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    Effects of Free-Stream Turbulence Intensity on a Boundary Layer Recovering From Concave Curvature Effects

    Source: Journal of Turbomachinery:;1995:;volume( 117 ):;issue: 002::page 240
    Author:
    M. D. Kestoras
    ,
    T. W. Simon
    DOI: 10.1115/1.2835652
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Experiments are conducted on a flat recovery wall downstream of sustained concave curvature in the presence of high free-stream turbulence (TI ∼ 8%). This flow simulates some of the features of the flow on the latter parts of the pressure surface of a gas turbine airfoil. The combined effects of concave curvature and TI, both present in the flow over a turbine airfoil, have so far been little studied. Computation of such flows with standard turbulence closure models has not been particularly successful. This experiment attempts to characterize the turbulence characteristics of this flow. In the present study, a turbulent boundary layer grows from the leading edge of a concave wall, then passes onto a downstream flat wall. Results show that turbulence intensities increase profoundly in the outer region of the boundary layer over the recovery wall. Near-wall turbulent eddies appear to lift off the recovery wall and a “stabilized” region forms near the wall. In contrast to a low-free-stream turbulence intensity flow, turbulent eddies penetrate the outer parts of the “stabilized” region where sharp velocity and temperature gradients exist. These eddies can more readily transfer momentum and heat. As a result, skin friction coefficients and Stanton numbers on the recovery wall are 20 and 10 percent, respectively, above their values in the low-free-stream turbulence intensity case. Stanton numbers do not undershoot flat-wall expectations at the same Reδ2 values as seen in the low-TI case. Remarkably, the velocity distribution in the core of the flow over the recovery wall exhibits a negative gradient normal to the wall under high-free-stream turbulence intensity conditions. This velocity distribution appears to be the result of two effects: (1) cross transport of kinetic energy by boundary work in the upstream curved flow and (2) readjustment of static pressure profiles in response to the removal of concave curvature.
    keyword(s): Turbulence , Boundary layers , Flow (Dynamics) , Eddies (Fluid dynamics) , Pressure , Airfoils , Temperature gradients , Gas turbines , Turbines , Boundary layer turbulence , Computation , Gradients , Momentum , Heat , Kinetic energy AND Skin friction (Fluid dynamics) ,
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      Effects of Free-Stream Turbulence Intensity on a Boundary Layer Recovering From Concave Curvature Effects

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    http://yetl.yabesh.ir/yetl1/handle/yetl/116153
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    contributor authorM. D. Kestoras
    contributor authorT. W. Simon
    date accessioned2017-05-08T23:48:37Z
    date available2017-05-08T23:48:37Z
    date copyrightApril, 1995
    date issued1995
    identifier issn0889-504X
    identifier otherJOTUEI-28643#240_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/116153
    description abstractExperiments are conducted on a flat recovery wall downstream of sustained concave curvature in the presence of high free-stream turbulence (TI ∼ 8%). This flow simulates some of the features of the flow on the latter parts of the pressure surface of a gas turbine airfoil. The combined effects of concave curvature and TI, both present in the flow over a turbine airfoil, have so far been little studied. Computation of such flows with standard turbulence closure models has not been particularly successful. This experiment attempts to characterize the turbulence characteristics of this flow. In the present study, a turbulent boundary layer grows from the leading edge of a concave wall, then passes onto a downstream flat wall. Results show that turbulence intensities increase profoundly in the outer region of the boundary layer over the recovery wall. Near-wall turbulent eddies appear to lift off the recovery wall and a “stabilized” region forms near the wall. In contrast to a low-free-stream turbulence intensity flow, turbulent eddies penetrate the outer parts of the “stabilized” region where sharp velocity and temperature gradients exist. These eddies can more readily transfer momentum and heat. As a result, skin friction coefficients and Stanton numbers on the recovery wall are 20 and 10 percent, respectively, above their values in the low-free-stream turbulence intensity case. Stanton numbers do not undershoot flat-wall expectations at the same Reδ2 values as seen in the low-TI case. Remarkably, the velocity distribution in the core of the flow over the recovery wall exhibits a negative gradient normal to the wall under high-free-stream turbulence intensity conditions. This velocity distribution appears to be the result of two effects: (1) cross transport of kinetic energy by boundary work in the upstream curved flow and (2) readjustment of static pressure profiles in response to the removal of concave curvature.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleEffects of Free-Stream Turbulence Intensity on a Boundary Layer Recovering From Concave Curvature Effects
    typeJournal Paper
    journal volume117
    journal issue2
    journal titleJournal of Turbomachinery
    identifier doi10.1115/1.2835652
    journal fristpage240
    journal lastpage247
    identifier eissn1528-8900
    keywordsTurbulence
    keywordsBoundary layers
    keywordsFlow (Dynamics)
    keywordsEddies (Fluid dynamics)
    keywordsPressure
    keywordsAirfoils
    keywordsTemperature gradients
    keywordsGas turbines
    keywordsTurbines
    keywordsBoundary layer turbulence
    keywordsComputation
    keywordsGradients
    keywordsMomentum
    keywordsHeat
    keywordsKinetic energy AND Skin friction (Fluid dynamics)
    treeJournal of Turbomachinery:;1995:;volume( 117 ):;issue: 002
    contenttypeFulltext
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