mathematical models for biomagnetic fluid flow and applications
mathematical models for biomagnetic fluid flow and applications
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