1965
DOI: 10.1017/s0022112065001374
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The three-dimensional laminar boundary layer on a rotating helical blade

Abstract: The equations of motion of an incompressible viscous fluid are given in a rotating helical co-ordinate system, which is non-orthogonal. Partial differential equations are derived for the boundary-layer flow on a rotating helical blade. Numerical solutions of these equations show that the radial flow in the boundary layer is strongly dependent upon the stagger and speed of rotation of the blade.

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Cited by 11 publications
(4 citation statements)
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“…A calculation of the laminar velocity profiles was made using the analysis of Horlock & Wordsworth (1965). It is assumed in this analysis that there is no streamwise pressure gradient and this assumption is therefore implied in the calculation, so that for small cross-flows the Blasius solution results for the T FIGURE 7 .…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…A calculation of the laminar velocity profiles was made using the analysis of Horlock & Wordsworth (1965). It is assumed in this analysis that there is no streamwise pressure gradient and this assumption is therefore implied in the calculation, so that for small cross-flows the Blasius solution results for the T FIGURE 7 .…”
Section: Discussionmentioning
confidence: 99%
“…On turbine blades extended areas of laminar flow are possible (see Horlock 1969). A general solution of the equations describing the laminar boundary layer on a blade rotating in a radial pressure gradient has been given (Horlock & Wordsworth 1965) and the initial object of the experiments described here was to provide measurements for comparison with this solution. Figure 1 shows the helical co-ordinate system that was used for the original t Present address : TJniversity of Salford, Salford M5 4WT, England.…”
Section: Introductionmentioning
confidence: 99%
“…Fogarty (1951) and Mager & Hansen (1952) were amongst the first to report that integral boundary methods demonstrated that the magnitude of the radial and streamwise components of flow in the boundary layer were comparable. Horlock & Wordsworth (1965) showed that this radial migration of flow within the boundary layer was dependent 3.…”
Section: Mid-height Boundary Layermentioning
confidence: 99%
“…This causes the bulk passage flow in the rotor to move radially outward and in the stator to move radially inward. Second, a differential boundary layer effect where the differential effect of centrifugal and Coriolis forces cause the boundary layers in the rotor to be accelerated towards the casing, Horlock & Wordsworth (1965). This effect is critical to this paper as it acts as a natural asymmetry between the way in which the rotor and stator boundary layers develop.…”
Section: Effect Of Rotationmentioning
confidence: 99%