scholarly journals Discussion: “Turbulent Flow in the Inlet Region of a Smooth Pipe” (Barbin, A. R., and Jones, J. B., 1963, ASME J. Basic Eng., 85, pp. 29–33)

1963 ◽  
Vol 85 (1) ◽  
pp. 33-33
Author(s):  
Karl Brenkert
1980 ◽  
Vol 102 (1) ◽  
pp. 97-103 ◽  
Author(s):  
Mitsukiyo Murakami ◽  
Kouji Kikuyama

Experimental results concerning the flow pattern and hydraulic resistance in a rotating pipe are described. A fully developed turbulent flow was introduced into a long smooth pipe rotating about its axis, and changes of the flow pattern, together with hydraulic loss within the pipe, were examined by measuring the velocity and pressure distributions across sections at various distance from the pipe entrance. Increase of pipe rotation continuously reduces the hydraulic loss and gradually changes the axial velocity profile from a turbulent type to a laminar one. Governing factors for these changes are discussed.


1968 ◽  
Vol 90 (3) ◽  
pp. 431-433 ◽  
Author(s):  
D. A. Bowlus ◽  
J. A. Brighton
Keyword(s):  

1963 ◽  
Vol 85 (1) ◽  
pp. 29-33 ◽  
Author(s):  
A. R. Barbin ◽  
J. B. Jones

This paper reports measurements of mean velocities, turbulence intensities, and turbulence (Reynolds) stresses in the inlet region of a smooth pipe. Data are presented for the first 40 diameters of pipe length. Fully developed flow is not attained in this length for a Reynolds number (based on pipe diameter and mean velocity) of 388,000, but the wall shear stress and the static pressure gradient attain their fully developed values within the first 15 diameters. Velocity profiles at successive sections in the inlet region are not similar as assumed in some published calculation methods. Longitudinal convection of turbulence energy is appreciable; except very near the pipe entrance, radial convection is negligible.


2010 ◽  
Vol 13 (2) ◽  
pp. 48-58
Author(s):  
Duc Van Le

Based on law of shear stress in turbulent flow. Prandd's mixing length theory, and Bakhmeteflfs point of view on "wall velocity", turbulent velocity distribution u on wetted area can be derived for smooth pipe and complete turbulence, rough pipe. Discharge Q and average velocity y are obtained, after the integration, Q= ∫∫wu.dw is done. Relying on the properties of uniform flow, relationship between V, friction factor λ, and shear velocity u is set up. After eliminating u*. velocity V is obtained as a function of Reynolds number Re or relative roughness e/D. Finally, the value of friction factor z can be derived as a function of Re or e/D for the two above-mentioned cases. These formations of z formulas are almost same as the experimental ones introduced by Nikuradse with minor deviations in the factors and their relative errors do not exceed 1% for smooth pipe, and 2% for complete turbulence, rough pipe. Through this research result, the rightness of Prandtl's mixing length theory is almost asserted.


2010 ◽  
Vol 136 (9) ◽  
pp. 626-632 ◽  
Author(s):  
Kaveh Sookhak Lari ◽  
Maarten van Reeuwijk ◽  
Čedo Maksimović

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