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Introduction to Sports Biomechanics: Analysing Human Movement ...

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Buoyancy<br />

dry and wet surface friction coefficients of around 1.0 and 0.4, respectively. The treads<br />

allow water <strong>to</strong> be removed from the contact area between the tyre and road surface.<br />

Likewise, most sports shoes have treaded or cleated soles, and club and racket grips are<br />

rarely perfectly smooth. In some cases, the cleats on the sole of a sports shoe will also<br />

provide some form locking with certain surfaces.<br />

Pulley friction<br />

Passing a rope around the surface of a pulley makes it easier <strong>to</strong> resist a force of large<br />

magnitude at one end by a much smaller force at the other end because of the friction<br />

between the rope and the pulley. This principle is used, for example, in abseiling<br />

techniques in rock climbing and mountaineering. It also explains the need for synovial<br />

membranes <strong>to</strong> prevent large friction forces when tendons pass over bony prominences.<br />

Buoyancy is the force experienced by an object immersed, or partly immersed, in a<br />

fluid. It always acts vertically upwards at the centre of buoyancy (CB in Figure 5.6).<br />

The magnitude of the buoyancy force (B) is expressed by Archimedes’ principle, ‘the<br />

upthrust is equal <strong>to</strong> the weight of fluid displaced’, and is given by B = V ρ g, where<br />

V is the volume of fluid displaced, ρ is the density of the fluid and g is gravitational<br />

acceleration. The buoyancy force is large in water – pure fresh water has a density of<br />

1000 kg/m 3 – and much smaller, but not entirely negligible, in air, which has a density<br />

of around 1.23 kg/m 3 . For a person or an object <strong>to</strong> float and not sink, the magnitudes of<br />

the buoyancy force and the weight of the object must be equal, so that B = G.<br />

The swimmer in Figure 5.6 will only float if her average body density is less than or<br />

equal <strong>to</strong> the density of water. How much of her body is submerged will depend on the<br />

ratio of the two densities. If the density of the swimmer is greater than that of the water,<br />

Figure 5.6 Buoyancy force: (a) forces acting; (b) forces in equilibrium.<br />

CAUSES OF MOVEMENT – FORCES AND TORQUES<br />

171

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