1973
DOI: 10.1017/s0022112073002016
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Numerical study of slightly viscous flow

Abstract: A numerical method for solving the time-dependent Navier–Stokes equations in two space dimensions at high Reynolds number is presented. The crux of the method lies in the numerical simulation of the process of vorticity generation and dispersal, using computer-generated pseudo-random numbers. An application to flow past a circular cylinder is presented.

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Cited by 1,294 publications
(823 citation statements)
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“…Nevertheless, the PVM is quite unstable in general. A vortex blob was introduced by Chorin in 1973 [7] to replace the point vortex, known as vortex blob method, and was successfully used in a computation of the flow past cylinder along with two other seminal ideas: creation of vorticity on the boundary to enforce the no-slip boundary condition and using random walk to approximate the viscosity. Krasny performed careful studies for the vortex sheet problem with the vortex blob methods [15].…”
Section: Introductionmentioning
confidence: 99%
“…Nevertheless, the PVM is quite unstable in general. A vortex blob was introduced by Chorin in 1973 [7] to replace the point vortex, known as vortex blob method, and was successfully used in a computation of the flow past cylinder along with two other seminal ideas: creation of vorticity on the boundary to enforce the no-slip boundary condition and using random walk to approximate the viscosity. Krasny performed careful studies for the vortex sheet problem with the vortex blob methods [15].…”
Section: Introductionmentioning
confidence: 99%
“…The class of vortex methods are used to simulate incompressible and slightly compressible flows [41,65].…”
Section: Spectral Methodsmentioning
confidence: 99%
“…The origin of modern meshless methods could be dated back to the 70's with the pioneering works in generalized finite differences and vortex particle methods [20], [21], [22]. However, the strongest influence upon the present trends is commonly attributed to early Smoothed Particle Hydrodynamics (SPH) formulations [23], [24], [25], where a lagrangian particle tracking is used to describe the motion of a fluid.…”
Section: Meshless Approximantsmentioning
confidence: 99%
“…The overall accuracy of the resulting algorithm is, therefore, second order, and one integration point per cell face (the midpoint) is sufficient to compute the boundary integrals (Figure 2 left). Third order spatial accuracy could be obtained using the cubic basis (21). In this case a higher order quadrature rule is required for the evaluation of boundary integrals.…”
Section: Accuracy and Implementationmentioning
confidence: 99%