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    Turbulent Flow in Smooth and Rough Pipes

    Source: Journal of Fluids Engineering:;1972:;volume( 094 ):;issue: 002::page 353
    Author:
    H. W. Townes
    ,
    J. L. Gow
    ,
    R. E. Powe
    ,
    N. Weber
    DOI: 10.1115/1.3425420
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Fully developed turbulent flow in both smooth and rough-walled pipes is investigated for Reynolds numbers from 30,000 to 480,000. The values of mean velocity, root-mean-square values of the fluctuating velocity components, and cross-correlation values of the fluctuating velocities are presented for flow in a smooth pipe and two sand-roughened pipes, R/ε = 208 and R/ε = 26.4. The quantity R/ε is the ratio of the actual pipe radius to the average sand particle size. The experimental measurements for flow in smooth pipes are in good agreement with those of previous investigations throughout the Reynolds number range considered. Several of the rough pipe turbulence quantities show substantial deviations from the corresponding smooth pipe quantities. For rough pipes, the measured uv cross-correlation values approach those predicted empirically from the Reynolds equations for fully developed, axisymmetric flow as the flow approaches the hydraulically smooth case. However, as the Reynolds number is increased and the flow proceeds through the transition region from smooth to fully rough flow and to the fully rough flow region, the values of the uv cross correlation in rough pipes are significantly lower than the predicted values. This difference between predicted and measured data becomes more pronounced as the Reynolds number is further increased and the flow becomes fully rough. The difference between measured and predicted uv values, and other differences between smooth and rough pipe results, suggests that the accepted reduction of the Reynolds equations for flow in smooth pipes is not valid for flow in rough pipes. Thus, the Reynolds equations are re-examined for flow in rough pipes, and it is shown that these equations can be satisfied by the experimental data if secondary flows and angular variations in the mean velocity are postulated.
    keyword(s): Turbulence , Surface roughness , Pipes , Flow (Dynamics) , Reynolds number , Equations , Sands , Measurement , Particle size AND Fully developed turbulent flow ,
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      Turbulent Flow in Smooth and Rough Pipes

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    https://yetl.yabesh.ir/yetl1/handle/yetl/162366
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    • Journal of Fluids Engineering

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    contributor authorH. W. Townes
    contributor authorJ. L. Gow
    contributor authorR. E. Powe
    contributor authorN. Weber
    date accessioned2017-05-09T01:32:46Z
    date available2017-05-09T01:32:46Z
    date copyrightJune, 1972
    date issued1972
    identifier issn0098-2202
    identifier otherJFEGA4-27393#353_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/162366
    description abstractFully developed turbulent flow in both smooth and rough-walled pipes is investigated for Reynolds numbers from 30,000 to 480,000. The values of mean velocity, root-mean-square values of the fluctuating velocity components, and cross-correlation values of the fluctuating velocities are presented for flow in a smooth pipe and two sand-roughened pipes, R/ε = 208 and R/ε = 26.4. The quantity R/ε is the ratio of the actual pipe radius to the average sand particle size. The experimental measurements for flow in smooth pipes are in good agreement with those of previous investigations throughout the Reynolds number range considered. Several of the rough pipe turbulence quantities show substantial deviations from the corresponding smooth pipe quantities. For rough pipes, the measured uv cross-correlation values approach those predicted empirically from the Reynolds equations for fully developed, axisymmetric flow as the flow approaches the hydraulically smooth case. However, as the Reynolds number is increased and the flow proceeds through the transition region from smooth to fully rough flow and to the fully rough flow region, the values of the uv cross correlation in rough pipes are significantly lower than the predicted values. This difference between predicted and measured data becomes more pronounced as the Reynolds number is further increased and the flow becomes fully rough. The difference between measured and predicted uv values, and other differences between smooth and rough pipe results, suggests that the accepted reduction of the Reynolds equations for flow in smooth pipes is not valid for flow in rough pipes. Thus, the Reynolds equations are re-examined for flow in rough pipes, and it is shown that these equations can be satisfied by the experimental data if secondary flows and angular variations in the mean velocity are postulated.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleTurbulent Flow in Smooth and Rough Pipes
    typeJournal Paper
    journal volume94
    journal issue2
    journal titleJournal of Fluids Engineering
    identifier doi10.1115/1.3425420
    journal fristpage353
    journal lastpage361
    identifier eissn1528-901X
    keywordsTurbulence
    keywordsSurface roughness
    keywordsPipes
    keywordsFlow (Dynamics)
    keywordsReynolds number
    keywordsEquations
    keywordsSands
    keywordsMeasurement
    keywordsParticle size AND Fully developed turbulent flow
    treeJournal of Fluids Engineering:;1972:;volume( 094 ):;issue: 002
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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