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Introduction to Sports Biomechanics: Analysing Human Movement ...

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CAUSES OF MOVEMENT – FORCES AND TORQUES<br />

Figure 5.9 Typical path of a swimmer’s hand relative <strong>to</strong> the water: (a) side view; (b) view from in front of the swimmer; (c)<br />

view from below the swimmer.<br />

as tennis and table tennis both <strong>to</strong> vary the flight of the ball and <strong>to</strong> alter its bounce. In<br />

cricket, a spin bowler usually spins the ball so that it is rotating about the axis along<br />

which it is moving (its velocity vec<strong>to</strong>r), and the ball only deviates when it contacts<br />

the ground. However, if the ball’s spin axis does not coincide with its velocity vec<strong>to</strong>r, the<br />

ball will also move laterally through the air. A baseball pitcher also uses the Magnus<br />

effect <strong>to</strong> ‘curve’ the ball; at a pitching speed of 30 m/s the spin imparted can be as high<br />

as 30 Hz, which gives a lateral deflection of 0.45 m in 18 m. A soccer ball can be made<br />

<strong>to</strong> swerve, or ‘bend’, in flight by moving the foot across the ball as it is kicked. This<br />

causes rotation of the ball about the vertical axis. If the foot is moved from right <strong>to</strong> left<br />

as the ball is kicked, the ball will swerve <strong>to</strong> the right. Slicing and hooking of a golf ball<br />

are caused, inadvertently, by sidespin imparted at impact. In crosswinds, the relative<br />

direction of motion between the air and the ball is changed; a small amount of sidespin,<br />

imparted by ‘drawing’ the ball with a slightly open club face, or ‘fading’ the ball with a<br />

slightly closed club face depending on the wind direction, can then increase the length<br />

of the drive.<br />

A negative Magnus effect can also occur for a ball travelling below the critical<br />

Reynolds number. This happens when the boundary layer flow remains laminar on the<br />

side of the ball moving in the direction of the relative air flow, as the Reynolds number<br />

here remains below the critical value. On the other side of the ball, the rotation<br />

increases the relative speed between the air and the ball so that the boundary layer<br />

becomes turbulent. If this happens on a back-spinning ball, laminar boundary layer<br />

179

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