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Introduction to Sports Biomechanics: Analysing Human Movement ...

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QUANTITATIVE ANALYSIS OF MOVEMENT<br />

Figure 4.14 Tangential velocity and tangential and centripetal acceleration components for a gymnast rotating about a<br />

bar. Her angular velocity vec<strong>to</strong>r lies along the bar as shown by the blue arrow; the position vec<strong>to</strong>r (dashed white arrow)<br />

runs from the bar <strong>to</strong> the gymnast’s centre of mass. The tangential velocity vec<strong>to</strong>r (black arrow) is perpendicular <strong>to</strong> the position<br />

vec<strong>to</strong>r and passes posterior <strong>to</strong> her centre of mass. The tangential acceleration vec<strong>to</strong>r is also represented by the black arrow.<br />

The centripetal acceleration vec<strong>to</strong>r, shown by the continuous white arrow, is in the direction opposite <strong>to</strong> that of the position<br />

vec<strong>to</strong>r.<br />

human performer. Most of these conventions have certain problems, one of which is <strong>to</strong><br />

have an angle convention that is easily unders<strong>to</strong>od. Further discussion of this <strong>to</strong>pic is<br />

beyond the scope of this book (but see Milner, 2007; Further Reading, page 152).<br />

The specification of the angular orientation of the human performer as a whole is<br />

also problematic. The representation of Figure 4.15, for example, has been used <strong>to</strong><br />

analyse airborne movements in gymnastics, diving and trampolining. In this, rotation is<br />

specified by the somersault angle (φ) about a horizontal axis through the centre of mass,<br />

the twist angle (ψ) about the longitudinal axis of the performer, and the tilt angle (θ).<br />

The last named is the angle between the longitudinal axis and the fixed plane normal <strong>to</strong><br />

the somersault angular velocity vec<strong>to</strong>r.<br />

147

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