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Mathematical form of mass conservation of continuum body:

Integral formDifferential form
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\frac{d}{dt} \iiint_\Omega \rho \, dV =0
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\frac{\partial \rho}{\partial t} + \nabla (\rho \, {\bf u}) = 0

where

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body\rho

continuum body spatial density distribution

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body\bf u

continuum body spatial velocity distribution



For the stationary fluid flow:

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\frac{\partial \rho}{\partial t} = 0 \rightarrow  \nabla (\rho \, {\bf u}) = 0

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