Reynolds stress and joint probability density distributions in the u‐v plane of a turbulent channel flow
The joint probability density distributions, p (u,v), of the u and v turbulence components are presented for nine positions across a fully developed turbulent channel flow. These distributions were determined by using 512 000 pairs of u and v values at each position and thus enable comparison of the...
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Veröffentlicht in: | The Physics of fluids (1958) 1977-03, Vol.20 (3), p.351-355 |
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container_issue | 3 |
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container_title | The Physics of fluids (1958) |
container_volume | 20 |
creator | Wallace, James M. Brodkey, Robert S. |
description | The joint probability density distributions, p (u,v), of the u and v turbulence components are presented for nine positions across a fully developed turbulent channel flow. These distributions were determined by using 512 000 pairs of u and v values at each position and thus enable comparison of the relative character between the distributions. To show the contribution to the Reynolds stress, −ρ
uv
̄
at each point in the u‐v plane, the distributions of u
v
p (u,v) were determined. These distributions show the relative contributions to
uv
̄
as a function of position across the channel. Finally, the distributions of p (u,v) are compared with those of u
v
p (u,v). The most probable pairs of velocities do not produce the largest contribution to
uv
̄
. |
doi_str_mv | 10.1063/1.861897 |
format | Article |
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uv
̄
at each point in the u‐v plane, the distributions of u
v
p (u,v) were determined. These distributions show the relative contributions to
uv
̄
as a function of position across the channel. Finally, the distributions of p (u,v) are compared with those of u
v
p (u,v). The most probable pairs of velocities do not produce the largest contribution to
uv
̄
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uv
̄
at each point in the u‐v plane, the distributions of u
v
p (u,v) were determined. These distributions show the relative contributions to
uv
̄
as a function of position across the channel. Finally, the distributions of p (u,v) are compared with those of u
v
p (u,v). The most probable pairs of velocities do not produce the largest contribution to
uv
̄
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uv
̄
at each point in the u‐v plane, the distributions of u
v
p (u,v) were determined. These distributions show the relative contributions to
uv
̄
as a function of position across the channel. Finally, the distributions of p (u,v) are compared with those of u
v
p (u,v). The most probable pairs of velocities do not produce the largest contribution to
uv
̄
.</abstract><doi>10.1063/1.861897</doi><tpages>5</tpages></addata></record> |
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language | eng |
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title | Reynolds stress and joint probability density distributions in the u‐v plane of a turbulent channel flow |
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