1991
DOI: 10.1146/annurev.fl.23.010191.002213
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Incompressible Fluid Dynamics: Some Fundamental Formulation Issues

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Cited by 360 publications
(230 citation statements)
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“…A 33 point equallength finite-difference grid in the vertical provided an economic compromise between the resolution needs of the boundary layers and those of the long-range fluxes. We worked with the equations of motion in their biharmonic form (1)- (3) rather than the more traditional streamfunction-vorticity formulation in order to avoid (a) inversion of the Poisson operator, and (b) difficulties arising from the coupling between the stream function and vorticity [12]. These are associated with the peculiar nature of the boundary conditions for the stream function • and the initial conditions on the vorticity w, which lacks boundary conditions [13].…”
Section: 0x104mentioning
confidence: 99%
“…A 33 point equallength finite-difference grid in the vertical provided an economic compromise between the resolution needs of the boundary layers and those of the long-range fluxes. We worked with the equations of motion in their biharmonic form (1)- (3) rather than the more traditional streamfunction-vorticity formulation in order to avoid (a) inversion of the Poisson operator, and (b) difficulties arising from the coupling between the stream function and vorticity [12]. These are associated with the peculiar nature of the boundary conditions for the stream function • and the initial conditions on the vorticity w, which lacks boundary conditions [13].…”
Section: 0x104mentioning
confidence: 99%
“…In this case, the boundary conditions imposed at the top and the bottom are zero normal velocity (no-penetration) and zero normal derivative of the horizontal velocities (free-slip) and the scalar field χ (adiabatic). The Neumann boundary conditions for the Poisson equation for the pressure at the top and the bottom are then [26] ∂ p ∂z = 1 Re…”
Section: Numerical Algorithmsmentioning
confidence: 99%
“…A discussion and analysis of the various forms of incompressible Navier-Stokes equations can be found for instance in [13,18,22]. Let Ω be a bounded domain in R 2 or R 3 , we assume that Ω contains regular obstacles the reunion of which is called Ω s .…”
Section: Preliminariesmentioning
confidence: 99%