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Biomechanics and Medicine in Swimming XI

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<strong>Biomechanics</strong><strong>and</strong>medic<strong>in</strong>e<strong>in</strong>swimm<strong>in</strong>gXi<br />

The variable for the active drag equation could then be computed<br />

through substitution know<strong>in</strong>g the one value for active drag at the swimmer’s<br />

maximum swim velocity.<br />

126<br />

where 210 N = active drag at 1.81 m·s -1<br />

Drag (N)<br />

Velocity (m·s -1 ) Passive (N) Active (N)<br />

250<br />

200<br />

150<br />

100<br />

50<br />

0<br />

2.2 127.31 380.49<br />

2.1 109.31 326.71<br />

2 93.86 280.53<br />

1.9 80.59 240.87<br />

1.8 69.20 206.82<br />

1.7 59.42 177.59<br />

1.6 51.02 152.49<br />

1.5 43.81 130.93<br />

1.4 37.61 112.42<br />

1.2 27.73 82.89<br />

1.1 23.81 71.17<br />

0.8 15.07 45.05<br />

Drag vs Velocity<br />

Passive Active Difference<br />

0.6 0.8 1 1.2 1.4 1.6 1.8 2<br />

Velocity (m.s -1 )<br />

where b used for active <strong>and</strong> passive drag<br />

F = a ⋅e<br />

bv<br />

a = F / e<br />

bv<br />

b = 1.<br />

524<br />

= 210/<br />

e<br />

( 1.<br />

524×<br />

1.<br />

81 )<br />

= 13<br />

. 31204<br />

Table 1: Characteristics of each swimmer, together with the constants<br />

used to derive the active <strong>and</strong> passive drag equations. a a is the constant<br />

for active drag, p a is the constant for passive drag <strong>and</strong> aa− p is the<br />

constant for the difference between active <strong>and</strong> passive drag. b is a constant<br />

represent<strong>in</strong>g a swimmer’s overall drag.<br />

Subject Gender Event (m) R2 Trend<br />

p aa aa− p<br />

1 M 200 0.9921 8.01 1.21 19.97 11.96<br />

2 F 200 0.9702 3.91 1.59 18.68 14.78<br />

3 F 200 0.9944 3.81 1.48 18.92 15.11<br />

4 F 100 0.9831 5.21 1.29 22.97 17.77<br />

5 F 100 0.9779 5.60 1.28 22.12 16.52<br />

6 F 400 0.9718 5.99 1.29 14.63 8.64<br />

7 M 200 0.9957 4.45 1.52 13.31 8.86<br />

8 F 200 0.9859 4.84 1.45 11.42 6.59<br />

9 F 100 0.9768 6.43 1.21 19.85 13.41<br />

10 F 200 0.9819 4.91 1.36 24.57 19.67<br />

11 F 200 0.9879 6.07 1.31 15.83 9.76<br />

a b<br />

dIscussIon<br />

In both active <strong>and</strong> passive drag equations, the value of the drag force is<br />

represented as an exponential function of swimm<strong>in</strong>g velocity. The active<br />

drag values will however rise or <strong>in</strong>crease more rapidly than that of passive<br />

drag. There will still be a similar exponential relationship between the two<br />

curves <strong>and</strong> only the <strong>in</strong>creased rate of rise will differentiate between the<br />

active <strong>and</strong> passive drag equations. Given that the rate of rise between the<br />

active <strong>and</strong> passive drag equations is represented by a s<strong>in</strong>gle constant, these<br />

two constants may be used as an <strong>in</strong>dex to describe the <strong>in</strong>dividual swimmer’s<br />

capabilities. The constant <strong>in</strong> the equation for passive drag would<br />

represent an <strong>in</strong>dex of the swimmer’s <strong>in</strong>nate physical characteristics such<br />

as size, shape <strong>and</strong> cross sectional frontal surface area. A lower <strong>in</strong>dex <strong>in</strong>dicates<br />

a more efficient body shape for aquatics movement. The difference<br />

between the constant used <strong>in</strong> the active drag equation <strong>and</strong> the constant<br />

<strong>in</strong> the passive drag equation could be used as an <strong>in</strong>dex to represent the<br />

efficiency of the swimmer technique. This <strong>in</strong>dex may provide <strong>in</strong>sight as to<br />

the capability of the swimmer to compete <strong>in</strong> particular events.<br />

Exponential functions for both active <strong>and</strong> passive drag were ex-<br />

( b⋅V<br />

)<br />

pressed by the equation F = a ⋅ e , where b was constant for a<br />

particular swimmer <strong>and</strong> a def<strong>in</strong>ed the active or passive drag constant.<br />

The a a represented the constant used <strong>in</strong> the active drag equation, p a<br />

represented the constant used <strong>in</strong> the passive drag equation <strong>and</strong> aa− p<br />

represented the constant used for the difference between active <strong>and</strong> passive<br />

drag. The constant a was useful, <strong>in</strong> that a p def<strong>in</strong>ed the unique<br />

aquatic characteristics of the <strong>in</strong>dividual. This research suggested that the<br />

lower the number, the more effective the <strong>in</strong>dividual characteristic was<br />

with respect to movement through water. The constant aa− p provided<br />

valuable <strong>in</strong>sight <strong>in</strong>to the efficiency of the swimmer’s technique. Once<br />

aga<strong>in</strong>, the lower the value of a the more efficient was the technique.<br />

a−<br />

p<br />

For example, subject six was the Australian 400 m freestyle champion<br />

over a number of consecutive years. The data identified that subject six<br />

had a lower a value than all but one other subject. This highlighted<br />

a−<br />

p<br />

that subject six had an efficient technique. Similarly, subject eight presented<br />

the lowest aa− p value <strong>and</strong> she demonstrated excellent technical<br />

skills. Subject one had the highest a p value <strong>and</strong> this <strong>in</strong>dicated his anthropometric<br />

characteristics were not ideal for swimm<strong>in</strong>g. However, the<br />

a value demonstrated good technical efficiency <strong>in</strong> the swimmer. The<br />

a−<br />

p<br />

exam<strong>in</strong>ation of the aa− p of swimmers at various times <strong>in</strong> the season<br />

may identify changes <strong>in</strong> technical efficiency.

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