1977
DOI: 10.1016/0017-9310(77)90064-3
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Etude experimentale de la turbulence au voisinage de la paroi d'un tube legerement chauffe

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Cited by 17 publications
(6 citation statements)
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“…The skewness of the IWT temperature ÿeld agrees with the MT results for y + ¡10; beyond this distance, the quantitative agreement is lost and the IWT proÿle attains smaller 595 positive values. The experimental data by Elena [25] are in excellent quantitative agreement with the present IWT results. The large negative values of S # for the MT and IWT temperature ÿelds, for y + ¡20, are consistent with the large positive values of S ux and S ur , which denote the presence of intense sweep events.…”
Section: Turbulent Heat Uxessupporting
confidence: 90%
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“…The skewness of the IWT temperature ÿeld agrees with the MT results for y + ¡10; beyond this distance, the quantitative agreement is lost and the IWT proÿle attains smaller 595 positive values. The experimental data by Elena [25] are in excellent quantitative agreement with the present IWT results. The large negative values of S # for the MT and IWT temperature ÿelds, for y + ¡20, are consistent with the large positive values of S ux and S ur , which denote the presence of intense sweep events.…”
Section: Turbulent Heat Uxessupporting
confidence: 90%
“…Figure 7(b) shows the kurtosis of the velocity components and of the three temperature ÿelds. The experimental data by Elena [25] for F # are in relatively good agreement with the IWT result in the near-wall region. The kurtosis of all velocity components and of the MT and IWT temperature ÿelds increases sharply approaching the wall, due to the wall-blocking e ect; due to the low correlation between the radial velocity and the IWHF temperature uctuations, the IWHF atness does not present relevant variations approaching the wall and attains an approximately constant value of 3 in the viscous wall region, corresponding to the normal distribution.…”
Section: Turbulent Heat Uxessupporting
confidence: 81%
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