1980
DOI: 10.1143/jpsj.49.2091
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Magnetohydrodynamical Flow with Hall Effects, Past an Infinite Porous Plate and Heat Transfer

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Cited by 3 publications
(2 citation statements)
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“…The plates of the channel are at y = ±h and that the relative velocity between the two plates is 2u 0 and also, there is no pressure gradient in the flow field. The uniform magnetic field B 0 makes an angle θ with Xaxis induced a magnetic field B(y) or the imposed magnetic field makes an angle θ to the free stream velocity [1,2]. The plate at y = −h is maintained at temperature T 0 , while the other plate y = +h is kept at temperature T 1 (T 1 > T 0 ) and the plates are electrically non-conducting.…”
Section: Formulation Of the Problemmentioning
confidence: 99%
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“…The plates of the channel are at y = ±h and that the relative velocity between the two plates is 2u 0 and also, there is no pressure gradient in the flow field. The uniform magnetic field B 0 makes an angle θ with Xaxis induced a magnetic field B(y) or the imposed magnetic field makes an angle θ to the free stream velocity [1,2]. The plate at y = −h is maintained at temperature T 0 , while the other plate y = +h is kept at temperature T 1 (T 1 > T 0 ) and the plates are electrically non-conducting.…”
Section: Formulation Of the Problemmentioning
confidence: 99%
“…Borkakati and Bharali [1] have discussed the flow and heat transfer between two horizontal parallel plates, where the lower plate is a stretching sheet and the upper one is a porous solid plate in the presence of a transverse magnetic field. The heat transfer in an axisymmetric flow between two parallel porous disks under the effect of a transverse magnetic field is studied by Bharali and Borkakati [2].…”
Section: Introductionmentioning
confidence: 99%