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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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obtained as 2.5007(m/sec)sec. This result can be obtained from the mathematical model when<br />

k is taken as 10.45 kg/m. This modification of the drag coefficient is in agreement with<br />

b<br />

Martin et al. [4] who also needed to reduce k b from 30 to 13 kg/m to obtain reasonble results.<br />

The necessity of using a much smaller k b than that measured in passive thowing can be<br />

explained by the fact that the arms contribute to passive drag but are propulsive elements in<br />

active swimming which could greatly reduce the swimmer's effective drag coeeficient [4].<br />

Conclusion<br />

Tether Force (N)<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

0.0 1.0 2.0 3.0 4.0 5.0 6.0<br />

Time (s)<br />

Mathematical<br />

model<br />

Experiment<br />

Figure 5. Tether force versus time obtained from the experiments<br />

and the mathematical model for f = 0.33 sec -1<br />

In this study, a three dimensional mathematical model is developed for crawl stroke<br />

swimming. Using the basic dynamic relations, the equation of motion is derived and solved<br />

numerically. In order to check the performance of the mathematical model, the numerical<br />

results are compared with the results of the two experiments. The average values of the tether<br />

force of the model for two selected stroke rates are close to those of the tether force<br />

experiments. The results of the free swimming experiments for normal style were found to be<br />

close to the predictions of the model. The proposed model does not consider the leg action,<br />

skin friction and uplift force. The first two of these three forces does not have much effect on<br />

the stroke as compared with drag forces. The effect of uplift force on the strike is more<br />

pronounced while the arm is entering the water. In a real stroke, the arm angles and<br />

frequencies change during the arm pull. This more complex action having different arm<br />

angles at different periods of arm pull together with variable frequencies can be modelled by<br />

the proposed modelling technique easily. For further studies on modelling the crawl stroke,<br />

mathematical models considering the propulsive effect of lift, overlapping strokes and action<br />

of legs are suggested. The patterns of the motions of the body segments should be defined in

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