The variable is a rotating-flow pressure potential including the conservative body-force and centrifugal potentials. For constant mass density,up to an additive function of time, where is any imposed conservative potential. The last term is the centrifugal potential; its negative gradient is the centrifugal acceleration. The Coriolis force remains explicit in the equation because it is velocity-dependent and cannot be absorbed into a scalar position potential.
The further constraint is incompressible flow:For the specified shear, and . Its Coriolis acceleration is , so the corresponding total basic pressure potential can be chosen as . This supplies the force balance required for the basic state used below.
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