$B9V1i(B $B;~9o(B | $B9V1i(B $BHV9f(B | $B9V1iBjL\!?H/I= | $B%-!<%o!<%I(B | $BJ,N`(B $BHV9f(B | $B |
---|---|---|---|---|---|
$BN3;R!&N.BN%W%m%;%9(B | |||||
(9:20$B!A(B10:20)$B!!(B($B:BD9(B $B;3K\!!NL0l(B) | |||||
D202 | $BG4@-N.BNCf$r<+M31?F0$9$kC10l1UE)$N0BDj@-(B | Drop rise motion Instability Nonlinear dynamics | 2-e | 57 | |
D203 | $B0lMM$JL.F0N.Cf$N5e7AN3;R$KF/$/93NO$NI>2A(B | drag force direct numerical simulation oscillating flow | 2-e | 310 | |
D204 | $B5<;wE*D>@\?tCM7W;;$K$*$1$k5eN3;R$NG4@-Dq93$*$h$S7A>uDq93$NDj<02=$H8!>Z(B | Macroscopic particle model Drag force Virtual mass force | 2-e | 492 | |
(10:20$B!A(B11:00)$B!!(B($B:BD9(B $BBg@n86!!??0l(B) | |||||
D205 | $BHyN3;RD@9_7O$K$*$1$kB.EYAj4X(B | Direct Numerical Simulation(DNS) Correlation Function Density Fluctuation | 2-e | 288 | |
D206 | $BMn2<5e$rMQ$$$?%2%k2=H?1~Cf$N%"%k%_%J%9%i%j!<$NG4EYI>2A(B | falling sphere viscosity alumina slurry | 2-e | 711 | |
(11:00$B!A(B12:00)$B!!(B($B:BD9(B $BB@ED!!8w9@(B) | |||||
D207 | Taylor-Couette$BN.$l$rMxMQ$7$?1U!98~N.1s?4Cj=PAuCV$N3+H/(B | centrifuge extractor Taylor-Couette flow counter-current | 2-e | 428 | |
D208 | $B%(%?%N!<%k$NG;=L$K8~$1$?D62;GHL82=!&Nd5Q2s<}%W%m%;%9$N9=C[(B | ultrasonic atomization ethanol separation mist recovery | 2-e | 550 | |
D209 | $B%+%i!<%O%$%9%T!<%I%+%a%i$rMQ$$$?Fs?'(BLIF$BK!$K$D$$$F(B | two-color LIF high-speed camera pH measurement | 2-e | 345 |