low GWP refrigerant
vapor-liquid equilibrium
Peng-Robinson equation of state
1-a155
9:36$B!A(B 9:48A04$BNL;R2=3X$HE}7WG.NO3X$K4p$E$/%$%*%s1UBN$HHs?eMOG^$N:.9g;~$N2a>j%(%s%?%k%T!2A(B
($BCf1{BgM}9)(B) ($B3X(B)$B!{EOIt(B $B>0BAO:(B$B!&(B ($BCf1{BgM}9)(B/JST ACT-X) ($B@5(B)$B9uLZ(B $B:ZJ];R(B$B!&(B ($BCf1{BgM}9)(B/$BJ,;R8&(B) ($B@5(B)$B?9(B $B42IR(B
non aqueous ionic liquid solutions
ab initio statistical thermodynamics simulations
excess enthalpy
1-a240
9:48$B!A(B 10:00A05$B%V%i%$%K%/%k$N8&5f(B
($BBg:eI\N)E72&;{9bEy3X9;(B) ($B9b(B)$B!{1d0B(B $B0l??(B$B!&(B ($B9b(B)$B!{>eLn(B $BBY2m(B$B!&(B ($B9b(B)$B!{LS2<(B $B7kB@(B$B!&(B ($B9b(B)$B!{@>8}(B $B98J?(B
Brinicle
Ice
Icicle
14-e161
10:00$B!A(B 10:12A06($B9V1iCf;_(B)

10031
10:12$B!A(B 10:24A07$BE7A3AG:`$r86NA$H$7$?M;E@$N9b$$%j%C%W%/%j!<%`$N:n@.$H$=$N8zG=(B
($BBg:eI\N)E72&;{9bEy3X9;(B) ($B9b(B)$B!{NS(B $BM~;R(B$B!&(B ($B9b(B)$B!{@n86(B $BN\;R(B$B!&(B ($B9b(B)$B!{5H2,(B $BF|:Z;R(B$B!&(B ($B9b(B)$B!{|bED(B $BI42V(B
natural materials
melting point
moisture
1-b147
10:24$B!A(B 10:36$B5Y7F(B
$B4pACJ*@-(B
(10:36$B!A(B12:00) ($B:BD9(B $B5\K\(B $BBY9T!&?9(B $B42IR(B)
10:36$B!A(B 10:48A09$B?M9)%K%e!<%i%k%M%C%H%o!<%/$rMQ$$$?(BPC-SAFT$B>uBVJ}Dx<0$N%Q%i%a!<%??d;;(B
($BElM}Bg(B) $B!{KL86(B $B??G7(B$B!&(B ($B@5(B)$B>>@n(B $BGnN<(B$B!&(B ($B@5(B)$BB<>e(B $BM5:H(B$B!&(B ($B@5(B)$B>1Ln(B $B8|(B$B!&(B ($B@5(B)$BBgC](B $B>!?M(B
Artificial Neural Network
PC-SAFT EoS
Group Contribution method
1-a178
10:48$B!A(B 11:00A10$BJ,;R>pJs$rF~NO$7$?%K%e!<%i%k%M%C%H%o!<%/$K$h$k(BCO2$B5[<}%$%*%N%2%k$N@_7W(B
($BEl9)BgJ*$B!&(B ($B@5(B)$B?%ED(B $B9LI'(B$B!&(B ($B@5(B)$B2<;3(B $BM52p(B
CO2 absorption
molecular information
neural network
1-a200
11:00$B!A(B 11:12A11$BJ,;R%7%_%e%l!<%7%g%s$rMQ$$$?%3%i!<%2%s$N%0%i%U%'%s5[Ce$N9M;!(B
($B>k@13X9b(B) ($B9b(B)$B!{CfDM(B $B2BF`(B$B!&(B ($BJ<8K8)BgM}(B) $B>.NS(B $B7rMN(B$B!&(B ($BJ<8K8)Bg1!%7%_%e(B) $B>>2,(B $BNJ(B$B!&(B ($B@5(B)$B@P0f(B $BNI$B!&(B $BOIDE(B $B?N;V(B
molecular dynamics
graphene
collagen
1-a260
11:12$B!A(B 11:24A12$B2+?'%4%`>uN22+$N@8@.MW0x(B
($B>>;3Cf1{9b(B) ($B9b(B)$B!{>.NS(B $BEm;R(B$B!&(B ($B9b(B)$B!{Cf@n(B $BM%F`(B$B!&(B ($BM!(B)$Bt"(B $BBgJe(B
sulfur
soft sulfur
yellow
1-b47
11:24$B!A(B 11:36A13$BE4(B(III)$B%$%*%s$H%A%*%7%"%s;@%$%*%s$K$h$kDh?'H?1~$HB`?'(B
($B>>;3Cf1{9b(B) ($B9b(B)$B!{:d0f(B $B7r(B$B!&(B ($B9b(B)$B!{:4!9LZ(B $B?p5*(B$B!&(B ($B9b(B)$B!{B^ED(B $BNCJ?(B$B!&(B ($B9b(B)$B!{?eC+(B $BOBG7(B$B!&(B ($BM!(B)$Bt"(B $BBgJe(B
iron
thiocyanate ion
discoloration
1-a48
11:36$B!A(B 11:48A14$B2+F<$NAH@.$NJQ2=$K$*$1$k%$%*%s2=798~$NJQ2=(B
($B@92,Bh;0(B) ($B9b(B)$B!{1sF#(B $B_:3p(B$B!&(B ($B9b(B)$B!{Bg5WJ](B $BCN5*(B$B!&(B ($B9b(B)$B!{9b66(B $B$B!&(B ($B9b(B)$B!{>H0f(B $B;|?%(B$B!&(B ($B9b(B)$B!{CfB<(B $BA3(B$B!&(B ($B9b(B)$B!{;wFb(B $BAUB@(B
Ionization tendency
Brass
Alloy composition
1-b80
11:48$B!A(B 12:00A15($B9V1iCf;_(B)

10032
12:00$B!A(B 12:12$BCk5Y$_(B
$BN3;R!&N.BN%W%m%;%9(B
(13:00$B!A(B14:24) ($B:BD9(B $BK\4V(B $B=S;J!&D+86(B $B@?(B)
13:00$B!A(B 13:12A21Villermaux-Dushman$BH?1~$rMQ$$$?%9%W%l!<<0:.9g%7%9%F%`Fb:.9g>uBVI>2A(B
($BElM}Bg9)(B) $B!{B@(B$B!&(B ($B@5(B)$BB<>e(B $BM5:H(B$B!&(B ($B@5(B)$B>>@n(B $BGnN<(B$B!&(B ($B@5(B)$BBgC](B $B>!?M(B$B!&(B ($B@5(B)$B>1Ln(B $B8|(B
Villermaux-Dushman reaction
Spray Mixing
Segregation Index
2-b64
13:12$B!A(B 13:24A22$BYxYBAeFb$G$NN3;R4,$-9~$_FC@-2r@O(B
($BElM}Bg9)(B) $B!{5Z@n(B $BM:4n(B$B!&(B ($B@5(B)$BB<>e(B $BM5:H(B$B!&(B ($B@5(B)$B>>@n(B $BGnN<(B$B!&(B ($B@5(B)$BBgC](B $B>!?M(B$B!&(B ($B@5(B)$B>1Ln(B $B8|(B
Complete drawdown
Mixing process
Floating particles
2-b77
13:24$B!A(B 13:36A23$BB?CJMc3IYBAe$NF0NO!&:.9gFC@-$N2A(B
($B2#9qBgM}9)(B) $B!{|b66(B $BNh(B$B!&(B ($B2#9qBg9)(B) ($B@5(B)$B;03Q(B $BN4B@(B
mixing
PIV
multi-stage stirred vessel
2-b114
13:36$B!A(B 13:48A24$B%9%F%l%*(BPIV$B$K$h$k3IYB1):,<~$j$NB.EY(B3$B@.J,$NF1;~B,Dj$HMpN.%(%M%k%.!<$NDjNL2=(B
($B2#9qBgM}9)(B) $B!{;3K\(B $B:Z!9Jf(B$B!&(B ($B2#9qBg9)(B) ($B@5(B)$B;03Q(B $BN4B@(B
mixing
PIV
2-b120
13:48$B!A(B 14:00A25$B2sE>Mc$rMQ$$$?YxYBAe$K$*$1$k(BiPS$B:YK&$NBg5,LOG]M\$K$D$$$F$N?tCM2r@O(B
($B:eBg(B) ($B3X(B)$B!{>.H+(B $BNMJe(B$B!&(B ($B:eBg1!(B) ($B3X(B)$B0kIt(B $BN$B!&(B ($B@5(B)$B2,Ln(B $BBYB'(B$B!&(B ($B@5(B)$B5*%N2,(B $B@5Gn(B$B!&(B ($BF#?99)6H(B) ($BK!(B)$BETAR(B $BCN9@(B$B!&(B ($BK!(B)$B>>ED(B $BGn9T(B
iPS cells
suspension culture
2-b185
14:00$B!A(B 14:12A26$B%@%`%V%l%$%/$r79
($BJ<8K8)Bg(B) $B!{BgC+(B $B@29a(B$B!&(B ($B@5(B)$B0KF#(B $BOB9((B$B!&(B ($B@5(B)$BED8}(B $BfF8g(B$B!&(B ($B@5(B)$B;3K\(B $BBs;J(B$B!&(B ($B@5(B)$BA0ED(B $B8w<#(B
non Newtonian fluid
dam break flow
numerical calculation
2-a66
14:12$B!A(B 14:24A27$B6bB0%l!<%s>e$GI9$,F0$/8=>]$K$D$$$F(B
($BG#:j9b9;(B) ($B9b(B)$B!{L>$B!&(B ($B9b(B)$B!{@u@n(B $B<#6p(B$B!&(B ($B9b(B)$B!{
ice
surface tension
metal lane
8-b145
14:24$B!A(B 14:36$B5Y7F(B
$BN3;R!&N.BN%W%m%;%9(B
(14:36$B!A(B16:00) ($B:BD9(B $BED8}(B $BfF8g!&;03Q(B $BN4B@(B)
14:36$B!A(B 14:48A29$B0lHL:BI87O3J;R%\%k%D%^%sK!$rMQ$$$?(B2$B1_Cl<~$j$NN.$l(B
($BETN)Bg(B) $B!{>.NS(B $BBg2p(B$B!&(B ($B@5(B)$BED@n(B $B=SIW(B
Lattice Boltzmann method
Generalized coordinate system
Rotating cylinder
2-a87
14:48$B!A(B 15:00A30$B%$%s%/%8%'%C%H%N%:%k$+$i$N1UE)@8@.$*$h$SCeCF%7%_%e%l!<%7%g%s(B
($B:k6LBg9)(B) $B!{B?ED(B $BM5B@(B$B!&(B ($B:k6LBg1!M}9)(B) ($B3X(B)$B5H>B(B $BM%51(B$B!&(B ($B:k6LBg1!(B) ($B@5(B)$BK\4V(B $B=S;J(B
inkjet
VOF
droplets
2-a130
15:00$B!A(B 15:12A31$BMOM;%,%i%9$NEAG.$*$h$SN.F02r@O(B
($B:k6LBg9)(B) $B!{>.;3(B $BN?Lp(B$B!&(B ($B:k6LBg1!M}9)(B) ($B3X(B)$B@iMU(B $B9/B@O:(B$B!&(B ($B:k6LBg1!(B) ($B@5(B)$BK\4V(B $B=S;J(B
glass melts
unsteady heat transport
flow in a circular tube
2-a128
15:12$B!A(B 15:24A32$B9bG4@-N.BN$K$*$1$k%-%c%S%F%#Fb<+A3BPN.$N?tCM2r@O(B
($B:k6LBg9)(B) $B!{:4!9LZ(B $BN6Lk(B$B!&(B ($B:k6LBg1!M}9)(B) ($B3X(B)$B@iMU(B $B9/B@O:(B$B!&(B ($B:k6LBg1!(B) ($B@5(B)$BK\4V(B $B=S;J(B
highly viscous fluid
natural convection
CFD
2-a127
15:24$B!A(B 15:36A33$B%U%C2=H?1~AuCV$N?tCM2r@O(B
($B:k6LBg9)(B) $B!{c7F#(B $BIp=)(B$B!&(B ($B:k6LBg1!(B) ($B@5(B)$BK\4V(B $B=S;J(B
Fuel debris
Fluoride volatility method
Numerical analysis
2-a123
15:36$B!A(B 15:48A34$B5$Cl$N6&LD!!!A2;H/EE$N8zN(2=$rL\;X$7$F!A(B
($B9-Eg9qBY;{9b9;(B) ($B9b(B)$B@62H(B $BD>Lo(B
wavelength
doubled vibration
resonance
2-a26
15:48$B!A(B 16:00A35$B%P%9%?%V12$NH/@85/8;(B
($B9-Eg9qBY;{9b9;(B) ($B9b(B)$B!{?7ED(B $BM4Lo(B$B!&(B ($B9b(B)$B!{A0ED(B $BMK(B
flow of different directions
initial velocity
Partition plate
2-g25
16:00$B!A(B 16:10$B5Y7F(B
$BFCJL9V1i(B, $BI=>4?3::7k2LH/I=(B
(16:10$B!A(B16:55) ($B;J2q(B $B2.Ln(B $BGn9/(B)
16:10$B!A(B 16:55A37$B2=3X9)3X$r6n;H$7$FL58BBg$N2ACM$rAOB$$9$k(B
($BElKLBg1!9)(B) ($B@5(B)$BKL@n(B $B>0H~(B
Plenary lecture
17-a337
16:55$B!A(B $BI=>4?3::7k2LH/I=(B
$B9V1iH/I=%W%m%0%i%`(B
$BBh(B23$B2s2=3X9)3X2q3X@8H/I=2q(B
(C) 2021 $B8x1W
Most recent update: 2021-03-04 21:47:01
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