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- W3100553111 abstract "Taylor (1915) drew attention to an identity which connects the gradient in Reynolds stress with the transport of components of vorticity. Numerical results for this transport of vorticity for pipe flow are presented. The difference between the two terms in this vorticity transport, scaled by outer variables at high Reynolds number, must be 0 for Couette flow, -1 for channel flow and -2 for pipe flow. Each vorticity flux and the difference between them are examined from a consideration of the corresponding probability density function (pdf) and the associated symmetric “cumulative integral (CI) for the mean value”. The CI results show that the last 10% of the final mean value is contributed by local values that are approximately 300 times larger in magnitude than the mean value! Thus local, very large, but infrequent, events contribute greatly to the mean value. Even the familiar 2D transport term is far from Taylor's approximation. For the other transport term there is a change in sign near the wall." @default.
- W3100553111 created "2020-11-23" @default.
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- W3100553111 date "2020-12-11" @default.
- W3100553111 modified "2023-09-27" @default.
- W3100553111 title "Vorticity Transport in Turbulent Pipe Flow" @default.
- W3100553111 doi "https://doi.org/10.14264/b2d6025" @default.
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