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Introduction to Sports Biomechanics: Analysing Human Movement ...

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INTRODUCTION TO SPORTS BIOMECHANICS<br />

Figure 5.7 Separation points (S) on a smooth ball for boundary layer flow that is: (a) laminar; (b) turbulent. T indicates<br />

transition from laminar <strong>to</strong> turbulent boundary flow.<br />

174<br />

An object moving from a region of low pressure <strong>to</strong> one of high pressure, experiences<br />

a drag force, which will be discussed below. The boundary layer separation, which<br />

leads <strong>to</strong> the formation of the wake, occurs far more readily if the fluid flow in the<br />

boundary layer is laminar (Figure 5.7(a)) than if the flow is turbulent (Figure 5.7(b)).<br />

This is because kinetic energy is more evenly distributed across a turbulent boundary<br />

layer, enabling the fluid particles near the boundary <strong>to</strong> better resist the increasing<br />

pressure. Figure 5.7 shows the difference in the separation point (S) positions and the<br />

size of the wake between laminar and turbulent boundary layers on a ball. The<br />

change from laminar <strong>to</strong> turbulent boundary layer flow will occur, for a given object<br />

and conditions, at a speed related <strong>to</strong> the critical Reynolds number. The change<br />

occurs at the transition point (T, Figure 5.7(b)), and the relationship between the<br />

transition and separation points is very important. If separation occurs before its<br />

transition <strong>to</strong> turbulent flow, a large wake is formed (Figure 5.7(a)), whereas transition<br />

<strong>to</strong> turbulent flow upstream of the separation point results in a smaller wake (Figure<br />

5.7(b)).

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