Free convection effects on extracellular fluid in the presence of a transverse magnetic field

The model of the magnetohydrodynamic boundary-layer equations for a perfectly conducting micropolar fluid is established. This model is applied to study the effects of free convection currents with one relaxation time on the extracellular fluid (the internal environment) in the presence of a constant magnetic field. The state space approach developed in [M. Ezzat, Can. J. Phys. 1 (1994) 311; M. Ezzat, J. Appl. Math. Comput. 64 (1995) 191] is adopted for the one-dimensional problems including heat sources with one relaxation time. The resulting formulation is applied to a problem for the whole space with a plane distribution of heat sources. The reflection method together with the solution obtained for the whole space is applied to a semi-space problem with a plane distribution of heat sources located inside the fluid. This method was proposed by Nowacki in the context of coupled thermoelasticity. The Laplace transform technique is used. The inversion of the Laplace transforms is carried out using a numerical approach. Numerical results for the velocity, the induced electric and magnetic field, the electric current and the electric potential distributions are given and illustrated graphically for given problems.

[1]  M. Othman,et al.  A problem of a micropolar magnetohydrodynamic boundary- layer flow , 1999 .

[2]  T. Ariman On the analysis of blood flow. , 1971, Journal of biomechanics.

[3]  J. M. Coulson,et al.  Heat Transfer , 2018, A Concise Manual of Engineering Thermodynamics.

[4]  A. Eringen THEORY OF THERMO-MICRO-POLAR FLUIDS , 1972 .

[5]  A. Cemal Eringen,et al.  Theory of thermomicrofluids , 1972 .

[6]  M. Ezzat,et al.  Free convection effects on a viscoelastic boundary layer flow with one relaxation time through a porous medium , 1997 .

[7]  M. Ezzat,et al.  State space formulation to viscoelastic fluid flow of magnetohydrodynamic free convection through a porous medium , 1996 .

[8]  H. Lord,et al.  A GENERALIZED DYNAMICAL THEORY OF THERMOELASTICITY , 1967 .

[9]  H. Okino [Pulsatile blood flow]. , 1972, Kokyu to junkan. Respiration & circulation.

[10]  M. Mathur,et al.  Similarity solutions for laminar free convection flow of a thermomicropolar fluid past a non-isothermal vertical flat plate , 1981 .

[11]  A. Hodgkin,et al.  The influence of potassium and chloride ions on the membrane potential of single muscle fibres , 1959, The Journal of physiology.

[12]  A. L. Florence,et al.  Dynamic problems of thermoelasticity , 1975 .

[13]  M. Ezzat Free convection effects on perfectly conducting fluid , 2001 .

[14]  M. Ezzat State space approach to generalized magneto-thermoelasticity with two relaxation times in a medium of perfect conductivity , 1997 .

[15]  Ya. S. Podstrigach,et al.  Some dynamic problems of the thermoelasticity of thin shells , 1966 .

[16]  G. Honig,et al.  A method for the numerical inversion of Laplace transforms , 1984 .

[17]  A. Eringen,et al.  THEORY OF MICROPOLAR FLUIDS , 1966 .

[18]  M. Ezzat,et al.  State Space Approach to Viscoelastic Fluid Flow of Hydromagnetic Fluctuating Boundary‐Layer through a Porous Medium , 1997 .

[19]  S. J. Allen,et al.  Concentration effects in oscillatory blood flow. , 1969, Biorheology.