$B9V1i(B $B;~9o(B | $B9V1i(B $BHV9f(B | $B9V1iBjL\!?H/I=$B%-!<%o!<%I(B | $BJ,N`(B $BHV9f(B | $B$BHV9f(B | |
A $B2q>l(B |
(13:00$B!A(B14:24) ($B:BD9(B $BK\4V(B $B=S;J!&D+86(B $B@?(B) |
13:00$B!A(B 13:12 | A21 | Villermaux-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 $B8|(B | Villermaux-Dushman reaction Spray Mixing Segregation Index
| 2-b | 64 |
13:12$B!A(B 13:24 | A22 | $BYxYBAeFb$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 $B8|(B | Complete drawdown Mixing process Floating particles
| 2-b | 77 |
13:24$B!A(B 13:36 | A23 | $BB?CJMc3IYBAe$NF0NO!&:.9gFC@-$N2A(B
($B2#9qBgM}9)(B) $B!{|b66(B $BNh(B$B!&(B ($B2#9qBg9)(B) ($B@5(B)$B;03Q(B $BN4B@(B | mixing PIV multi-stage stirred vessel
| 2-b | 114 |
13:36$B!A(B 13:48 | A24 | $B%9%F%l%*(BPIV$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 $BN4B@(B | mixing PIV
| 2-b | 120 |
13:48$B!A(B 14:00 | A25 | $B2sE>Mc$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 $BGn9T(B | iPS cells suspension culture
| 2-b | 185 |
14:00$B!A(B 14:12 | A26 | $B%@%`%V%l%$%/$r79
($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 $B8w<#(B | non Newtonian fluid dam break flow numerical calculation
| 2-a | 66 |
14:12$B!A(B 14:24 | A27 | $B6bB0%l!<%s>e$GI9$,F0$/8=>]$K$D$$$F(B
($BG#:j9b9;(B) ($B9b(B)$B!{L>$B!&(B ($B9b(B)$B!{@u@n(B $B<#6p(B$B!&(B ($B9b(B)$B!{ | ice surface tension metal lane
| 8-b | 145 |
|
(14:36$B!A(B16:00) ($B:BD9(B $BED8}(B $BfF8g!&;03Q(B $BN4B@(B) |
14:36$B!A(B 14:48 | A29 | $B0lHL:BI87O3J;R%\%k%D%^%sK!$rMQ$$$?(B2$B1_Cl<~$j$NN.$l(B
($BETN)Bg(B) $B!{>.NS(B $BBg2p(B$B!&(B ($B@5(B)$BED@n(B $B=SIW(B | Lattice Boltzmann method Generalized coordinate system Rotating cylinder
| 2-a | 87 |
14:48$B!A(B 15:00 | A30 | $B%$%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 $B=S;J(B | inkjet VOF droplets
| 2-a | 130 |
15:00$B!A(B 15:12 | A31 | $BMOM;%,%i%9$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 $B=S;J(B | glass melts unsteady heat transport flow in a circular tube
| 2-a | 128 |
15:12$B!A(B 15:24 | A32 | $B9bG4@-N.BN$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 $B=S;J(B | highly viscous fluid natural convection CFD
| 2-a | 127 |
15:24$B!A(B 15:36 | A33 | $B%U%C2=H?1~AuCV$N?tCM2r@O(B
($B:k6LBg9)(B) $B!{c7F#(B $BIp=)(B$B!&(B ($B:k6LBg1!(B) ($B@5(B)$BK\4V(B $B=S;J(B | Fuel debris Fluoride volatility method Numerical analysis
| 2-a | 123 |
15:36$B!A(B 15:48 | A34 | $B5$Cl$N6&LD!!!A2;H/EE$N8zN(2=$rL\;X$7$F!A(B
($B9-Eg9qBY;{9b9;(B) ($B9b(B)$B@62H(B $BD>Lo(B | wavelength doubled vibration resonance
| 2-a | 26 |
15:48$B!A(B 16:00 | A35 | $B%P%9%?%V12$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-g | 25 |
B $B2q>l(B |
(9:00$B!A(B10:24) ($B:BD9(B $BLnB<(B $B4490!&CgB<(B $B1QLi(B) |
9:00$B!A(B 9:12 | B01 | LCP$B
($B:eBg(B) ($B3X(B)$B!{9b5H(B $B=a:H(B$B!&(B ($B:eBg1!(B) $B8U(B $BZ_E7(B$B!&(B ($B%]%j%W%i%9%A%C%/%9(B) $BzpLn(B $BM5Je(B$B!&(B $B@DLZ(B $B8=(B$B!&(B ($B:eBg1!(B) ($B@5(B)$B2,Ln(B $BBYB'(B | Injection Molding OpenFOAM DEM
| 2-a | 206 |
9:12$B!A(B 9:24 | B02 | 3D$B%P%$%*%W%j%s%F%#%s%0$N%$%s%/@Z$jBX$(;~$K$*$1$k%N%:%kFbN.$l$N?tCM2r@O(B
($B:eBg(B) $B!{;3K\(B $B@?;NO:(B$B!&(B ($B:eBg1!(B) $BF|9b(B $B8w>-(B$B!&(B ($B@5(B)$B6-(B $B?5;J(B$B!&(B $B>.Eh(B $B>!(B$B!&(B ($B@5(B)$B2,Ln(B $BBYB'(B | VOF model OpenFOAM Bioprinting
| 2-e | 282 |
9:24$B!A(B 9:36 | B03 | $B1UE)HyN32=$K$*$1$kN3EYJ,I[M=B,<0$N8!F$(B
($B4tIlBg(B) $B!{LpED(B $B;~1)(B$B!&(B $B?@C+(B $BJ~9((B$B!&(B $B?eLn(B $B63J<(B$B!&(B ($B@5(B)$BD+86(B $B@?(B$B!&(B $B5\:d(B $BIp;V(B | atomaization droplet size distribution shadow sizing method
| 2-e | 326 |
9:36$B!A(B 9:48 | B04 | $B%^%$%/%m%P%V%k$rMQ$$$?%7%j%+Cf6uN3;R$N3+H/5Z$S:GE,2=(B
($B;37ABg9)(B) $B!{9b66(B $B2mLi(B$B!&(B ($B@5(B)$BKkED(B $B | silica microbubbles hollow particles
| 2-e | 211 |
9:48$B!A(B 10:00 | B05 | $B%^%$%/%mN.O)Fb$K$*$1$k1U%3%$%k8=>]$NN.F0>uBV2r@O(B
($BElM}Bg9)(B) $B!{$B!&(B ($B%*%U%#%9<<1`(B) ($B@5(B)$B<<1`(B $B9@;J(B$B!&(B ($BElM}Bg9)(B) ($B@5(B)$BB<>e(B $BM5:H(B$B!&(B ($B@5(B)$B>>@n(B $BGnN<(B$B!&(B ($B@5(B)$BBgC](B $B>!?M(B$B!&(B ($B@5(B)$B>1Ln(B $B8|(B | Microfluidics Liquid rope-coil effect Particle method
| 2-e | 83 |
10:00$B!A(B 10:12 | B06 | $B%^%$%/%mN.F0AX$NN.F02=FC@-$K4X$9$k8&5f(B
($B:4@$J]9b@l(B) ($B@l(B4)$B!{%8%g!<%s%9(B $B%8%'!<%`%9(B$B!&(B ($B@l(B4)$BA0ED(B $BBYM$(B$B!&(B ($B@l(B4)$BDEN1:j(B $BM%EM(B$B!&(B $BzpED(B $BM59/(B$B!&(B ($B@5(B)$B>kLn(B $BM4@8(B | Fluidized bed Microreactor Numerical simulation
| 2-c | 215 |
10:12$B!A(B 10:24 | B07 | $B%^%$%/%m%W%i%9%A%C%/$NIb>eJ,N%$K4X$9$k8&5f(B
($B:4@$J]9b@l(B) ($B@l(B4)$B!{B<>e(B $B>D(B$B!&(B ($B@l(B4)$BEDJU(B $B>M8c(B$B!&(B $BEDCf(B $BBYI'(B$B!&(B $B>>;3(B $B;K7{(B$B!&(B $BCfEg(B $B8-<#(B$B!&(B ($B@5(B)$B>kLn(B $BM4@8(B | Fine bubble Microplastic Floating Separation
| 2-e | 219 |
|
(10:36$B!A(B12:00) ($B:BD9(B $BD+86(B $B@?!&7'@Z(B $B@t(B) |
10:36$B!A(B 10:48 | B09 | $B%+!<%F%sEII[$N;0
($B:k6LBg9)(B) $B!{IZ3_(B $B97B@(B$B!&(B ($B:k6LBg1!M}9)(B) ($B3X(B)$B@iMU(B $B9/B@O:(B$B!&(B ($B:k6LBg1!(B) ($B@5(B)$BK\4V(B $B=S;J(B | curtain coating adhesive CFD
| 2-a | 126 |
10:48$B!A(B 11:00 | B10 | $B9b05(BCO2$B$rMQ$$$?J.L84%AgK!$K$h$k%+%U%'%$%sHyN3;RAO@=$KBP$9$kD4@=05NO$N1F6A(B
($B6bBtBgM}9)(B) $B!{>>2,(B $B1{8J(B$B!&(B ($B6bBtBg1!<+A3(B) ($B3X(B)Xie Bo$B!&(B ($B3X(B)$B;32<(B $BCR?J(B$B!&(B ($B6bBtBgM}9)(B) ($B@5(B)$BFbED(B $BGn5W(B | Spray drying High pressure CO2 Caffeine micronization
| 2-f | 269 |
11:00$B!A(B 11:12 | B11 | $B%O%$%V%j%C%I2CG.MQ(BCNT$B4^M-%"%k%_%JJ#9g:`NA$NM6EEFC@-$NI>2A(B
($B9-Bg9)(B) $B!{;3ED(B $B2m98(B$B!&(B ($B86;RNO5!9=(B) $B@%@n(B $BCR?C(B$B!&(B ($B9-Bg1!9)(B) ($B@5(B)$B?<_7(B $BCRE5(B$B!&(B ($B@5(B)$B@P?@(B $BE0(B$B!&(B ($B@5(B)$BJ!0f(B $B9qGn(B | CNT uniformity Dielectric properties
| 2-f | 203 |
11:12$B!A(B 11:24 | B12 | $B?75,$J%8%'%C%H%_%k$N3+H/$H$=$NJ4:U@-G=$NI>2A(B
($B:eI\Bg9)(B) $B!{>>1J(B $B$B!&(B ($B:eI\Bg1!9)(B) ($B@5(B)$BBg:j(B $B=$;J(B$B!&(B ($B@5(B)$BCgB<(B $B1QLi(B$B!&(B ($B@5(B)$BLJLn(B $BE/(B | Dry grinding Fluidized bed jet mill Classification
| 2-f | 232 |
11:24$B!A(B 11:36 | B13 | $BBG>{%W%m%;%9$K$*$1$k11JILL2Y=EB,Dj(B
($B:eI\Bg9)(B) $B!{:#5H(B $BM%Je(B$B!&(B ($B:eI\Bg1!9)(B) ($B@5(B)$BBg:j(B $B=$;J(B$B!&(B ($B@5(B)$BCgB<(B $B1QLi(B$B!&(B ($B@5(B)$BLJLn(B $BE/(B | Compression speed Tableting process Finite Element Method
| 2-f | 100 |
11:36$B!A(B 11:48 | B14 | DEM$B%7%_%e%l!<%7%g%s$GLM@8CO$rI=8=$9$k$?$a$NIUCeNO$N8!F$(B
($B2,;3M}Bg5!3#%7%9%F%`9)3X2J(B) $B!{:4!9LZ(B $BM'0T(B$B!&(B ($B@5(B)$B7,LZ(B $B8-Li(B$B!&(B ($B@5(B)$BJ?Ln(B $BGnG7(B | Powder Discrete Element Method Cohesive force
| 2-f | 223 |
11:48$B!A(B 12:00 | B15 | $B1U2M66$rM-$9$kJ4BNGS=PN.F0$N(BDEM$B?tCM2r@O(B
($B:4@$J]9b@l(B) ($B@l(B4)$B!{>>1J(B $B44B@(B$B!&(B $BzpED(B $BM59/(B$B!&(B $B>>;3(B $B;K7{(B$B!&(B $BCfEg(B $B8-<#(B$B!&(B ($B@5(B)$B>kLn(B $BM4@8(B | Discrete Element Method Powder Liquid bridge
| 2-f | 221 |