$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 $BBh(B1$BF|(B |
| (9:00$B!A(B10:00)$B!!(B($B:BD9(B $B>>1:>OM5(B) |
| 9:00$B!A(B 9:20 | A101 | $B<><0%/%i%C%A$K$*$1$k%*%$%kN.F08z2L(B ($B@EBgAO2J1!(B) $B!{(B($B3X(B)$B5\@n(B $B>-IR(B$B!&(B($B@EBg1!(B) ($B3X(B)$B@DLZ(B $BM&M4(B$B!&(B($B@EBg(B) $B>.@n(B $B@57I(B$B!&(B($B@EBgAO2J1!(B) ($B@5(B)$B2,Ln(B $BBYB'(B$B!&(B($B%(%U!&%7!$B!&(B$B:4!9LZ(B $BG&(B$B!&(B$B1|0f(B $B0lG7(B | Oil flow Wet clutch Torque
| 2-a | 161 |
| 9:20$B!A(B 9:40 | A102 | $B%X%l!&%7%g%&%;%kFb$G$N1UBN$NCV49$K$*$1$k%9%Q%$%i%k%Q%?!<%s$N7A@.(B ($BL>9)Bg(B) $B!{(B($B3X(B)$BH<(B $B8w>-(B$B!&(B($B@5(B)$BD9DE(B $BM:0lO:(B$B!&(B($B@5(B)$B2CF#(B $BDw?M(B$B!&(B($B@5(B)$BB?ED(B $BK-(B | Spiral pattern Displacement process Reacting flow
| 2-a | 358 |
| 9:40$B!A(B 10:00 | A103 | $BD@EBH?1~$rH<$&(BViscous fingering ($BL>9)Bg(B) $B!{(B($B3X(B)Bae Sikyun$B!&(B($B@5(B)$BD9DE(B $BM:0lO:(B$B!&(B($B@5(B)$B2CF#(B $BDw?M(B$B!&(B($B@5(B)$BB?ED(B $BK-(B | viscous fingering precipitation reaction reacting flow
| 2-a | 393 |
| (10:00$B!A(B11:00)$B!!(B($B:BD9(B $BBgB?M(B) |
| 10:00$B!A(B 10:20 | A104 | $B%U%i%/%?%k3J;RMpN.$ND>@\?tCM%7%_%e%l!<%7%g%s(B ($BL>Bg9)(B) $B!{(B($B3X(B)$BNkLZ(B $BGn5.(B$B!&(B($B@5(B)$BD9ED(B $B9'Fs(B$B!&(B($B6&(B)$B$B!&(B($BElKLBgN.BN8&(B) ($B6&(B)$BAa@%(B $BIR9,(B$B!&(B($BL>Bg%(%3(B) ($B6&(B)$B5WJ](B $B5.(B | Direct numerical simulation grid turbulence fractal grid
| 2-a | 605 |
| 10:20$B!A(B 10:40 | A105 | $B<'>l%Y%J!<%kBPN.$N%+%*%9FC@-(B ($BN)L?4[Bg(B) $B!{C]Fb(B $BN$B!&(B$B?7LZK\(B $B42G7(B$B!&(B($BIt(B)$B8eF#ED(B $B9@(B | Magnetic Field Benard Convection Chaos
| 2-a | 751 |
| 10:40$B!A(B 11:00 | A106 | ($B7gHV(B)
|
| 100 | 776 |
| (11:00$B!A(B12:00)$B!!(B($B:BD9(B $B8VED1YG7(B) |
| 11:00$B!A(B 11:20 | A107 | $B%F%$%i!<12N.$K$*$1$kDcL)EYN3;R$NJ,5i5sF0(B ($B?@8MBg1!9)(B) $B!{(B($B@5(B)$BBgB<(B $BD>?M(B$B!&(B($B3X(B)$B4HK\(B $B7z$B!&(B($B3X(B)$B;3OF(B $B7r;J(B$B!&(B$B7'C+(B $B@k5W(B | Taylor Vortex Fow Solid-Liquid Flow Particle Classification
| 2-a | 38 |
| 11:20$B!A(B 11:40 | A108 | $B8w3X%;%s%5!<$rMQ$$$?3IYBAe$NHs@\?(:.9gB,Dj(B ($B?@8MBg1!9)(B) $B!{(B($B@5(B)$BBgB<(B $BD>?M(B$B!&(B($B?@8MBg9)(B) $B?@Be(B $BAa5*(B$B!&(B($B?@8MBg1!9)(B) $B7'C+(B $B@k5W(B$B!&(B($B%b%k%U%#(B) $B=E2,(B $BMx9'(B | Optical Sensor Mixing Stirred Tank
| 2-a | 39 |
| 11:40$B!A(B 12:00 | A109 | $BC_G.HyN3;R%9%i%j!<$N%-%c%T%i%j! ($B;37ABg1!M}9)(B) $B!{(B($B3X(B)$B4];3(B $BOB5A(B$B!&(B($B@5(B)$BLg3p(B $B=($B!&(B($B@5(B)$B86ED(B $B1QFs(B$B!&(B($B@5(B)$B7*;3(B $B2mJ8(B | latent heat phase change heat transfer
| 2-a | 1 |
|
| (13:00$B!A(B14:00)$B!!(B($B:BD9(B $BLg3p=( |
| 13:00$B!A(B 13:20 | A113 | $B3&LL3h@-:^$K$h$kDq93Dc8:N.$l$N6uD4@_Hw$K$*$1$kEAG.FC@-I>2A(B ($B;38}Bg1!(B) $B!{(B($B@5(B)$B:4Gl(B $BN4(B$B!&(B($B3X(B)$BFb;3(B $BM52p(B | Drag reduction Heat transfer air conditioning
| 2-a | 219 |
| 13:20$B!A(B 13:40 | A114 | $BDq93Dc8:2=3&LL3h@-:^MO1U$NB?=E4KOB;~4VFC@-(B ($B?@8MBg1!(B) $B!{(B($B3X(B)$BEOJU(B $B7$B!&(B($B?@8MBg1!9)(B) ($B@5(B)$BNkLZ(B $BMN(B$B!&(B($B@5(B)$B8VED(B $B1YG7(B$B!&(B($B@5(B)$BGv0f(B $BMN4p(B | Surfactants Relaxation time Counter-ion
| 2-a | 373 |
| 13:40$B!A(B 14:00 | A115 | $B5[<}NdE`5!$N5[<}4o%3%s%Q%/%H2=$K6!$9$k?eOBJ*%9%i%j!<$NN.F0!&EAG.FC@-(B ($B?@8MBg1!(B) $B!{(B($B3X(B)$B4_K\(B $BN4;J(B$B!&(B($B?@8MBg1!9)(B) ($B@5(B)$BNkLZ(B $BMN(B$B!&(B($B@5(B)$B8VED(B $B1YG7(B$B!&(B($B@5(B)$BGv0f(B $BMN4p(B | Absorption chiller Hydrate slurry Flow and heat transfer
| 2-a | 385 |
| (14:00$B!A(B15:00)$B!!(B($B:BD9(B $B:4GlN4(B) |
| 14:00$B!A(B 14:20 | A116 | $B=x5$2~\:Y(BCFD$B%b%G%j%s%0(B ($BEl9)Bg1!M}9)(B) $B!{(B($B3X(B)$B9uLZ(B $BKcM3(B$B!&(B($B@5(B)$BBg@n86(B $B??0l(B$B!&(B($B@5(B)$B>.@n(B $B9@J?(B | packed bed reactor methane steam reforming high-fidelity CFD modeling
| 2-a | 75 |
| 14:20$B!A(B 14:40 | A117 | $B%,%92~2A$K8~$1$?J.N.7?%,%9:.9g4o$N:GE,9=B$I>2A(B ($BF1;V$B!&(B$B$B!&(B$B2,:j(B $B??Li(B$B!&(B($B@5(B)$B?9(B $B9/0](B$B!&(B(JRCM) $B1JIM(B $BMN(B | gas mixing jet numerical simulation
| 2-a | 784 |
| 14:40$B!A(B 15:00 | A118 | $B%^%$%/%mN.O)$rMQ$$$?%j%]%=!<%`$N@8@.5!9=(B ($B?@8MBg1!9)(B) $B!{(B($B@5(B)$BNkLZ(B $BMN(B$B!&(B($B?@8MBg1!(B) ($B3X(B)$BIMB<(B $BH;Lp(B$B!&(B($B?@8MBg1!9)(B) ($B@5(B)$B>!ED(B $BCN>0(B$B!&(B($B@5(B)$B2CF#(B $B<"M:(B$B!&(B($B@5(B)$B8VED(B $B1YG7(B$B!&(B($B@5(B)$BGv0f(B $BMN4p(B | Liposome Micro-flow Size effect
| 2-a | 330 |
| (15:00$B!A(B16:00)$B!!(B($B:BD9(B $BBg@n86??0l(B) |
| 15:00$B!A(B 15:20 | A119 | $B1_4IFb$r<+M3Mn2<$9$kC10l1UE)$N1?F0$N?tCM2r@O(B ($B:k6LBg1!(B) $B!{(B($B@5(B)$BK\4V(B $B=S;J(B$B!&(B($B:k6LBg9)(B) $B;3C<(B $B?.I'(B$B!&(B($B:k6LBg1!(B) ($B@5(B)$B8E4W(B $BFsO:(B | drop Front-Tracking numerical simulation
| 2-a | 145 |
| 15:20$B!A(B 15:40 | A120 | $B1U!9FsAjN.$K$*$1$k%9%i%0@8@.(B ($B2,M}Bg9)(B) $B!{(B($B@5(B)$BJ?Ln(B $BGnG7(B$B!&(B($B2,M}Bg1!(B) ($B3X(B)$BCfDE(B $BM52p(B$B!&(B($B3X(B)$B>>Ln(B $B905.(B$B!&(B($B2,M}Bg9)(B) $B2&(B $BUG(B$B!&(B($B@5(B)$B2,K\(B $BD>9'(B | slug flow liquid-liquid two-phase flow
| 2-a | 336 |
| 15:40$B!A(B 16:00 | A121 | $B1UE)$N5$1U3&LL$rDL$7$F$NG.0\F0$K5Z$\$9>xH/$N1F6A(B ($B5~Bg1!(B) $B!{(B($B3X(B)$BF#ED(B $B>4Mx(B$B!&(B($B5~Bg9)(B) ($B@5(B)$B9u@%(B $BNI0l(B$B!&(B($B@5(B)$B>.?9(B $B8g(B | Heat transfer Evaporation Droplet
| 2-a | 711 |
| (16:00$B!A(B16:40)$B!!(B($B:BD9(B $BJ?LnGnG7(B) |
| 16:00$B!A(B 16:20 | A122 | MPS$BK!$K$h$kJQ7A0\F0J*BNN.$l$N%7%_%e%l!<%7%g%s(B ($B@EBg9)(B) $B!{(B($B3X(B)$BCSC+(B $B?r(B$B!&(B($B%G%s%=!<%F%/%N(B) $B=)ED(B $BBg4n(B$B!&(B($B@EBg9)(B) ($B@5(B)$B@%Ln(B $BCi0&(B | MPS numerical simulation elastic body
| 2-a | 708 |
| 16:20$B!A(B 16:40 | A123 | $B6d%$%*%s$NEE6KH?1~$rH<$&6/@)3H;6(B ($B5~Bg(B) $B!{(B($B@5(B)$B2.Ln(B $BJ84](B | ion migration electrochemical reaction silver-water system
| 11-b | 355 |
| A$B2q>l(B $BBh(B2$BF|(B |
| (9:00$B!A(B10:00)$B!!(B($B:BD9(B $B0f>e5AO/(B) |
| 9:00$B!A(B 9:20 | A201 | $B%\%k%F%C%/%9%j%s%0$rH/@8$5$;$k%*%/%?%8%C%H$N:.9gFC@-(B ($BL>9)Bg(B) ($B@5(B)$B2CF#(B $BDw?M(B$B!&(B$B!{(B($B3X(B)$B86ED(B $B3H(B$B!&(B($B@5(B)$BB?ED(B $BK-(B$B!&(B($B@5(B)$BD9DE(B $BM:0lO:(B$B!&(B($BLnB<%^%$%/%m%5%$%(%s%9(B) ($B@5(B)$BCfC+(B $BE/<#(B | mixing new type impeller vortex ring
| 2-b | 215 |
| 9:20$B!A(B 9:40 | A202 | $B%N%s%(%l%a%s%H%_%-%5!<$N0z$-?-$P$7!&@^$j$?$?$_8z2L(B ($B7DXfBg1!(B) $B!{(B($B3X(B)$BHu8}(B $B>09'(B$B!&(B($B3X(B)$BQA(B $BA1Z_(B$B!&(B($B7DXfBgM}9)(B) ($B@5(B)$B?"ED(B $BMx5W(B | static mixer chaotic mixing visualization
| 2-b | 794 |
| 9:40$B!A(B 10:00 | A203 | Kenics$B%9%?%F%#%C%/%_%-%5!<$NFbItN.F02D;k2=(B ($B7DXfBg1!(B) $B!{(B($B3X(B)$BQA(B $BA1Z_(B$B!&(B($B3X(B)$BHu8}(B $B>09'(B$B!&(B($B7DXfBgM}9)(B) ($B@5(B)$B?"ED(B $BMx5W(B | static mixer chaotic mixing visualization
| 2-b | 795 |
| (10:00$B!A(B11:00)$B!!(B($B:BD9(B $B?"EDMx5W(B) |
| 10:00$B!A(B 10:20 | A204 | Kullback-Leibler$B>pJsNL$K4p$E$/:.9gG=$NI>2A(B ($B:eBg4p9)(B) $B!{(B($B3X(B)$B$B!&(B($B@5(B)$B0f>e(B $B5AO/(B | Kullback-Leibler divergence fluid mixing mixing ability
| 2-b | 335 |
| 10:20$B!A(B 10:40 | A205 | $BIT6Q0l3J;R$rMQ$$$?N%;6 ($B:eBg4p9)(B) $B!{(B($B3X(B)$B?9ED(B $BJ~9((B$B!&(B($B@5(B)$B0f>e(B $B5AO/(B | Mixing pattern Discrete mapping Error diffusion method
| 2-b | 356 |
| 10:40$B!A(B 11:00 | A206 | $BAj8_:nMQ$9$k(B2$B$D$N(BBelousov-Zhabotinsky$BH?1~7O$K$*$1$kF14|8=>](B ($B:eBg4p(B) $B!{(B($B3X(B)$BJ!K\(B $B9LJ?(B$B!&(B($B3X(B)$B2,ED(B $BJ8B@O/(B$B!&(B($B@5(B)$B0f>e(B $B5AO/(B | Belousov-Zhabotinsky reaction synchronization coupled-oscillation
| 2-b | 431 |
| (11:00$B!A(B12:00)$B!!(B($B:BD9(B $B9b669,;J(B) |
| 11:00$B!A(B 11:20 | A207 | $B:.9g%9%Z%/%H%k;XI8$K$h$kYxYBAuCV$N@-G=I>2A(B ($BEl9)Bg1!M}9)(B) $B!{(B($B3X(B)$BJR6M(B $B>-C#(B$B!&(B($B@5(B)$BBg@n86(B $B??0l(B$B!&(B($B@5(B)$B>.@n(B $B9@J?(B | mixing spectrum capacity index impeller
| 2-b | 85 |
| 11:20$B!A(B 11:40 | A208 | $B%Q%I%kMc3IYBAe$N@{2s%9%m%C%7%s%08=>]$K5Z$\$92sE>?t$N1F6A(B ($BK!@/Bg9)(B) $B!{(B($B3X(B)$BH<(B $B9/N4(B$B!&(B($B@5(B)$B?70f(B $BOB5H(B$B!&(B($B6&(B)$B4d86(B $B8wCK(B$B!&(B($B6&(B)$BD9>>(B $B> | mixing rotary sloshing rotational number
| 2-b | 408 |
| 11:40$B!A(B 12:00 | A209 | $B%i%0%i%s%8%eN3;RDI@WK!$K4p$E$/3IYB7?>=@OAe$K$*$1$k7k>=>WFM8=>]$N?tCM2r@O(B ($B2#9qBg1!9)(B) $B!{(B($B3X(B)$BCf@>(B $BNIJe(B$B!&(B($B@5(B)$B;03Q(B $BN4B@(B$B!&(B($B@5(B)$B?N;V(B $BOBI'(B$B!&(B($B@5(B)$B>e%N;3(B $B<~(B | mixing Euler-Lagrange approach particle impact energy
| 2-b | 172 |
|
| (13:00$B!A(B13:40)$B!!(B($B:BD9(B $B;03QN4B@(B) |
| 13:00$B!A(B 13:20 | A213 | $BAeDl7A>u$N0[$J$k3IYBAe$K$*$1$kJP?43IYB(B ($B;37ABg1!M}9)(B) $B!{(B($B3X(B)$B<286(B $BBgJe(B$B!&(B($B@5(B)$B9b66(B $B9,;J(B | mixing eccentric impeller bottom shape
| 2-b | 184 |
| 13:20$B!A(B 13:40 | A214 | $BHsDj>o3IYBA`:n$K$*$1$k9bG4@-N.BN$N:.9g(B ($B;37ABg1!M}9)(B) $B!{(B($B3X(B)$B7*:e(B $B0l@.(B$B!&(B($BBgF|K\%$%s%-(B) ($B@5(B)$B4X:,(B $B6Q(B$B!&(B($B;37ABg1!M}9)(B) ($B@5(B)$B9b66(B $B9,;J(B | mixing unsteady mixing high viscosity
| 2-b | 198 |
| A$B2q>l(B $BBh(B3$BF|(B |
| (9:00$B!A(B10:00)$B!!(B($B:BD9(B $BB@ED8w9@(B) |
| 9:00$B!A(B 9:20 | A301 | $B5$K"Ec$N%,%9%[!<%k%I%"%C%W$KBP$9$kEc$N79 ($B?@F`@n9)Bg9)(B) $B!{(B($B@5(B)$B;32<(B $BJ!;V(B$B!&(B$BNkLZ(B $BCRG7(B | Bubble Column Gas Holdup Simulation
| 2-d | 59 |
| 9:20$B!A(B 9:40 | A302 | $B5$K"Ec$N%,%9%[!<%k%I%"%C%W$KBP$9$k%,%9$N ($B?@F`@n9)Bg9)(B) $B!{(B($B@5(B)$B;32<(B $BJ!;V(B$B!&(B$BC]NS(B $B5.;V(B$B!&(B$BCfEg(B $B0&(B | Bubble Column Gas holdup He gas
| 2-d | 60 |
| 9:40$B!A(B 10:00 | A303 | $B= ($BEl9)Bg1!M}9)(B) $B!{(B($B@5(B)$BBg@n86(B $B??0l(B$B!&(B$B:4F#(B $BM42p(B$B!&(B($B@5(B)$B>.@n(B $B9@J?(B | packed bed visualization VOF
| 2-d | 300 |
| (10:00$B!A(B11:00)$B!!(B($B:BD9(B $B;{:d9(0l(B) |
| 10:00$B!A(B 10:20 | A304 | $B3&LL3h@-:^$N%*%>%sJ,2r$N(Bsimulation ($B?@F`@n9)Bg9)(B) $B!{(B($B@5(B)$B;32<(B $BJ!;V(B$B!&(B$BNkLZ(B $BCRG7(B$B!&(B($B%"%s%7%9(B) $B>.NS(B $B<# | Bubble Column Ozone decomposition Simulation
| 2-d | 61 |
| 10:20$B!A(B 10:40 | A305 | $BC` ($B=;M'2=3X(B) $B!{(B($BIt(B)$BEgED(B $BD>$B!&(B($B6&(B)$B@FLZ(B $BM}F`(B$B!&(B($B?@8MBg(B) ($B6&(B)$BIZ;3(B $BL@CK(B | Computational Fluid Dynamics Bubble column Chemical Reaction
| 2-d | 193 |
| 10:40$B!A(B 11:00 | A306 | $BG4@-N.BNCf$r>e>:$9$k%9%+!<%H7?5$K"(B/$B1UE)$N?tCM2r@O(B ($B<$B!&(B($B@5(B)$B5HED(B $BK-(B$B!&(B(Florida State U.) ($B@5(B)Sussman M. | skirted shape bubble/dorp rise motion numerical analysis
| 2-d | 241 |
| (11:00$B!A(B12:00)$B!!(B($B:BD9(B $Bc7F#N4G7(B) |
| 11:00$B!A(B 11:20 | A307 | $BD62;GH>H ($B7DXfBgM}9)(B) $B!{(B($B@5(B)$B>.NS(B $BBgM4(B$B!&(B$B:4Ln(B $B0l$B!&(B($B@5(B)$B;{:d(B $B9(0l(B | Ultrasound Microbubble Agglomeration
| 2-d | 255 |
| 11:20$B!A(B 11:40 | A308 | $B5$1U:.9g$;$sCGJ}<0$K$h$j@8@.$7$?%^%$%/%m!&%J%N%P%V%k$NFC@-(B ($BJ!;3Bg9)(B) $B!{(B($B@5(B)$B7*1d(B $B=SB@O:(B$B!&(B($B6(OB5!@_(B) $BDT(B $B9/9-(B | micro-nano bubble generation shear flow
| 2-d | 261 |
| 11:40$B!A(B 12:00 | A309 | $B%I%i%U%H%A%e!<%VIU$-5$K"Ec$K%^%$%/%m%P%V%k$rJ,;6$5$;$?>l9g$NN.F0FC@-(B ($BL>Bg1!9)(B) $B!{(B($B3X(B)$B2&(B $B1'Ht(B$B!&(B($B3X(B)$B?$B!&(B($B3X(B)$B5H>>(B $B?r(B$B!&(B($B@5(B)$B0BED(B $B7<;J(B$B!&(B($B@5(B)$B:dEl(B $BK'9T(B$B!&(B($BF|K\%j%U%!%$%s(B) ($B@5(B)$B@n@%(B $BBY?M(B | Micro-Bubble Bubble Colume Flow Characteristics
| 2-d | 270 |
|
| (13:00$B!A(B14:00)$B!!(B($B:BD9(B $B:dElK'9T(B) |
| 13:00$B!A(B 13:20 | A313 | $B05NO?6F0C&K"$G$N5$K">e>:$KM?$($kG4CF@-8z2L(B ($BL>9)Bg(B) $B!{(B($B3X(B)$BBg@P(B $BL@9a(B$B!&(B($B3X(B)$B;3ED(B $BM*2p(B$B!&(B($B3X(B)$B9bEg(B $BE0(B$B!&(B($B@5(B)$B4dED(B $B=$0l(B$B!&(B($B@5(B)$B?9(B $B=( | defoaming air bubble shear-thinning fluids
| 2-d | 375 |
| 13:20$B!A(B 13:40 | A314 | $B1?F0%(%M%k%.!<$NMpN.M"Aw9`$K4^$^$l$k%l%$%N%k%:1~NO$HMpN.6/EY$N4X78!<5$1U:.AjN.F0$K$*$1$k4sM?!<(B ($B:eBg1!(B) $B!{(B($B@5(B)Ueyama Korekazu | Reynolds stress bubble column gas holdup
| 2-d | 491 |
| 13:40$B!A(B 14:00 | A315 | 2$Be>:$9$kC10l5$K"$N%&%'!<%/05FC@-(B ($BF1;V$B!&(B($B3X(B)$B4d>k(B $B=(IW(B$B!&(B$B;MJ}(B $BOBLi(B$B!&(B($B@5(B)$B?9(B $B9/0](B | bubble wake numerical simulation pressure distribution
| 2-d | 788 |
| (14:00$B!A(B15:00)$B!!(B($B:BD9(B $BEZ203hH~(B) |
| 14:00$B!A(B 14:20 | A316 | $B5$K"Ec7?G]M\AuCV$rMQ$$$?%(%N%-%?%16];eBN$N1UBNG]M\(B ($BF`NI9b@l(B) $B!{(B($B@5(B)$B2O1[(B $B44CK(B$B!&(B$BBgLn(B $BfFB@(B$B!&(B$B2,66(B $BBnFA(B$B!&(B($B%_%h%7L};i(B) $B>>K\(B $BZjZu(B$B!&(B$B7,ED(B $BOBI'(B$B!&(B($B4X@>2=3X(B) ($B@5(B)$BLnED(B $B=(IW(B | bubble column mushroom submerged culture
| 2-d | 256 |
| 14:20$B!A(B 14:40 | A317 | $B6k7A5$K"Ec$K$*$1$kJ*2A(B ($B@EBg9)(B) $B!{(B($B3X(B)$BHu8}(B $B@5$B!&(B($B@EBg1!(B) ($B3X(B)$B?9@n(B $B9/0l(B$B!&(B($B;0I)2=3X%(%s%8%K%"%j%s%0(B) ($B@5(B)$BEDCf(B $B?-9((B$B!&(B($B@EBg9)(B) ($B@5(B)$B??ED(B $B=SG7(B$B!&(B($B@EBg1!(B) ($B@5(B)$Bc7F#(B $BN4G7(B | Two-Phase Flow Conductivity Meter F-TOP
| 2-d | 413 |
| 14:40$B!A(B 15:00 | A318 | $B%U%)%H%U%'%s%H%sH?1~$rMxMQ$7$?5$(B-$B1U7O(BVOC$B=hM}AuCV$N3+H/(B ($BElMNBg9)(B) $B!{(B($B3X(B)$BFAB<(B $B2m90(B$B!&(B$BCfEg(B $BMxF`(B$B!&(B($B@5(B)$B@n@%(B $B5A6k(B | Volatile Organic Compounds Photo-Fenton reaction bubble column
| 2-d | 502 |
| B$B2q>l(B $BBh(B1$BF|(B |
| (10:00$B!A(B11:00)$B!!(B($B:BD9(B $BLZKs8w@5(B) |
| 10:00$B!A(B 10:20 | B104 | $B47@-%U%#%k%?$NJ,5i@-G=$K5Z$\$9N3;RBO@Q$N1F6A(B ($B6bBtBg9)(B) $B!{(B($B3X(B)$BL>AR(B $B?p5*(B$B!&(B($B6bBtBg1!(B) ($B3X(B)$B?e>e(B $BM[2p(B$B!&(B($B@5(B)$B@%8M(B $B>OJ8(B$B!&(B($B@5(B)$BBgC+(B $B5H@8(B | nanoparticles inertial classification model filter
| 2-f | 63 |
| 10:20$B!A(B 10:40 | B105 | $B4%<0%5%$%/%m%s$NJ,5i@-G=$K5Z$\$91_?mBN7A>u$N1F6A(B ($B9-Bg9)(B) $B!{(B($B3X(B)$B@>B<(B $BMNM4(B$B!&(B($B@5(B)$B;3K\(B $BE0Li(B$B!&(B($B@5(B)$BJ!0f(B $B9qGn(B$B!&(B($B@5(B)$B5HED(B $B1Q?M(B | classification cyclone visualization
| 2-f | 359 |
| 10:40$B!A(B 11:00 | B106 | $BEE>l0u2C7?$N?edA$K$h$kN3;R$NJ,N%FC@-(B ($B9-Bg1!9)(B) ($B3X(B)$B6b8w(B $BCR;K(B$B!&(B($B@5(B)$BJ!0f(B $B9qGn(B$B!&(B($B@5(B)$B;3K\(B $BE0Li(B$B!&(B$B!{(B($B@5(B)$B5HED(B $B1Q?M(B | Wet-classification Separation size Water-sieve
| 2-f | 253 |
| (11:00$B!A(B12:00)$B!!(B($B:BD9(B $BJ!0f9qGn(B) |
| 11:00$B!A(B 11:20 | B107 | $B%S!<%:%_%k$rMQ$$$?9[J*$NJ4:U$K4X$9$k8&5f(B ($B;37ABg1!M}9)(B) $B!{(B($B3X(B)$B:4F#(B $B$B!&(B($B@5(B)$BLZKs(B $B8w@5(B$B!&(B($B@5(B)$BD9C+@n(B $B@/M5(B | grinding bead mill clay
| 2-f | 534 |
| 11:20$B!A(B 11:40 | B108 | $BJ4F}$N05=L@.7?BN$N@=B$K!$H$=$NFC@-(B ($BL@<#F}6H(B) $B!{BgDZ(B $BOB8w(B$B!&(B$B$B!&(B($B@5(B)$BK-ED(B $B3h(B | Milk Powder Solid Milk Tablet
| 2-f | 293 |
| 11:40$B!A(B 12:00 | B109 | $BC:;@%+%k%7%&%`HyN3;R$N5[CeFC@-$K4X$9$k8&5f(B ($B?@8MBg1!(B) $B!{(B($B@5(B)$BKY0f(B $BM[Je(B$B!&(B($B?@8MBg1!9)(B) ($B@5(B)$B8VED(B $B1YG7(B$B!&(B($B@5(B)$BNkLZ(B $BMN(B$B!&(B($B@5(B)$BGv0f(B $BMN4p(B | Fine particle AFM Thixotropy model
| 2-f | 346 |
|
| (13:00$B!A(B14:00)$B!!(B($B:BD9(B $B>>:d=$Fs(B) |
| 13:00$B!A(B 13:20 | B113 | $B05NO6nF0N.$l$K$*$1$k9bG;EY1UAj%J%NN3;R7O$N<+8JAH?%2=(B ($BElBg1!9)(B) $B!{(B($B3X(B)$B??Ln(B $BNCJ?(B$B!&(B($B@5(B)$B0p_7(B $B?8(B$B!&(B($B@5(B)$BF#ED(B $B>;Bg(B$B!&(B($B@5(B)$B;38}(B $BM34tIW(B | nanoparticle pressure-driven flow self-organization
| 2-f | 464 |
| 13:20$B!A(B 13:40 | B114 | $B?e$*$h$S(BPBS$BCf$K$*$1$k%U%i!<%l%sN3;R$N6E=8!&J,;6(B ($B;:Am8&(B) $B!{(B($B@5(B)$B1sF#(B $BLP$B!&(B$B4](B $B=g;R(B$B!&(B$BFbED(B $BK.IW(B | fullerene dispersion PBS
| 2-f | 493 |
| 13:40$B!A(B 14:00 | B115 | $B%9%/%j%e!<%U%#!<%@!uBV2r@O(B ($B;37ABg1!M}9)(B) $B!{(B($B3X(B)$BH<:_(B $B7rB@(B$B!&(B($B@5(B)$BLZKs(B $B8w@5(B$B!&(B($B@5(B)$BD9C+@n(B $B@/M5(B | Discrete Element Method Screw feeder Angle of repose
| 2-f | 586 |
| (14:00$B!A(B15:20)$B!!(B($B:BD9(B $B2CG<=cLi(B) |
| 14:00$B!A(B 14:20 | B116 | $BN.BN(B-$B%S!<%:5sF0%7%_%e%l!<%7%g%s$K$h$kG^BN3IYB%_%kFb%(%M%k%.! ($BF1;V1:(B $BBY2p(B$B!&(B($B3X(B)$BOFED(B $BM'5.;R(B$B!&(B$B!{(B($B@5(B)$B2<:d(B $B8|;R(B$B!&(B($B@5(B)$BGr@n(B $BA19,(B$B!&(B($B@5(B)$BF|9b(B $B=E=u(B | Stirred media mill Dispersion LES-DEM Simulation
| 2-f | 627 |
| 14:20$B!A(B 14:40 | B117 | $BJ?9TJ?HDEE6K$K$h$kJ4BN$NK`;$BSEE%a%+%K%:%`$N2r@O(B ($B5~Bg(B) $B!{(B($B3X(B)$BA0Cf(B $B9a?%(B$B!&(B$B4dC+(B $B7rEM(B$B!&(B($B@5(B)$B>>:d(B $B=$Fs(B | tribo-charging electric-field particle shear stress
| 2-f | 309 |
| 14:40$B!A(B 15:00 | B118 | $BHyN3;R6E=8BN8GM-$N05=LJQ7AFC@-$K4X$9$k ($B:eI\Bg1!9)(B) $B!{(B($B3X(B)$BCv8}(B $B9d(B$B!&(B($B@5(B)$B?y2,(B $B7r0l(B$B!&(B($B@5(B)$BDMED(B $BN4IW(B$B!&(B($BElBg1!9)(B) ($B@5(B)$BF#ED(B $B>;Bg(B$B!&(B($B@5(B)$B;38}(B $BM34tIW(B | Particle aggregates Mechanical properties Compression test
| 2-f | 319 |
| 15:00$B!A(B 15:20 | B119 | $BB?Aj8rN.EE3&$K$*$1$kBSEEHyN3;R$NHy;kE*5sF04Q;!(B ($B5~Bg9)(B) $B!{(B($B3X(B)$B;{@>(B $B0l53(B$B!&(B($B3X(B)$BCfED(B $B8-;V(B$B!&(B($B@5(B)$B4];3(B $BGnG7(B$B!&(B($B@5(B)$B>>:d(B $B=$Fs(B | charged particle electrostatic force multi-phase
| 2-f | 121 |
| (15:20$B!A(B16:20)$B!!(B($B:BD9(B $BDMEDN4IW(B) |
| 15:20$B!A(B 15:40 | B120 | $B8zN(E*$JHyJ4:U$r2DG=$K$9$kYxYB%_%k$N2sE>%m!<%?7A>u(B ($BElKLBgB?858&(B) $B!{A>ED(B $BNO1{(B$B!&(B($B@5(B)$B2CG<(B $B=cLi(B$B!&(B($B@5(B)$Bc7F#(B $BJ8NI(B | stirred mill grinding performance simulation
| 2-f | 371 |
| 15:40$B!A(B 16:00 | B121 | $BBP8~N.:.9gJ}<0$rMQ$$$?5$Aj?(G^(BCVD$BK!$K$h$k(BCNT$B$N9g@.(B ($B6bBtBg1!<+(B) $B!{(B($B3X(B)$B;3K\(B $B5W;L(B$B!&(B($B3X(B)$B>>K\(B $BN$B!&(B($B6bBtBg9)(B) ($B3X(B)$B@u0f(B $B0lI'(B$B!&(B($B6bBtBg1!<+(B) ($B@5(B)$B@%8M(B $B>OJ8(B$B!&(B($B@5(B)$BBgC+(B $B5H@8(B$B!&(B($B;:Am8&(B) ($B@5(B)$BJ?_7(B $B@?0l(B | Carbon nanotube Chemical vapor deposition method aerosol
| 2-f | 348 |
| 16:00$B!A(B 16:20 | B122 | $B>F5QHt3%!"2HC\9|J4$r:F;q8;2=$7$?9b%W%m%H%sEEF3Kl$rMQ$$$?G3NAEECS$NH/EEFC@-(B ($B9-Bg9)(B) $B!{(B($B@5(B)$BJ!0f(B $B9qGn(B$B!&(B($B3X(B)$BLZ8M8}(B $BAo(B$B!&(B($B3X(B)$BM-K~(B $BD>$B!&(B($B@5(B)$B;3K\(B $BE0Li(B$B!&(B($B@5(B)$B5HED(B $B1Q?M(B | Fast proton conductor Incineration ash Fuel cell
| 2-f | 251 |
| B$B2q>l(B $BBh(B2$BF|(B |
| (9:40$B!A(B11:00)$B!!(B($B:BD9(B $B5H@n;KO:(B) |
| 9:40$B!A(B 10:00 | B203 | $B8w%U%!%$%P!<%W%m!<%VK!$K$h$kHy>.1UE)$N7WB,@:EY(B ($B@EBg9)(B) $B!{(B($B3X(B)$B>>ED(B $B7KJe(B$B!&(B($B@EBg1!(B) ($B3X(B)$B>._7(B $BM$Je(B$B!&(B($B@EBg9)(B) ($B@5(B)$B??ED(B $B=SG7(B$B!&(B($BIM>>%[%H%K%/%9Cf1{8&(B) $BBg@P(B $B??8c(B$B!&(B$B@DEg(B $B?B0lO:(B$B!&(B($B@EBg1!(B) ($B@5(B)$Bc7F#(B $BN4G7(B | S-TOP(Single-Tip Optical fiber Probe) Micro-droplets Multiphase Flow
| 2-e | 414 |
| 10:00$B!A(B 10:20 | B204 | $B>x5$!&?e:.9gJ.N.$NFC@-I>2A(B ($B@EBg9)(B) $B!{(B($B3X(B)$B;066(B $BM$5,(B$B!&(B($B@5(B)$B??ED(B $B=SG7(B$B!&(B($B%"%/%"%5%$%(%s%9(B) $B;3@%(B $B2mCK(B$B!&(B($B@EBg1!(B) ($B@5(B)$Bc7F#(B $BN4G7(B | steam-water mixture high-speed photography nozzle
| 2-e | 479 |
| 10:20$B!A(B 10:40 | B205 | $BEE5$N.BNNO3X$K$h$k(BEHD$B>.7?%]%s%W$N3+H/(B ($B@iMUBg1!<+(B) $B!{(B($B3X(B)$B?y;3(B $BGn><(B$B!&(B($B@iMUBg9)(B) ($B@5(B)$B>.AR(B $BM5D>(B$B!&(B($B@5(B)$BBgDZ(B $BBYJ8(B | electrohydrodynamics pumping herringbone pattern
| 2-e | 95 |
| 10:40$B!A(B 11:00 | B206 | $B5kErMQF]$K5Z$\$9Hy:Y5$K"$N1F6A(B ($BL>Bg1!9)(B) $B!{(B($B3X(B)$B>>2,(B $BN<(B$B!&(B($B@5(B)$B0BED(B $B7<;J(B$B!&(B($B@5(B)$B:dEl(B $BK'9T(B$B!&(B($B=;M'7Z6bB09)6H(B) $BNkLZ(B $BG&(B$B!&(B$B;3ED(B $BK-(B$B!&(B$B2OLn(B $B9@;0(B | Copper Tube Erosion Corrosion Micro-Bubble
| 2-e | 186 |
| (11:00$B!A(B12:00)$B!!(B($B:BD9(B $B0BED7<;J(B) |
| 11:00$B!A(B 11:20 | B207 | $BHy>.6k7AN.O)$K$*$1$k5$1U%KAjN.$NN.F0>uBV(B ($BEl9)Bg9)(B) $B!{(B($B3X(B)$B0f>e(B $B=a0l(B$B!&(B($BEl9)Bg1!M}9)(B) ($B@5(B)$B5H@n(B $B;KO:(B | gas-liquid two-phase flow rectangular micro-channels flow pattern
| 2-e | 333 |
| 11:20$B!A(B 11:40 | B208 | PIV$B5Z$S(BLIF$BK!$K$h$k%8%0%6%0>e>:5$K"$N<~0O1UAj1?F0$HMO2r2aDx$NF1;~7WB,(B ($B@EBg9)(B) $B!{(B($B3X(B)$B;3K\(B $B3X(B$B!&(B($B@EBg1!(B) $B;3ED(B $B2m?M(B$B!&(B($B@EBg9)(B) ($B@5(B)$B??ED(B $B=SG7(B$B!&(B($B@EBg1!(B) ($B@5(B)$Bc7F#(B $BN4G7(B | PIV LIF bubble
| 2-e | 411 |
| 11:40$B!A(B 12:00 | B209 | $B?6F03J;RMpN.>l$K$*$1$k5$K"72:.F~$K$h$k%(%M%k%.! ($B@EBg9)(B) $B!{(B($B3X(B)$B6b(B $B3Xo.(B$B!&(B($B@EBg1!(B) ($B3X(B)$B?9@n(B $B9/0l(B$B!&(B($B@EBg9)(B) ($B@5(B)$B??ED(B $B=SG7(B$B!&(B($B@EBg1!(B) ($B@5(B)$Bc7F#(B $BN4G7(B | Oscillating-grid turbulence Bubble swarm Turbulence characteristics
| 2-e | 490 |
| B$B2q>l(B $BBh(B3$BF|(B |
| (9:00$B!A(B10:00)$B!!(B($B:BD9(B $BLnEDNh<#(B) |
| 9:00$B!A(B 9:20 | B301 | $B;@2=%A%?%s8w?(G^N.F0AX$K$*$1$kC&>KFC@-(B ($BIY;3Bg1!(B) $B!{(B($B@5(B)$B;3yu(B $BNLJ?(B$B!&(B$B>.;3(B $BM5Li(B$B!&(B$BCf0f(B $BK-(B$B!&(B$B5H86(B $BM4Li(B$B!&(B($B@5(B)$BN-(B $B5.7D(B$B!&(B($B@5(B)$B9u2,(B $BIp=S(B | Fluidized bed Denitration Photo catalyst
| 2-c | 27 |
| 9:20$B!A(B 9:40 | B302 | $B?eJ??6F0>l$K$*$1$k?6F0%Q%i%a!<%?!<$,5$K"FC@-$K5Z$\$91F6A(B ($B6e9)Bg9)(B) $B!{C]K\(B $BOB;J(B$B!&(B($B@5(B)$BGOEO(B $B2B=((B$B!&(B($B@5(B)$B;3B<(B $BJ}?M(B$B!&(B($B@5(B)$B | fuidization vibration bubble
| 2-c | 268 |
| 9:40$B!A(B 10:00 | B303 | Geldart$B$N(BA$BN3;R$N1tD>?6F0>l$K$*$1$kN.F02=FC@-$K4X$9$k8&5f(B ($B6e9)Bg9)(B) $B!{(B($B@5(B)$BGOEO(B $B2B=((B$B!&(B$B?9Ln(B $B@590(B$B!&(B$BBgC+(B $BZe(B$B!&(B($B@5(B)$B;3B<(B $BJ}?M(B$B!&(B($B@5(B)$B | fluidized bed vibration
| 2-c | 519 |
| (10:00$B!A(B11:00)$B!!(B($B:BD9(B $BGOEO2B=((B) |
| 10:00$B!A(B 10:20 | B304 | $B%I%i%U%H%A%e!<%VIU$-2~NI7?J.N.AX$NN.F0FC@-(B ($BJ!2,Bg9)(B) $B!{(B($B@5(B)$B1JEg(B $BBg(B$B!&(B($B@5(B)$B@Pi6(B $BMxJ8(B | spout-fluid bed gas bypassing solids circulation rate
| 2-c | 62 |
| 10:20$B!A(B 10:40 | B305 | $BB?@.J,7O1tD>4IFb8G1UFsAjN.F0AX$NN.F0FC@-(B ($B$B!&(B($B@5(B)$B?eED(B $B7I(B$B!&(B$B4d8M(B $B@.98(B$B!&(B($B@5(B)$B>>K\(B $BMxC#(B | fluidized bed multiple components two phase flow
| 2-c | 678 |
| 10:40$B!A(B 11:00 | B306 | $BN.F0AXG.=hM}$K$h$kFs;@2=%A%?%s$NCbAG%I!<%W$K5Z$\$986NA$N1F6A(B ($B72Bg1!9)(B) $B!{(B($B@5(B)$BCfN$(B $BJY(B$B!&(B$B0$It(B $BM42p(B$B!&(B($B@5(B)$BLnED(B $BNh<#(B$B!&(B($B@5(B)$BCf@n(B $B?B9%(B | titanium dioxide particle size fluidized bed
| 2-c | 780 |
| (11:00$B!A(B12:00)$B!!(B($B:BD9(B $BCfN$(B $BJY(B) |
| 11:00$B!A(B 11:20 | B307 | $B%]%j%(%9%F%k=E9g4o$NN.F05sF0$K4X$9$kAj;wB'$N8!>Z(B ($BF|N)(B) $B!{(B($B@5(B)$B2,(B $B7{0lO:(B$B!&(B($B@5(B)$B>>Hx(B $B=SL@(B$B!&(B($B@5(B)$B>e@n(B $B>-9T(B$B!&(B($BF|N)%W%i%s%H%F%/%N%m%8!<(B) $B2,K\(B $B@.63(B$B!&(B$B:4@$(B $B9/@.(B | flow behavior similarity law impulse response
| 2-g | 73 |
| 11:20$B!A(B 11:40 | B308 | $BJ,;RF0NO3X$H(BCFD$B$NO"7k%7%_%e%l!<%7%g%s$N%b%G%k(B ($B5~Bg9)!&2=9)(B) $B!{(B($B@5(B)$B0BED(B $B=$8g(B$B!&(B($B@5(B)$B;3K\(B $BNL0l(B | softmatter multiscale simulation
| 2-g | 248 |
| 11:40$B!A(B 12:00 | B309 | $B9bEE052<$K$*$1$k(Bwater bridge$B$N@8@.(B ($BK!@/9)Bg1!(B) $B!{(B($B3X(B)$BK\ED(B $BJ87I(B$B!&(B($B@5(B)$B@>3$(B $B1QM:(B | water bridge
| 2-g | 578 |
|
| (13:00$B!A(B13:40)$B!!(B($B:BD9(B $B0BED=$8g(B) |
| 13:00$B!A(B 13:20 | B313 | $B8GDjH/@88;$+$i$N(BPM10/2.5$BGS=P5sF0B,DjMQ$H$7$F$N%(%"%m%>%kJ,5i ($B@P@n9b@l(B) $B!{(B($B@5(B)$BOBED(B $B6);J(B$B!&(B($B:eBg(B) ($B@5(B)$B6aF#(B $B8w(B$B!&(B($B%&%#!<%sBg(B) ($B@5(B)Szymanski W. W.$B!&(B($BElG@9)Bg(B) ($B@5(B)$BDMED(B $B$^$f$_(B$B!&(B($B@5(B)Lenggoro W.$B!&(B($B=P8w6=;:(B) ($B@5(B)$BF#86(B $B>0$B!&(B($B;:Am8&(B) ($B@5(B)$B>.Jk(B $B?.G7(B$B!&(B($B:eBg(B) ($B@5(B)$BFbF#(B $BKRCK(B$B!&(B($B@P@n9b@l(B) ($B@5(B)$B6b2,(B $B@i2ECK(B$B!&(B($BElG@9)Bg(B) ($B@5(B)$B?@C+(B $B=(Gn(B | PM10/PM2.5 virtual impactor cascade impactor
| 2-g | 770 |
| 13:20$B!A(B 13:40 | B314 | $B2V2&$K$*$1$kJ4?PGzH/KI;_BP:v(B ($B2V2&(B) $B!{Ln85(B $B=(Mx(B$B!&(B($B@5(B)$B;M==J*(B $B@6(B$B!&(B$B>.NS(B $BDgIW(B | risk accessment
| 2-g | 830 |