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| \phi \cdot c_t \cdot \partial_t p + \nabla {\bf u}
= \sum_k q_k(t) \cdot \delta({\bf r}-{\bf r}_k) |
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| {\bf u} = - M \cdot ( \nabla p - \rho \, {\bf g}) |
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| anchor | qGamma |
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| alignment | left |
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| \int_{\Gamma} \, {\bf u} \, d {\bf \Sigma} = q_\Gamma(t) |
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| or |
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| \phi \cdot c_t \cdot \partial_t p + \nabla {\bf u} = 0 |
| | LaTeX Math Block |
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| {\bf u} = - M \cdot ( \nabla p - \rho \, {\bf g}) |
| | LaTeX Math Block |
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| \int_{\Sigma_k} \, {\bf u} \, d {\bf \Sigma} = q_k(t) |
| | LaTeX Math Block |
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| anchor | qGamma |
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| alignment | left |
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| \int_{\Gamma} \, {\bf u} \, d {\bf \Sigma} = q_\Gamma(t) |
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| or |
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| \phi \cdot c_t \cdot \partial_t p =
\nabla \big( M \cdot ( \nabla p - \rho \, {\bf g}) \big) |
| | LaTeX Math Block |
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| \int_{\Sigma_k} \, {\bf u} \, d {\bf \Sigma} = q_k(t) |
| | LaTeX Math Block |
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| anchor | qGamma |
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| alignment | left |
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| \int_{\Gamma} \, {\bf u} \, d {\bf \Sigma} = q_\Gamma(t) |
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See also
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Physics / Mechanics / Continuum mechanics / Fluid Mechanics / Fluid Dynamics / Pressure Diffusion / Pressure Diffusion @model / Single-phase pressure diffusion @model
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