Proceedings of the Third GAMM — Conference on Numerical Methods in Fluid Mechanics 1980
DOI: 10.1007/978-3-322-86146-7_17
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Treatment of Incompressibility and Boundary Conditions in 3-D Numerical Spectral Simulations of Plane Channel Flows

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Cited by 159 publications
(153 citation statements)
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“…Both the Kleiser-Schumann [14]and Kim-Moin-Moser [13] methods begin by substituting the truncated Fourier expansion of the velocity field u. The various Fourier modes are coupled through the nonlinear term.…”
Section: The Kim-moin-moser Equationsmentioning
confidence: 99%
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“…Both the Kleiser-Schumann [14]and Kim-Moin-Moser [13] methods begin by substituting the truncated Fourier expansion of the velocity field u. The various Fourier modes are coupled through the nonlinear term.…”
Section: The Kim-moin-moser Equationsmentioning
confidence: 99%
“…Instead, pressure is determined implicitly through the incompressibility constraint on the velocity field. One of the key algorithms for solving the Navier-Stokes equations in channel and plane Couette geometries is due to Kleiser and Schumann [14,1980]. Kleiser and Schumann introduced a numerical technique for enforcing the physically correct boundary conditions on pressure.…”
Section: Introductionmentioning
confidence: 99%
“…As the simulation focuses on the linear and weakly nonlinear dynamics, the de-aliasing of the nonlinear term in the spatial expansion of the solution is not of crucial importance and is omitted to decrease the computational cost. Owing to the assumption of a divergence-free flow, the influence matrix method, introduced in Kleiser & Schumann (1980, 1984, is used to evaluate the pressure and the velocity field; the pressure gradient in the Navier-Stokes equation then being discretized by an implicit Euler scheme. Finally, the buoyancy term is also discretized in time by an implicit Euler scheme, since the energy equation is solved before the Navier-Stokes equations.…”
Section: Numericsmentioning
confidence: 99%
“…Velocity and pressure are represented as Fourier expansions in the periodic streamwise and spanwise directions and as Chebyshev polynomials in the wall-normal direction. Channelflow uses the influence-matrix method of Kleiser & Schumann (1980) to integrate the Navier-Stokes equations forward in time. This method solves the Navier-Stokes equations at each time step via solutions of a sequence of onedimensional scalar Helmholtz equations forũ,ṽ,w andp for each wavenumber pair, with homogenous Dirichlet boundary conditions at the walls.…”
Section: Dns Resultsmentioning
confidence: 99%