Biomechanics and Medicine in Swimming XI
Biomechanics and Medicine in Swimming XI
Biomechanics and Medicine in Swimming XI
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These trials allowed verify<strong>in</strong>g that the force signal produced by the wave<br />
was reasonably symmetric (Fig. 3). In normal turn<strong>in</strong>g situations, swimmers<br />
touch the platform, allow<strong>in</strong>g it to record the swimmer’s push<strong>in</strong>g<br />
action aga<strong>in</strong>st the wall. However, as already stated, before the swimmer<br />
touches the wall, a water wave hits the platform be<strong>in</strong>g also recorded. To<br />
remove this extraneous force, two assumptions were made: (i) the wave<br />
force to time curve be<strong>in</strong>g symmetrical, <strong>and</strong> (ii) that the peak value of the<br />
water wave force occurs at the time <strong>in</strong>stant of swimmer’s wall contact.<br />
From the force platform data was extracted the time of water wave force<br />
start, <strong>and</strong> from the image-based k<strong>in</strong>ematics the time of swimmer’s first<br />
contact was obta<strong>in</strong>ed. We assume this to be co<strong>in</strong>cident with half water<br />
wave curve. This half force to time curve of the water wave was then mirrored<br />
<strong>and</strong> its values were subtracted from the total force values registered<br />
by the platform (Fig. 2) to allow obta<strong>in</strong><strong>in</strong>g: (i) the swimmer’s contact<br />
force to time curve, <strong>and</strong> (ii) the water wave force to time curve.<br />
Solid l<strong>in</strong>e: force registered; dotted<br />
l<strong>in</strong>e: wave mirror<strong>in</strong>g; vertical<br />
l<strong>in</strong>e: time of contact<br />
Solid l<strong>in</strong>e: force registered; dotted<br />
l<strong>in</strong>e: force after wave removal;<br />
vertical l<strong>in</strong>e: time of contact<br />
Figure 2. Graphical representation of the removal of the water wave of<br />
the total force to time curve obta<strong>in</strong>ed dur<strong>in</strong>g a crawl flip turn.<br />
With a sample of 17 swimmers, 9 males <strong>and</strong> 8 females, aged 17.88 ±<br />
3.19 years, height 1.73 ± 0.09, body mass 64.48 ± 11.90 kg, all participants<br />
at the Absolute Portuguese National Championships, 154 valid<br />
turns were analysed. The force to time curve produced by the water wave<br />
was elim<strong>in</strong>ated graphically from the force to time curve produced by<br />
the swimmer’s contact. Moreover, the wave force to time curve was also<br />
treated to characterize their ma<strong>in</strong> characteristics. Descriptive statistics<br />
were used for data analysis.<br />
RESULTS<br />
The force curves generated by the water wave obta<strong>in</strong>ed without the<br />
swimmer touch<strong>in</strong>g the wall resulted <strong>in</strong> a mean curve (Fig. 3).<br />
Figure 3. Mean force curve of the water wave generated by the displacement<br />
of the swimmer dur<strong>in</strong>g the turn without touch<strong>in</strong>g the force<br />
platform.<br />
chaPter2.<strong>Biomechanics</strong><br />
It is possible to observe that the behavior of the curve is not l<strong>in</strong>ear but<br />
follows a pattern tend<strong>in</strong>g to a symmetrical condition, as observed before<br />
by Fujishima (1999). Mean results obta<strong>in</strong>ed for the quantitative parameters<br />
of the water wave obta<strong>in</strong>ed with the turns performed without<br />
touch<strong>in</strong>g the wall are presented <strong>in</strong> Table 1, as well as the data regard<strong>in</strong>g<br />
eight turns from the same swimmer touch<strong>in</strong>g the wall <strong>and</strong> the 154 turns<br />
performed by the total sample of 17 swimmers.<br />
Table 1. Mean values (Mean) ± st<strong>and</strong>ard deviations (SD) obta<strong>in</strong>ed for<br />
the variables: maximum <strong>and</strong> mean force value produced by the water<br />
wave, <strong>and</strong> wave impulse, grouped <strong>in</strong> normalized <strong>and</strong> absolute values <strong>in</strong> 3<br />
situations of wave measurement dur<strong>in</strong>g the flip turn.<br />
WAVE DATA<br />
Turn<strong>in</strong>g trials<br />
8 turns without<br />
touch<strong>in</strong>g the wall<br />
8 turns touch<strong>in</strong>g<br />
the wall<br />
154 turns touch<strong>in</strong>g<br />
the wall<br />
NORMALIZADED VALUES ABSOLUT VALUES<br />
Maximal<br />
(N/bw)<br />
Mean ±<br />
SD<br />
Mean (N/<br />
bw)<br />
Mean ±<br />
SD<br />
Impulse<br />
(N.s/bw)<br />
Mean ±<br />
SD<br />
0.38 ± 0.77 0.16 ± 0.33 0.01 ± 0.002<br />
0.52 ± 0.12 0.24 ± 0.06 0.01 ± 0.008<br />
0.49 ± 0.24 0.19 ± 0.12 0.04 ± 0.02<br />
Maximal<br />
(N)<br />
Mean ±<br />
SD<br />
320.17 ±<br />
65.59<br />
448.88 ±<br />
106.32<br />
323.17 ±<br />
191.94<br />
Mean<br />
(N)<br />
Mean ±<br />
SD<br />
140.62 ±<br />
28.05<br />
206.97 ±<br />
65.76<br />
128.68 ±<br />
90.44<br />
Impulse<br />
(N.s)<br />
Mean ±<br />
SD<br />
10.5 ± 0.17<br />
15.44 ± 4.07<br />
27.16 ± 19.29<br />
Figures 4 <strong>and</strong> 5 represent an example of the swimmer’s contact/impulse<br />
force to time curve, before (Fig. 4) <strong>and</strong> after removal (Fig. 5) of the water<br />
wave specific curve. In this case, the wave was almost fully <strong>in</strong>corporated<br />
<strong>in</strong>to the swimmers’ contact curve, <strong>and</strong> the <strong>in</strong>terference of the wave phenomenon<br />
<strong>in</strong>to the swimmers’ k<strong>in</strong>etics is presumably important, mak<strong>in</strong>g<br />
it more difficult to assess the effect of the wave over the impulse curve.<br />
Figure 4. Example of a force to time curve produced dur<strong>in</strong>g a flip turn<br />
with the effect of the water wave impact.<br />
Figure 5. Example of a force to time curve produced dur<strong>in</strong>g a flip turn<br />
without the effect of the water wave impact.<br />
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