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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 />

Hydrodynamic Characterization of the First <strong>and</strong><br />

Second Glide Positions of the Underwater Stroke<br />

Technique <strong>in</strong> Breaststroke<br />

costa, l. 1 ; ribeiro, J. 1 ; Figueiredo, P. 1 ; Fern<strong>and</strong>es, r.J. 1 ; Mar<strong>in</strong>ho,<br />

d. 2,3 ; silva, A.J. 3,4 ; rouboa, A. 3,4 ; Vilas-Boas, J.P. 1 ; Machado,<br />

l. 1<br />

1 University of Porto, Faculty of Sport, Cifi2d, Porto, Portugal<br />

2 University of Beira Interior, Covilhã, Portugal<br />

3 Research Center In Sports, Health <strong>and</strong> Human Development, Vila Real,<br />

Portugal<br />

4 University of Trás-os-Montes <strong>and</strong> Alto Douro, Vila Real, Portugal<br />

The aim of the present study was to characterize two different ventral<br />

glide positions, both used after start <strong>and</strong> turns: the arms extended at the<br />

front, <strong>and</strong> the arms extended along the trunk, respectively the first <strong>and</strong><br />

the second glide positions of the breaststroke underwater stroke. Inverse<br />

Dynamics was used for obta<strong>in</strong><strong>in</strong>g the passive drag <strong>and</strong> the drag coefficient,<br />

based upon the velocity to time curve of each glide, monitored<br />

through a swim-meter. The first glide position presented lower values<br />

of drag <strong>and</strong> drag coefficient, manag<strong>in</strong>g to reach higher velocities. The<br />

cross sectional area (planimetry) values were lower for first glide position<br />

<strong>in</strong> comparison with the second one (759.95 ±124.12 cm2 vs. 814.46 ±<br />

111.23 cm2). These results po<strong>in</strong>t out the need of technical evaluation<br />

<strong>and</strong> control <strong>in</strong> order to reduce drag dur<strong>in</strong>g swimm<strong>in</strong>g performance.<br />

KeY Words: swimm<strong>in</strong>g, breaststroke, passive drag, drag coefficient,<br />

glid<strong>in</strong>g position<br />

IntroductIon<br />

In swimm<strong>in</strong>g the total event time is determ<strong>in</strong>ed by the start, swim, turn<br />

<strong>and</strong> f<strong>in</strong>ish partial times (Halj<strong>and</strong> <strong>and</strong> Saagpakk, 1994). Starts <strong>and</strong> turns<br />

appear to be a significant part of the total swimm<strong>in</strong>g event time (Vilas-<br />

Boas <strong>and</strong> Fern<strong>and</strong>es, 2003). Chatard et al. (1990) stated that the glid<strong>in</strong>g<br />

phase after starts <strong>and</strong> turns corresponds to 10 to 25% of the total<br />

event time (depend<strong>in</strong>g on events <strong>and</strong> the length of the swimm<strong>in</strong>g pool).<br />

D’Acquisto et al. (1988) showed that, dur<strong>in</strong>g the breaststroke events, the<br />

glid<strong>in</strong>g phases represent 44% of the total swimm<strong>in</strong>g time. These authors<br />

showed that the glid<strong>in</strong>g phase dist<strong>in</strong>guishes elite from good level breaststroke<br />

swimmers, with higher glid<strong>in</strong>g time for the elite swimmers. Race<br />

analysis suggested that rather than the start technique used by swimmers;<br />

it is the position under the water that mostly determ<strong>in</strong>es the success of the<br />

start (Cossor <strong>and</strong> Mason, 2001). Therefore, it is essential to analyse <strong>and</strong><br />

underst<strong>and</strong> this phase. The passive drag of swimmers mov<strong>in</strong>g underwater<br />

<strong>in</strong> a streaml<strong>in</strong>ed position has been measured experimentally (Clarys, 1979;<br />

Kolmogorov et al., 1997; Lyttle et al., 2000; Toussa<strong>in</strong>t et al., 2004; Vilas-<br />

Boas et al., <strong>in</strong> press). However, there are other glid<strong>in</strong>g phases <strong>in</strong> which the<br />

swimmers assume a prone position but with the arms extended at the side<br />

of the trunk, as <strong>in</strong> the second glide position after the breaststroke underwater<br />

arm stroke. To our knowledge, these two glide positions were compared<br />

experimentally only by Vilas-Boas et al. (<strong>in</strong> press), <strong>and</strong> numerically<br />

by Mar<strong>in</strong>ho et al. (2009). In both cases, the glides were compared <strong>in</strong> common<br />

velocities, not consider<strong>in</strong>g the total range of velocities at which they<br />

are usually performed. The aim of the present study was to experimentally<br />

characterize the first <strong>and</strong> second glid<strong>in</strong>g positions of the breaststroke underwater<br />

stroke used after starts <strong>and</strong> turns at the total range of velocities<br />

commonly performed, consider<strong>in</strong>g: (i) glid<strong>in</strong>g velocity (v); (ii) body cross<br />

sectional area (S); (iii) drag coefficient (C D ), <strong>and</strong> (iv) passive drag (D).<br />

Methods<br />

Six Portuguese national level male swimmers (18.2 ± 4.0 years old, 178.2<br />

± 9.0 cm of height <strong>and</strong> 64.4 ± 11.4 kg of body mass) participated <strong>in</strong> this<br />

62<br />

study. Test<strong>in</strong>g sessions were conducted <strong>in</strong> a 25 m pool, 2 m deep, with water<br />

temperature at 27.5 ºC. It was used a similar methodology to the described <strong>in</strong><br />

Vilas-Boas et al. (<strong>in</strong> press), namely the S determ<strong>in</strong>ation us<strong>in</strong>g planimetry, <strong>and</strong><br />

the passive drag assessed through <strong>in</strong>verse dynamics based upon the velocity to<br />

time (v (t) ) curve of each glide, monitored through a swim-meter (Lima et al.<br />

2006). Acceleration (a) was obta<strong>in</strong>ed through the numerical derivative of the<br />

velocity curve. The drag force was computed us<strong>in</strong>g the expression:<br />

D = m . a . (1)<br />

To quantify the drag coefficient, the follow<strong>in</strong>g equation was used, assum<strong>in</strong>g<br />

water density (ρ) as 1000 kg/m3 :<br />

C D = 2 D / ρ S v 2 (2)<br />

Each swimmer performed 3 repetitions of the breaststroke underwater stroke,<br />

at maximal <strong>in</strong>tensity (2 m<strong>in</strong> of <strong>in</strong>terval). Dur<strong>in</strong>g the rest <strong>in</strong>terval, swimmers<br />

received proper feedback <strong>in</strong> order to improve their performance. The video<br />

images <strong>and</strong> data process<strong>in</strong>g (v (t) curves <strong>and</strong> acceleration to time curves representations)<br />

of the first <strong>and</strong> second glide of the underwater breaststroke were<br />

obta<strong>in</strong>ed accord<strong>in</strong>g to Vilas-Boas et al. (<strong>in</strong> press). Not all swimmers atta<strong>in</strong>ed<br />

all velocity values, be<strong>in</strong>g reta<strong>in</strong>ed the v values (<strong>in</strong>dependently <strong>in</strong> each glide)<br />

for which there were values from at least three swimmers. The processes of D<br />

<strong>and</strong> C D calculations were described also <strong>in</strong> Vilas-Boas et al. (<strong>in</strong> press).<br />

results<br />

The ma<strong>in</strong> results of this study are presented <strong>in</strong> Table 1 <strong>and</strong> <strong>in</strong> Figures<br />

1 <strong>and</strong> 2. Table 1 shows the S values for each swimmer <strong>in</strong> the first <strong>and</strong><br />

second glides while Fig. 1 <strong>and</strong> 2 show D <strong>and</strong> C D , respectively, for each<br />

glide <strong>and</strong> for all v values atta<strong>in</strong>ed.<br />

Table 1. Individual <strong>and</strong> mean ± SD values of the cross-sectional area of<br />

the body (S) assessed for the two studied breaststroke glid<strong>in</strong>g positions.<br />

Swimmer<br />

S (cm2)<br />

for first glide position<br />

S (cm2)<br />

for second glide position<br />

1 971.13 942.1<br />

2 719.73 886.91<br />

3 641.7 668.47<br />

4 689.17 769.24<br />

5 692.6 718.05<br />

6 845.34 901.99<br />

Mean ± SD 759.95 ±124.12 814.46 ± 111.23<br />

The mean ± SD v values for the first <strong>and</strong> second glide positions were<br />

1.50 ± 0.22m/s <strong>and</strong> 1.15 ± 0.24m/s, respectively. The first glide presented<br />

higher values of mean v, while the second glid<strong>in</strong>g was characterized<br />

by higher values of acceleration (0.61 ± 0.24m/s 2 to 0.66 ± 0.06m/<br />

s 2 versus 0.40 ± 0.06 m/s 2 to 0.63 ± 0.16m/s 2 for common values of v,<br />

second <strong>and</strong> first glide respectively). The common velocities for the two<br />

glid<strong>in</strong>g phases were 1.20, 1.30, 1.40 <strong>and</strong> 1.50m/s (Fig. 1 <strong>and</strong> 2)<br />

Drag (N) first glide<br />

80<br />

second glide<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

0.8 0.9 1 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8<br />

Velocity (m/s)<br />

Figure 1. Drag versus velocity curve <strong>in</strong> two dist<strong>in</strong>ct glid<strong>in</strong>g positions:<br />

first glide <strong>and</strong> second glide of the breaststroke underwater stroke

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