Preliminary Surveys Of The Three Dimensional Boundary Layer On A Yawed Spinning Body Of Revolution PDF Download

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Preliminary Surveys of the Three Dimensional Boundary Layer on a Yawed, Spinning Body of Revolution

Preliminary Surveys of the Three Dimensional Boundary Layer on a Yawed, Spinning Body of Revolution
Author: Walter B. Sturek
Publisher:
Total Pages: 38
Release: 1975
Genre: Body of revolution
ISBN:

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Experimental measurements of the three dimensional boundary layer on a yawed, spinning tangent-ogive-cylinder model in supersonic flow are reported. The measurements were made using a flattened total head probe at one axial station near the base of the model for 10 azimuthal stations about the circumference. The test conditions were: M = 3, angle of attack = 4 deg, omega = 0 and 10,000 RPM. The trends observed in comparing measurements with and without the model spinning were: (1) the boundary layer is more thick and less full where surface spin opposes the crossflow velocity; and (2) the boundary layer is less thick and more full where surface spin is in the same direction as the crossflow velocity. (Author).


Applied Mechanics Reviews

Applied Mechanics Reviews
Author:
Publisher:
Total Pages: 968
Release: 1976
Genre: Mechanics, Applied
ISBN:

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Studies of Three-Dimensional Boundary Layers on Bodies of Revolution. III. Cones at Incidence in Supersonic Flow

Studies of Three-Dimensional Boundary Layers on Bodies of Revolution. III. Cones at Incidence in Supersonic Flow
Author: Tuncer Cebeci
Publisher:
Total Pages: 45
Release: 1982
Genre:
ISBN:

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An investigation is carried out into the properties of a nonsimiliar boundary layer on a cone at incidence with special reference to the flow near the leeside line of symmetry. The nonsimilarity is induced by allowing suction near the vertex of the cone and the external velocity is given by supersonic inviscid theory. The principal new results of the theory may be expressed in terms of a parameter -k, which is approximately equivalent to the angle of attack of the cone. Three ranges of k have been identified. For small negative values of k, the three-dimensional boundary layer on the cone is smooth everywhere and, once the suction is removed, rapidly approaches a semi-similarity form as the distance from the vertex increases. For more negative values of k the boundary layer is not smooth near the leeside of the cone but can be computed everywhere. The nature of this singularity is partially explained in terms of a collision phenomenon. If k decreases further, separation occurs in computations from the windward side of the cone. The solution develops a singularity along this line provided sufficient care is taken in the calculations. An apparent nonuniqueness in the solution prevents integration from the leeside over the remainder of the region of accessibility.


Studies on Three-Dimensional Boundary Layers on Bodies of Revolution. II. Three-Dimensional Laminar Boundary Layers and the OK of Accessibility

Studies on Three-Dimensional Boundary Layers on Bodies of Revolution. II. Three-Dimensional Laminar Boundary Layers and the OK of Accessibility
Author: Tuncer Cebeci
Publisher:
Total Pages: 66
Release: 1980
Genre:
ISBN:

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An investigation is carried out into the structure of the laminar boundary layer originating from the forward stagnation point of a prolate spheroid at incidence in a uniform stream, assuming that the external velocity distribution is given by attached potential theory. The principal new results of the study are: (1) A new transformation of the body coordinates is devised which facilitates the computation of the solution near the nose, (2) Two variations of the standard box method of solving the equations are devised to enable solutions to be computed in regions of cross-flow reversal, (3) Whereas in two dimensional flows the effect of the boundary layer approaching separation on the external flow may be represented by a blowing velocity, in the present study we find that this is only true near the windward line of symmetry, (4) The boundary layer over the whole of the spheroid cannot be computed in an integration from the forward stagnation point. (5) For alpha> or = 15 deg the accessible region on the leeward side of the ok is largely determined by the external streamline through the ok.


Three-Dimensional Boundary Layers on Bodies of Revolution at Incidence

Three-Dimensional Boundary Layers on Bodies of Revolution at Incidence
Author: V. C. Patel
Publisher:
Total Pages: 13
Release: 1978
Genre:
ISBN:

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This report summarizes the objectives and accomplishments of an experimental and theoretical investigation of the boundary layer development on bodies of revolution at incidence. The results of the flow visualization studies in laminar flow, detailed measurements in a turbulent boundary layer, and calculations of laminar as well as turbulent boundary layers using two different numerical schemes and turbulence models are reviewed to emphasize the important characteristics of separation in three dimensions.


Studies on Three-Dimensional Boundary Layers on Bodies of Revolution. I. Nose Separation

Studies on Three-Dimensional Boundary Layers on Bodies of Revolution. I. Nose Separation
Author: Tuncer Cebeci
Publisher:
Total Pages: 46
Release: 1978
Genre:
ISBN:

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The laminar boundary-layer development near the nose of a body of revolution and a two-dimensional airfoil is investigated until the onset of leading-edge separation. This is accomplished through the use of a coordinate transformation which eliminates any geometrical singularity at the nose in the governing boundary-layer equations. The resulting equations are examined by both asymptotic and numerical means. Comparable cases for the three-dimensional body of revolution and the two-dimensional airfoil are given and similarities as well as differences are discussed. (Author).


Three Dimensional Boundary Layer on a Rotating Cylinder

Three Dimensional Boundary Layer on a Rotating Cylinder
Author: William H Hayes J G Bowling
Publisher: Hassell Street Press
Total Pages: 100
Release: 2021-09-09
Genre:
ISBN: 9781014226563

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