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Biomechanics and Medicine in Swimming XI

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Ankle<br />

Figure 2. Diagram 0.5 of the robot’s k<strong>in</strong>ematics<br />

chaPter2.<strong>Biomechanics</strong><br />

-0.5<br />

0 20 40 60 80 100<br />

results<br />

Kick amplitudes did 0.3not<br />

appeared as a significant parameter (p>0.05). 0.3 0.6<br />

0<br />

However, snorkell<strong>in</strong>g kicks substantially differed <strong>in</strong> frequency <strong>and</strong><br />

depth. Snorkell<strong>in</strong>g frequency was lower than the two others practices<br />

(Table1). This last 0.1 result agrees with measurement made with different<br />

0.1 0.2<br />

0<br />

0<br />

snorkel f<strong>in</strong>s by Zamparo 0 et al. (2006). The kick depth, def<strong>in</strong>ed as the<br />

higher position of ankle dur<strong>in</strong>g a cycle, showed snorkell<strong>in</strong>g depths closer<br />

to the water surface -0.1 than swimm<strong>in</strong>g <strong>and</strong> body-board values.<br />

0<br />

-0.1 -0.2<br />

-0<br />

-0<br />

Table 1. Ma<strong>in</strong> ankle k<strong>in</strong>ematic parameters for the three practices: frequency,<br />

amplitude,<br />

-0.3<br />

<strong>and</strong> depth of swimm<strong>in</strong>g kicks.<br />

-0.3 -0.6<br />

-0<br />

Frequency Amplitude Depth<br />

Swimm<strong>in</strong>g<br />

-0.5 (Hz)<br />

1.01 0 ± 0.1720 (m)<br />

0.42 40± 0.02<br />

(m)<br />

60 -0.16 80 ± 0.08 100<br />

-0.5-1<br />

0 20 40 60 80 100<br />

-1<br />

Snorkell<strong>in</strong>g<br />

Body-board<br />

0.85 ± 0.19<br />

0.98 ± 0.18<br />

0.36 ± 0.02<br />

0.42 ± Knee 0.02<br />

0.02 ± 0.26<br />

data1<br />

-0.08 ± 0.08<br />

Body-board<br />

Ankle<br />

Swimm<strong>in</strong>g data1<br />

Hip<br />

Snork Bod<br />

1<br />

Concern<strong>in</strong>g the <strong>in</strong>verse dynamics results, torques values gradually <strong>in</strong>-<br />

0.5 1.5<br />

creased from the ankle to the hip jo<strong>in</strong>t. For all jo<strong>in</strong>ts, the highest amplitude<br />

was found around 0.6 the flexion/extension axis.<br />

0.3<br />

1<br />

0<br />

The robot reproduces seven stock swimm<strong>in</strong>g cycles with a st<strong>and</strong>ard<br />

deviation lower than 4%. On the ankle jo<strong>in</strong>t, amplitude patterns are<br />

lower for body-board. 0.2In<br />

knee <strong>and</strong> hip torque amplitudes, no difference<br />

0.5<br />

0.1<br />

0<br />

were found between the three activities. Forces <strong>and</strong> torques patterns<br />

measured on the ankle sensor of the robot showed only one oscillation.<br />

The torque pattern -0.2 computed by the model described a double oscillation<br />

dur<strong>in</strong>g stroke cycle, both <strong>in</strong> the knee <strong>and</strong> the hip (Figure 3). In the<br />

0<br />

-0.1<br />

-0.5<br />

-0<br />

knee jo<strong>in</strong>t, dur<strong>in</strong>g the snorkell<strong>in</strong>g activity, the second upper peak disap-<br />

-0.6<br />

peared, because value of this peak staid negative while the two others<br />

were positive, as well as <strong>in</strong> the second lower peak for body-board activity<br />

-0.3<br />

-1<br />

-0<br />

80<br />

on knee. In the hip jo<strong>in</strong>t, the oscillations were synchronous but snorkel-<br />

-1<br />

l<strong>in</strong>g 100amplitudes were lower 0 than 20 others. 40 60 80 100<br />

-0.5 -1.5<br />

0 20 40 60 80 100<br />

data1 Body-board Swimm<strong>in</strong>g<br />

Figure 3. Evolution of tri-dimensional jo<strong>in</strong>t torques for body-board,<br />

snorkell<strong>in</strong>g Snorkel<strong>in</strong>g <strong>and</strong> swimm<strong>in</strong>g activities.<br />

data1 Bod<br />

Flexion / Extension<br />

Flexion / Extension<br />

Flexion / Extension<br />

Flexion / Extension<br />

0.5<br />

0.3<br />

0.1<br />

0<br />

-0.1<br />

-0.3<br />

0.51<br />

Ankle<br />

Ankle Knee<br />

51<br />

0<br />

0<br />

-0<br />

-0<br />

data1 Bod<br />

1

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