TY - JOUR
T1 - Oscillatory magnetogasdynamic slip flow in a microchannel
AU - Agarwal, Ramesh K.
AU - Chusak, L.
N1 - Publisher Copyright:
© 2013, Springer Science+Business Media Dordrecht.
PY - 2014/2/1
Y1 - 2014/2/1
N2 - The problem of pressure-driven magnetogasdynamic (MGD) slip flow with small rarefaction through a long microchannel is considered. The flow is driven by a steady or oscillatory pressure gradient. The study of MGD flows in microchannels is of interest since they occur in many electromagnetic microscale devices. In obtaining the microfluidic solutions in the presence of a magnetic field, some additional physical, mathematical, and numerical issues need to be considered. These issues deal with the scaling laws for microscale MGD flows and the relevant parameters such as Mach number, Reynolds number, Hartmann number, magnetic Reynolds number, and Knudsen number. For planar constant area microchannels, it is possible to obtain the analytical solutions for both steady and oscillatory pressure-driven flows at low magnetic Reynolds numbers. The flow field is assumed to be quasi-isothermal, which is a good assumption in the absence of a strong electric field. As physically expected, at higher values of the magnetic field (that is at a higher Hartmann number) the velocity profile in the channel flattens, and the pressure varies nonlinearly along the channel.
AB - The problem of pressure-driven magnetogasdynamic (MGD) slip flow with small rarefaction through a long microchannel is considered. The flow is driven by a steady or oscillatory pressure gradient. The study of MGD flows in microchannels is of interest since they occur in many electromagnetic microscale devices. In obtaining the microfluidic solutions in the presence of a magnetic field, some additional physical, mathematical, and numerical issues need to be considered. These issues deal with the scaling laws for microscale MGD flows and the relevant parameters such as Mach number, Reynolds number, Hartmann number, magnetic Reynolds number, and Knudsen number. For planar constant area microchannels, it is possible to obtain the analytical solutions for both steady and oscillatory pressure-driven flows at low magnetic Reynolds numbers. The flow field is assumed to be quasi-isothermal, which is a good assumption in the absence of a strong electric field. As physically expected, at higher values of the magnetic field (that is at a higher Hartmann number) the velocity profile in the channel flattens, and the pressure varies nonlinearly along the channel.
KW - Flow in a microchannel
KW - Low-density rarefied flow
KW - Magnetogasdynamic flow
KW - Oscillatory flow
UR - http://www.scopus.com/inward/record.url?scp=84956759430&partnerID=8YFLogxK
U2 - 10.1007/s10665-013-9637-6
DO - 10.1007/s10665-013-9637-6
M3 - Article
AN - SCOPUS:84956759430
SN - 0022-0833
VL - 84
SP - 135
EP - 146
JO - Journal of Engineering Mathematics
JF - Journal of Engineering Mathematics
IS - 1
ER -