Navier-Stokes equations
Continuity
or, using the substantive derivative:
For an incompressible fluid, is constant, hence the velocity field must be divergence-free:
Momentum
(Also known as the Navier-Stokes equation.)
or, using the substantive derivative:
where is a volumetric force (e.g. Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \rho g} for gravity), and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \mathbb{T} } is the stress tensor.
The vector quantity Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \nabla \cdot\mathbb{T} } is the shear stress. For a Newtonian incompressible fluid,
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \nabla \mathbb{T} = \mu \nabla^2 \mathbf{v}, }
with Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \mu} being the (dynamic) viscosity.
For an inviscid fluid, the momentum equation becomes Euler's equation for ideal fluids:
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \rho \left(\frac{D \mathbf{v}}{D t} \right) = -\nabla p + \mathbf{f} . }