1977
DOI: 10.1299/kikai1938.43.2957
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Studies on a Two-Dimensional Impinging Jet Considering Initial Turbulence : 2nd Report, Static Behaviour of Boundary Layer in the Stagnation Region

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Cited by 4 publications
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“…7, we assume here that the average velocity distribution near the stagnation area can be approximated by theoretical relations for the impinging jet flow treated in past studies. Referring to the method proposed by Kamoi and Tanaka (1977), the flow field was analyzed from the integrated momentum equation, in which the velocity profile in the boundary layer was approximated by a polynomial satisfying the boundary conditions (Schlichting, 1979b). The static pressure at the stagnation point was calculated from the dynamic pressure at the maximum jet velocity shown in Fig.…”
Section: Experimental Results Of Adhesive Forcementioning
confidence: 99%
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“…7, we assume here that the average velocity distribution near the stagnation area can be approximated by theoretical relations for the impinging jet flow treated in past studies. Referring to the method proposed by Kamoi and Tanaka (1977), the flow field was analyzed from the integrated momentum equation, in which the velocity profile in the boundary layer was approximated by a polynomial satisfying the boundary conditions (Schlichting, 1979b). The static pressure at the stagnation point was calculated from the dynamic pressure at the maximum jet velocity shown in Fig.…”
Section: Experimental Results Of Adhesive Forcementioning
confidence: 99%
“…7. If the pressure distribution in the x-direction is approximated by a Gaussian profile, the free stream velocity can be obtained from Bernoulli's theorem (Kamoi and Tanaka, 1977). The integrated boundary layer equation can be solved numerically by the simple Runge-Kutta method.…”
Section: Experimental Results Of Adhesive Forcementioning
confidence: 99%