$B:G=*99?7F|;~!'(B2023-05-13 03:59:01
$B$3$NJ,N`$G$h$/;H$o$l(B $B$F$$$k%-!<%o!<%I(B | $B%-!<%o!<%I(B | $B | |
---|---|---|---|
Particle suspension | 2$B7o(B | ||
physical meaning | 2$B7o(B | ||
uroflowmetry | 1$B7o(B |
$B | $B9V1iBjL\!?H/I=$B%-!<%o!<%I(B | $BH/I=7A<0(B | |
---|---|---|---|
12 | $B;@AG%U%!%$%s%P%V%k$O;@AG1?HBBN$H$7$F5!G=$9$k$N$+!)(B | Finebubbles Micro-nano bubbles Oxygen | O |
39 | $BN.BNCf$N1?F0NLM"Aw(B($B?t<0$N0UL#$9$kJ*M}E*8=>]$*$h$S6-3&>r7o(B) | Navier-Stokes equation, momentum physical meaning | O |
40 | $BN.BNCf$N3Q1?F0NLM"Aw(B($B?t<0$N0UL#$9$kJ*M}E*8=>]$*$h$S6-3&>r7o(B) | Equation of vorticity transport angular-momentum physical meaning | O |
41 | $B12EY$K4X$9$k6-3&>r7o$NM-MQ@-(B(Blasius$B$N;X4xJm?tCM2r(B) | boundary condition for vorticity Blasius's equation One-way calculation from surface to infinity | O |
140 | $BG"J.N.$N%7%_%e%l!<%7%g%s(B | uroflowmetry CFD jet | P |
375 | $BB?9& | Microfluidic device Particle separation Porous substrate | P |
429 | $B?M9)CNG=$rMQ$$$?9b@:EY2r@O$K$h$k(BiPS$B:YK&G]M\:GE,3IYB>r7o$NDs0F(B | PINNs Shear stress iPS cells | P |
455 | $BN3;R7|By1U$N$;$sCGN.$l$K4X$9$k3J;R%\%k%D%^%s%7%_%e%l!<%7%g%s(B | Particle suspension Lattice Boltzmann Method Viscosity | O |
549 | $BHsDj>oQrCGN.$l$K$*$1$kN3;R7|By1U$N | Unsteady shear Effective viscosity Particle suspension | P |
603 | $B5$1U3&LL$rM-$9$k2sE>1_E{FbN.$l$N?tCM%7%_%e%l!<%7%g%s(B | Liquid-gas interface Numerical simulation Mixing | O |
619 | $B8w%U%!%$%P!<%W%m!<%V$rMQ$$$?Kl8|7WB,$K$*$1$k3&LL7A>u$H7WB,@:EY$N4X78(B | Liquid film flow Optical-fiber-based Reflective Probe Thickness measurement | P |