Biomechanics and Medicine in Swimming XI
Biomechanics and Medicine in Swimming XI
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 />
Graphic Removal of Water Wave Impact <strong>in</strong> the Pool<br />
Wall dur<strong>in</strong>g the Flip Turn<br />
Pereira, s.M. 1,2 , Gonçalves, P. 2 , Fern<strong>and</strong>es, r.J. 2 , Machado, l. 2 ,<br />
roesler, h. 1 , Vilas-Boas, J.P. 2<br />
1 University of the State of Santa Catar<strong>in</strong>a, Florianópolis, Brazil<br />
2 University of Porto, Faculty of Sport, Cifi2d, Porto, Portugal<br />
The aim of this study was to develop a graphical removal technique of<br />
the water wave that precedes the contact of the swimmer with the wall<br />
dur<strong>in</strong>g the front-crawl flip turn, as well as to characterize <strong>and</strong> quantify<br />
it. To do this the researchers used an underwater force platform <strong>and</strong> two<br />
digital video cameras. In a pilot approach, a swimmer performed 8 turns<br />
without touch<strong>in</strong>g the wall. Follow<strong>in</strong>g the pilot study, 17 swimmers of<br />
both genders, <strong>in</strong>cluded the swimmer who participated <strong>in</strong> pilot approach,<br />
performed 154 complete flip turns. The water wave was removed graphically<br />
through a rout<strong>in</strong>e programmed <strong>in</strong> MatLab that was based on the<br />
symmetry of the wave, <strong>and</strong> the <strong>in</strong>stant <strong>in</strong> time that the wave made<br />
contact with the wall. The average values for the maximum force of the<br />
wave were similar <strong>in</strong> both trials as well as to those previously published.<br />
Furthermore, the removal technique provided satisfactory results.<br />
Key words: dynamometry, swimm<strong>in</strong>g, flip turn, wave measurement<br />
IntroductIon<br />
To move a body through the aquatic environment, swimmers transmit a<br />
volume of water that is expla<strong>in</strong>ed by hydrodynamic drag. The volume of<br />
water depends, amongst other factors upon the swimmer’s body volume<br />
<strong>and</strong> the speed of travel (Barbosa & Vilas-Boas, 2005).<br />
When the swimmer approaches the wall <strong>in</strong> the turn, some of the<br />
water volume displaced, hits the wall before the swimmer’s feet make<br />
contact. This anticipated force record makes it difficult to assess the real<br />
contact force of the swimmer. It is difficult to calculate the force generated<br />
by the wave <strong>and</strong> to remove it from the total force curve (Blanksby<br />
et al., 1998; Lyttle, 2000; Roesler, 2002).<br />
Blanksby et al. (1998) were the first authors to recognize the presence<br />
of the bow water wave <strong>in</strong> the k<strong>in</strong>etic analysis of the turn <strong>in</strong> breaststroke<br />
swimmers of different ages. These researchers tried to elim<strong>in</strong>ate<br />
the wave’s effects through signal process<strong>in</strong>g. However, as the frequency<br />
of the wave was similar to the frequency of the swimmer’s force signal,<br />
this was not possible to totally elim<strong>in</strong>ate the bow wave without los<strong>in</strong>g a<br />
considerable amount of useful data.<br />
Lyttle <strong>and</strong> Mason (1997) attempted to expla<strong>in</strong> the slope of the wave<br />
shape dur<strong>in</strong>g the k<strong>in</strong>etic analysis of turns <strong>in</strong> front crawl <strong>and</strong> butterfly<br />
swimmers. The data at the <strong>in</strong>stant <strong>in</strong> time that the swimmer touched the<br />
wall (<strong>in</strong>strumented with a 3D force platform) was recorded manually. The<br />
force records from the wave reached a maximum value of 500 N, <strong>and</strong> the<br />
duration of the wave was not mentioned. The authors concluded that the<br />
magnitude of this force was proportional to the size of the force platform<br />
s<strong>in</strong>ce the force recorded by the wave should have been equal to the pressure<br />
generated, multiplied by the surface area of the force platform.<br />
Roesler (2002) conducted a study us<strong>in</strong>g two force platforms, placed<br />
side by side on the wall of the pool, where the swimmer’s contact zone<br />
was only on one of the platforms. Recorded force peak values were<br />
around 371 N with a wave duration of around 0.14 s. The second platform,<br />
even without the swimmer’s contact, detected a load seven times<br />
smaller than the force produced by the wave on the first platform. This<br />
decrease was attributed to the distance that the wave travelled to reach<br />
the second platform.<br />
The aim of the present study was to develop a graphical removal<br />
technique of the bow wave that precedes the contact of the swimmer<br />
with the wall dur<strong>in</strong>g the front-crawl flip turn, as well as characteriz<strong>in</strong>g<br />
<strong>and</strong> quantify<strong>in</strong>g it.<br />
148<br />
Methods<br />
In order to characterize <strong>and</strong> quantify the force time curve produced by<br />
the wave before the turn, an extensometric underwater force platform<br />
was used, developed <strong>in</strong> accordance with Roesler (1997). Dimensions<br />
<strong>and</strong> characteristics were: 500 x 500 x 70 mm, load <strong>and</strong> sensitivity of<br />
4000 <strong>and</strong> 2 N (respectively), natural frequency of 400 Hz, ga<strong>in</strong> = 600.<br />
The force platform allowed data acquisition of force only <strong>in</strong> the perpendicular<br />
component to the surface of the platform. The platform mean<br />
measurement error was calculated after calibration <strong>and</strong> was given from<br />
the weight<strong>in</strong>g values obta<strong>in</strong>ed from the platform <strong>and</strong> the real weight of<br />
dead-weights previously measure <strong>in</strong> a precision scale. The mean difference<br />
between the values acquired on the platform <strong>and</strong> the dead weights<br />
was less than 1%. The acquired signals were converted by an analog to<br />
digital (A / D) converter, with a 16 bit resolution (BIOPAC Systems,<br />
Inc.) <strong>and</strong> with <strong>in</strong>put voltage of ± 10 volts. The acquisition rate was of<br />
1000 Hz, powered by a 12 volts source, which allowed the subsequent<br />
import of the signal to a PC.<br />
The platform was set <strong>in</strong> an upright position on the opposite wall of<br />
the start<strong>in</strong>g blocks, <strong>in</strong> a metallic support that also <strong>in</strong>cluded a sta<strong>in</strong>less<br />
steel frame for improved comfort <strong>and</strong> safety of the swimmer. As the<br />
platform was 0.7 m apart from the turn<strong>in</strong>g wall, the black l<strong>in</strong>es at the<br />
bottom of the pool were modified to fit the new sett<strong>in</strong>g, rema<strong>in</strong><strong>in</strong>g at the<br />
official distance to allow normal turn<strong>in</strong>g performances.<br />
Data from the force platform were acquired through the program<br />
Acqknowledge ® (BIOPAC System Inc.). Signal process<strong>in</strong>g was programmed<br />
<strong>in</strong>to a MatLab base <strong>and</strong> consisted of: calibration, filter<strong>in</strong>g<br />
(Butterworth 4th order, with a cutoff frequency of 100 Hz) <strong>and</strong> DC<br />
offset removal. Normalization was done digitally by the program shar<strong>in</strong>g<br />
files <strong>and</strong> turned over by the force of the weight of the swimmer.<br />
Two video cameras were used to monitor the water <strong>and</strong> the swimmer<br />
movements, particularly the time of the <strong>in</strong>itial contact of the swimmer<br />
at the force platform. A digital type HC42E Sony camera was <strong>in</strong>stalled<br />
<strong>in</strong> a waterproof case (Sony SPK-HCB) <strong>and</strong> attached to the bottom of<br />
the pool perpendicular to the swimmers direction of movement (frontal<br />
to sagittal <strong>in</strong>termediate plan). A surveillance video camera (type B7W<br />
submergible camera - AC 230V) was fixed at the bottom of the pool,<br />
fac<strong>in</strong>g upward perpendicular to the swimm<strong>in</strong>g direction (frontal plan),<br />
<strong>in</strong> order to monitor the movement of the wave dur<strong>in</strong>g the turn.<br />
When the swimmer started swimm<strong>in</strong>g towards to the turn<strong>in</strong>g wall,<br />
a trigger was activated to the A/D convert<strong>in</strong>g system, which connected<br />
a underwater light visible by the video cameras. This process allowed<br />
synchroniz<strong>in</strong>g the video setup <strong>and</strong> the force records.<br />
A male swimmer of 22 years old, 1.82 m <strong>in</strong> height <strong>and</strong> 84.9 kg body<br />
weight, f<strong>in</strong>alist of spr<strong>in</strong>t races at the Portuguese National Championships,<br />
performed 8 flip turns. He started from the center of the pool,<br />
12.5 m apart from the turn<strong>in</strong>g wall, with maximum speed, but without<br />
touch<strong>in</strong>g the platform, as shown <strong>in</strong> Figure 1.<br />
Figure 1. Sequence of images of the wave generated by the movement of<br />
the swimmer perform<strong>in</strong>g the turn without touch<strong>in</strong>g the force platform.