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Viscous lifting and drainage of a conducting fluid in the presence of a transverse magnetic field

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Abstract

A theoretical investigation of the effects of a transverse magnetic field on the combined problem of viscous lifting and drainage of a conducting fluid on a plate is presented. The effects of inertia and transverse magnetic field on the liquid film thickness is studied for two cases namely a plate withdrawn with a constant velocity and one withdrawn with a constant acceleration. The expressions for the flow rate and the free surface profiles are obtained for the above two cases. It is found that the free surface profiles are convex in nature as in the non-magnetic case thus showing that the inertia does not effect the general pattern of flow, and the effect of the magnetic field is to retard both the lifting and drainage of the fluid.

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Abbreviations

a :

acceleration of the plate

A :

dimensionless acceleration,=a/g

B 0 :

transverse magnetic field

g :

acceleration due to gravity

h :

film thickness

H :

dimensionless film thickness,=h(g/ν 2)1/3

M :

Hartmann number,\( = \sqrt {{\sigma \mathord{\left/ {\vphantom {\sigma \mu }} \right. \kern-\nulldelimiterspace} \mu }} B_0 ({{v^2 } \mathord{\left/ {\vphantom {{v^2 } g}} \right. \kern-\nulldelimiterspace} g})^{\tfrac{1}{3}} \)

q :

mass flow rate

Q :

dimensionless mass flow rate,=q/ν

T :

dimensionless time,=t(g 2/ν)1/3

v 0 :

velocity of the plate

V 0 :

dimensionless velocity of the plate,=v 0/(νg)1/3

v :

fluid velocity

(x, y, z):

cartesian coordinates

Y :

dimensionlessy-coordinate,=y(g/ν 2)1/3

μ :

viscosity

σ :

conductivity

ρ :

density

ν :

kinematic viscosity,=μ/ρ

References

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Annapurna, N., Ramanaiah, G. Viscous lifting and drainage of a conducting fluid in the presence of a transverse magnetic field. Appl. Sci. Res. 31, 139–152 (1975). https://doi.org/10.1007/BF01795832

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  • DOI: https://doi.org/10.1007/BF01795832

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