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Second order partial differential equation of parabolic type on the space-time field variable 

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bodyU{\rm w}(t, {\bf r})
:

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\beta({\bf r}, U{\rm w}) \cdot \frac{\partial U {\rm w}}{\partial t} = \nabla \left(  \alpha({\bf r}, U {\rm w})   \nabla U {\rm w} \right) +  f({\bf r}) 


where 

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bodyU{\rm w}(t, {\bf r})

space-time field variable

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body\alpha({\bf r}, U{\rm w})

mobility kinetic coefficient

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body{t}

time

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body\beta({\bf r}, U{\rm w})

capacitance kinetic coefficient

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body{\bf r} = (x,y,z)

Position vector

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body f({\bf r})

density of external forces

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\frac{\partial U {\rm w}}{\partial t} = D \cdot \Delta U {\rm w}

where 

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bodyD
 is called the diffusion coefficient.

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