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    Torsional Instability of Fully Stalled Airfoil (or Supercavitating Hydrofoil)

    Source: Journal of Manufacturing Science and Engineering:;1967:;volume( 089 ):;issue: 004::page 671
    Author:
    M. S. Natesh
    DOI: 10.1115/1.3610131
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: A theoretical study is carried out to determine the conditions under which steady-state pitching oscillations of an airfoil in one degree of freedom are possible in two-dimensional subsonic incompressible stalled flow using Parkin’s [1] coefficients. The results show that such oscillations can occur if the axis of rotation is located at a point that is approximately rearward of airfoil midchord but not too far rearward of the airfoil trailing edge. The practical significance of these results with respect to flutter is briefly examined. Torsional flutter [2] in the case of potential flow can occur only at very low reduced frequencies and under special circumstances, namely, when the rotation point is ahead of quarter chord, K′ > 550 and k < 0.0435. The significant difference between classical and stall flutter (torsional) is that the real part of the pitching moment coefficient [2] is negative in the former case and is positive in the latter case in the region of instability. Therefore, stall flutter can occur at very low values of K′ , unlike classical flutter where K′ has to be greater than 550. The ratio of torsional natural frequency to flutter frequency is greater than 1 in the case of stall flutter, whereas in classical flutter the ratio is less than 1 because of the sign of the real part of the moment coefficient. A single-degree-of-freedom torsional flutter equation was derived, and by equating the real and the imaginary parts of the equation, relationships between the various flutter parameters were obtained. Stability boundaries were obtained for the structural damping coefficient gα = 0, 0.001, 0.005, 0.01, 0.02, 0.04, and 0.1 for various values of K′ , namely, 5, 20, 40, 60, 80, 100, and 1000. The above values practically cover all airplane wings and compressor blades. The significant results are tabulated and some of the important parameters are plotted in the attached figures. By utilizing these figures, a typical airfoil in question could be checked, whether it is flutter-free or not, and if it is in flutter, all the flutter parameters could be determined. The analysis was conducted using Parkin’s coefficients [1], which require that the airfoil be completely stalled during the cycle.
    keyword(s): Hydrofoil , Airfoils , Flutter (Aerodynamics) , Oscillations , Rotation , Flow (Dynamics) , Equations , Frequency , Steady state , Wings , Compressors , Chords (Trusses) , Stability , Degrees of freedom , Damping , Aircraft , Blades AND Cycles ,
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      Torsional Instability of Fully Stalled Airfoil (or Supercavitating Hydrofoil)

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    https://yetl.yabesh.ir/yetl1/handle/yetl/121045
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    • Journal of Manufacturing Science and Engineering

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    contributor authorM. S. Natesh
    date accessioned2017-05-08T23:57:41Z
    date available2017-05-08T23:57:41Z
    date copyrightNovember, 1967
    date issued1967
    identifier issn1087-1357
    identifier otherJMSEFK-27516#671_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/121045
    description abstractA theoretical study is carried out to determine the conditions under which steady-state pitching oscillations of an airfoil in one degree of freedom are possible in two-dimensional subsonic incompressible stalled flow using Parkin’s [1] coefficients. The results show that such oscillations can occur if the axis of rotation is located at a point that is approximately rearward of airfoil midchord but not too far rearward of the airfoil trailing edge. The practical significance of these results with respect to flutter is briefly examined. Torsional flutter [2] in the case of potential flow can occur only at very low reduced frequencies and under special circumstances, namely, when the rotation point is ahead of quarter chord, K′ > 550 and k < 0.0435. The significant difference between classical and stall flutter (torsional) is that the real part of the pitching moment coefficient [2] is negative in the former case and is positive in the latter case in the region of instability. Therefore, stall flutter can occur at very low values of K′ , unlike classical flutter where K′ has to be greater than 550. The ratio of torsional natural frequency to flutter frequency is greater than 1 in the case of stall flutter, whereas in classical flutter the ratio is less than 1 because of the sign of the real part of the moment coefficient. A single-degree-of-freedom torsional flutter equation was derived, and by equating the real and the imaginary parts of the equation, relationships between the various flutter parameters were obtained. Stability boundaries were obtained for the structural damping coefficient gα = 0, 0.001, 0.005, 0.01, 0.02, 0.04, and 0.1 for various values of K′ , namely, 5, 20, 40, 60, 80, 100, and 1000. The above values practically cover all airplane wings and compressor blades. The significant results are tabulated and some of the important parameters are plotted in the attached figures. By utilizing these figures, a typical airfoil in question could be checked, whether it is flutter-free or not, and if it is in flutter, all the flutter parameters could be determined. The analysis was conducted using Parkin’s coefficients [1], which require that the airfoil be completely stalled during the cycle.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleTorsional Instability of Fully Stalled Airfoil (or Supercavitating Hydrofoil)
    typeJournal Paper
    journal volume89
    journal issue4
    journal titleJournal of Manufacturing Science and Engineering
    identifier doi10.1115/1.3610131
    journal fristpage671
    journal lastpage680
    identifier eissn1528-8935
    keywordsHydrofoil
    keywordsAirfoils
    keywordsFlutter (Aerodynamics)
    keywordsOscillations
    keywordsRotation
    keywordsFlow (Dynamics)
    keywordsEquations
    keywordsFrequency
    keywordsSteady state
    keywordsWings
    keywordsCompressors
    keywordsChords (Trusses)
    keywordsStability
    keywordsDegrees of freedom
    keywordsDamping
    keywordsAircraft
    keywordsBlades AND Cycles
    treeJournal of Manufacturing Science and Engineering:;1967:;volume( 089 ):;issue: 004
    contenttypeFulltext
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