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Introduction to Sports Biomechanics: Analysing Human Movement ...

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Figure 5.11 Levers as examples of parallel force systems: (a) first-class lever; (b) third-class lever.<br />

when analysing the various soft tissue forces acting on a body segment. These force<br />

systems will not be covered further in this book.<br />

The vec<strong>to</strong>r equations of statics and the use of inertia forces can aid the analysis of the<br />

complex force systems that are commonplace in sport. However, many sports<br />

biomechanists feel that the use of the equations of static equilibrium obscures the<br />

dynamic nature of force in sport, and that it is more revealing <strong>to</strong> deal with the dynamic<br />

equations of motion, an approach that I prefer. In sport, force systems almost always<br />

change with time, as in Figure 5.2, which shows the vertical component of ground<br />

reaction force recorded from a force platform during a standing vertical jump. The<br />

effect of the force at any instant is reflected in an instantaneous acceleration of the<br />

performer’s centre of mass. The change of the force with time determines how<br />

the velocity and displacement of the centre of mass change, and it is important <strong>to</strong><br />

remember this.<br />

MOMENTUM AND THE LAWS OF LINEAR MOTION<br />

Inertia and mass<br />

CAUSES OF MOVEMENT – FORCES AND TORQUES<br />

The inertia of an object is its reluctance <strong>to</strong> change its state of motion. Inertia is directly<br />

measured or expressed by the mass of the object, which is the quantity of matter of<br />

which the object is composed. It is more difficult <strong>to</strong> accelerate an object of large mass,<br />

such as a shot, than one of small mass, such as a dart. Mass is a scalar, having no<br />

directional quality; the SI unit of mass is the kilogram (kg).<br />

183

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