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1 TÜRKİYE PROFESYONEL LİGLERİNDE GÖREV ... - Spor Bilim

1 TÜRKİYE PROFESYONEL LİGLERİNDE GÖREV ... - Spor Bilim

1 TÜRKİYE PROFESYONEL LİGLERİNDE GÖREV ... - Spor Bilim

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y<br />

b<br />

m m<br />

g<br />

a 1<br />

a 2<br />

z x<br />

shoulder<br />

elbow<br />

wrist<br />

front view left side view<br />

Figure 1. The model<br />

The velocity of an infinitesimal arm segment dr in the direction perpendicular to the axis of<br />

the arm segment, shown in Figure 2, can be written as<br />

Va t b<br />

= V -V<br />

sinq<br />

, (1)<br />

where V t is the tangential component of the velocity of the arm segment relative to the<br />

shoulder joint which is equal to 2p fr'<br />

, b V is the velocity of the body in x direction, q is the<br />

angle between the projection of the arm axis on x-y plane and x direction, f is the stroke rate<br />

and r ' is the projection on x-y plane of the length from the shoulder joint to the infinitesimal<br />

arm segment. We also note that r ' is the perpendicular distance from z-axis to the<br />

infinitesimal arm segment. The propulsive force of the infinitesimal element, dF p , can be<br />

written as<br />

dF<br />

p<br />

2<br />

= k DV dr . (2)<br />

a<br />

a<br />

Here, k a is the drag coefficient and D is the diameter of the arm. These basic relations will<br />

be used in the derivation of the propulsive force expression for each separate part of the arm.<br />

x<br />

90-q<br />

V t<br />

Figure 2. Infinitesimal element on the arm<br />

V b<br />

V a<br />

r'<br />

q<br />

y<br />

q<br />

a 2<br />

a 1<br />

y

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