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mathematical models for biomagnetic fluid flow and applications

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In all the above cases the magnetization M o is dependent on the temperature T of the<br />

<strong>fluid</strong>. In such a case (non-isothermal case), it is also necessary to consider in the<br />

<strong>mathematical</strong> model, describing the problem under consideration, the energy equation<br />

containing the temperature T of the <strong>fluid</strong>. This equation can be written as [8]<br />

DT ∂M<br />

<br />

o<br />

2<br />

ρ Cp<br />

+µ<br />

oT ⎡V⋅( ∇ H) ⎤ = k∇ T+<br />

ηΦ<br />

(12)<br />

Dt ∂T<br />

⎣ ⎦<br />

where k is the coefficient of thermal conductivity of the <strong>fluid</strong>, C p the specific heat <strong>and</strong> Φ the<br />

dissipation function.<br />

4. APPLICATIONS<br />

Biomagnetic <strong>fluid</strong> <strong>flow</strong> in a Channel<br />

As a simple, but representative, application of <strong>biomagnetic</strong> <strong>fluid</strong> <strong>flow</strong> we consider the steady<br />

two-dimensional laminar <strong>flow</strong> of an incompressible viscous <strong>biomagnetic</strong> <strong>fluid</strong> (blood) in a<br />

space between two parallel flat plates (channel). The length of the plates is L <strong>and</strong> the distance<br />

between them is h (h

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