APS March Meeting 2017
Volume 62, Number 4
Monday–Friday, March 13–17, 2017;
New Orleans, Louisiana
Session V35: General Fluid Mechanics
2:30 PM–5:06 PM,
Thursday, March 16, 2017
Room: 298
Sponsoring
Units:
DFD DCMP
Chair: Saad Bhamla, Stanford University
Abstract ID: BAPS.2017.MAR.V35.2
Abstract: V35.00002 : DSMC Simulation of High Mach Number Taylor-Couette Flow
2:42 PM–2:54 PM
Preview Abstract
Abstract
Author:
Dr. Sahadev Pradhan
(Department of Chemical Engineering, Indian Institute of Science, Bangalore- 560 012, India.)
The main focus of this work is to characterise the Taylor-Couette flow of an
ideal gas between two coaxial cylinders at Mach number \textit{Ma }$=$\textit{ (U\textunderscore w / }$\backslash
$\textit{sqrt\textbraceleft kb T\textunderscore w / m\textbraceright )}in the range 0.01 \textless Ma \textless 10, and Knudsen number \textit{Kn }$=$\textit{ (1 / (}$\backslash
$\textit{sqrt\textbraceleft 2\textbraceright }$\backslash $\textit{pi d\textasciicircum 2 n\textunderscore d (r\textunderscore 2 - r\textunderscore 1))) }in the range 0.001 \textless Kn \textless 5, using
two-dimensional (2D) direct simulation Monte Carlo (DSMC) simulations. Here,
\textit{r\textunderscore 1}and \textit{r\textunderscore 2}are the radius of inner and outer cylinder respectively,
\textit{U\textunderscore w}is the circumferential wall velocity of the inner cylinder,
\textit{T\textunderscore w}is the isothermal wall temperature, \textit{n\textunderscore d}is the number density of the gas
molecules, $m$and $d$ are the molecular mass and diameter, and \textit{kb}is the Boltzmann
constant. The cylindrical surfaces are specified as being diffusely
reflecting with the thermal accommodation coefficient equal to one.
In the present analysis of high Mach number compressible Taylor-Couette flow
using DSMC method, wall slip in the temperature and the velocities are found
to be significant. Slip occurs because the temperature/velocity of the
molecules incident on the wall could be very different from that of the
wall, even though the temperature/velocity of the reflected molecules is
equal to that of the wall. Due to the high surface speed of the inner
cylinder, significant heating of the gas is taking place. The gas
temperature increases until the heat transfer to the surface equals the work
done in moving the surface. The highest temperature is obtained near the
moving surface of the inner cylinder at a radius of about (1.26
r\textunderscore 1).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2017.MAR.V35.2