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The hydrodynamics of a magnetoelectrolytic cell

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Abstract

The characteristics of induced flow in a cylindrical magnetoelectrolytic cell under the influence of uniform and non-uniform magnetic fields are analysed. Experimental surface velocity values are predicted with reasonable accuracy by magnetohydrodynamic models incorporating open-channel flow concepts.

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Abbreviations

A, D :

parameters in Equation 7 [Gak equation]

B :

magnetic flux density vector;B r,B z its radial and axial components;B 0 its magnitude, ¯B its average magnitude

B 1 (pr) :

auxiliary function in the annular Hankel transform technique (Equation 6)

e :

unit vectors in the cylindrical coordinate system with componentse r,e o,e z

F θ :

magnitude of the MHD force density in theθ-direction

f c :

friction coefficient of energy loss due to curvature

g :

acceleration due to gravity

H :

height of the electrodes in electrolytic cell

h f :

energy head loss due to friction

h c :

energy head loss due to curvature

I :

electric current flow

J :

electric current density vector

K :

lumped parameter;K=IB o/2πHη

K f,K c :

K factors in terms of friction and curvature losses

k :

geometric shape factor,R/r o

P :

pressure

p :

annular Hankel transform parameter

R :

radius of the outer electrode

r o :

radius of the inner electrode

r :

radius measured from the centre of the electrolytic cell

V gq :

velocity in theθ-direction

¯V θ :

its average

α n :

regression coefficients in Equation 13

η :

dynamic viscosity of electrolyte

gn :

kinematic viscosity of electrolyte

ρ :

density of electrolyte

φ(p) :

function defined in Equation 8a

ψ(r) :

surface profile function (Equation 29)

References

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Mohanta, S., Fahidy, T.Z. The hydrodynamics of a magnetoelectrolytic cell. J Appl Electrochem 6, 211–220 (1976). https://doi.org/10.1007/BF00616143

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