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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 />

Table 1. Swimmer’s general characteristics (n = 8, SD: st<strong>and</strong>ard deviation,<br />

WR: world record, PB: personal best).<br />

Age (years)<br />

200 m freestyle<br />

Body mass (kg) Height (cm)<br />

WR / PB (%)<br />

Mean 22.3 62.2 174.7 96.73<br />

SD 4.1 6.2 5.8 2.25<br />

The swimmers were analysed dur<strong>in</strong>g a crawl tumble turn at maximum<br />

speed, when pass<strong>in</strong>g through a specific pre-calibrated space with mean<br />

dimensions of 4.2 x 1.1 x 1.9 m for the horizontal (ma<strong>in</strong> movement<br />

direction), vertical (pool depth) <strong>and</strong> lateral (lane width) directions, respectively<br />

placed <strong>in</strong> contact with the turn<strong>in</strong>g wall <strong>and</strong> the water surface.<br />

Five stationary m<strong>in</strong>i-DV video cameras (Sony DCR-HC62E <strong>and</strong><br />

DCR-HC96E) were located underwater at different depths <strong>in</strong> waterproof<br />

cases. The angle between axes of adjacent cameras was approximately<br />

45° <strong>and</strong> the five cameras were located on a semi-ellipse centred<br />

on the turn<strong>in</strong>g wall. Twelve to 14 calibration po<strong>in</strong>ts were used, <strong>and</strong> the<br />

synchronization of the images was obta<strong>in</strong>ed us<strong>in</strong>g an underwater strobe<br />

flash (Epoque ES-150 DS α) visible <strong>in</strong> the field of each video camera.<br />

An underwater piezoelectric 3D force platform (Kistler 9253B12) was<br />

also mounted on the turn<strong>in</strong>g wall record<strong>in</strong>g at a frequency of 2000 Hz.<br />

One complete turn was analysed for each swimmer. The test<strong>in</strong>g session<br />

took place <strong>in</strong> a 50 m <strong>in</strong>door pool.<br />

The anatomical reference po<strong>in</strong>ts of <strong>in</strong>terest were digitized manually,<br />

frame by frame (at a frequency of 50 Hz). The po<strong>in</strong>ts digitized for each<br />

camera were: centre of the skull (head), shoulders, elbows, wrists, f<strong>in</strong>gertips,<br />

hips, knees, ankles <strong>and</strong> tiptoes. Image coord<strong>in</strong>ates were transformed<br />

to 3D object-space coord<strong>in</strong>ates us<strong>in</strong>g the Direct L<strong>in</strong>ear Transformation<br />

algorithm (Abdel-Aziz & Karara, 1971). Reconstruction precision of<br />

calibration po<strong>in</strong>ts was 14.1 ± 9.1 mm with a maximal error of 42.8 mm.<br />

Miss<strong>in</strong>g coord<strong>in</strong>ates were <strong>in</strong>terpolated by a cubic spl<strong>in</strong>e function <strong>and</strong><br />

then smoothed by the Savitzky-Golay filter<strong>in</strong>g method (<strong>in</strong>terpolation<br />

order: 2, w<strong>in</strong>dow size: 13).<br />

The k<strong>in</strong>ematic data were the horizontal velocity of the head at the<br />

beg<strong>in</strong>n<strong>in</strong>g of the turn (when the head was 3 m before the wall, VIn <strong>in</strong><br />

m/s), 1 m before the rotation phase (V1mR <strong>in</strong> m/s), at the beg<strong>in</strong>n<strong>in</strong>g<br />

of the rotation phase (VR <strong>in</strong> m/s), at the maximum horizontal force<br />

peak (VPe <strong>in</strong> m/s), at the end of the push-off (VG <strong>in</strong> m/s), at the end<br />

of the glide (VU <strong>in</strong> m/s) <strong>and</strong> at the end of the turn (when the head<br />

was 3 m after the wall, VOut <strong>in</strong> m/s). The delimitation between the<br />

approach <strong>and</strong> the rotation phase was determ<strong>in</strong>ed when the swimmer<br />

<strong>in</strong>creased her head depth (vertical displacement). The horizontal position<br />

of the head when rotation began was also computed (RD <strong>in</strong> m).<br />

The end of the push-off (synchronisation po<strong>in</strong>t with dynamic data) <strong>and</strong><br />

the delimitation between the glide <strong>and</strong> the underwater propulsive phase<br />

was obta<strong>in</strong>ed by observ<strong>in</strong>g video data. This time ended the glide duration<br />

(GT <strong>in</strong> s).<br />

The dynamic data recorded were: maximum horizontal force peak<br />

(Pe <strong>in</strong> N) <strong>and</strong> f<strong>in</strong>al contact time (synchronisation po<strong>in</strong>t with k<strong>in</strong>ematic<br />

data). Vertical <strong>and</strong> lateral forces helped to discern the first contact time<br />

<strong>and</strong> the delimitation between the brak<strong>in</strong>g <strong>and</strong> the push-off phases. PeT<br />

(<strong>in</strong> s) was the time between the beg<strong>in</strong>n<strong>in</strong>g of the push-off <strong>and</strong> the maximum<br />

horizontal force peak. %PeT (<strong>in</strong> %) was the ratio between PeT <strong>and</strong><br />

the push-off duration (PoT <strong>in</strong> s).<br />

Pearson correlation <strong>and</strong> l<strong>in</strong>ear regression tests were used to identify<br />

the relationships among the tumble turn performance criterion<br />

(3mRTT as the time taken to swim from 3 m <strong>in</strong> to 3 m out the turn<strong>in</strong>g<br />

wall, <strong>in</strong> s) <strong>and</strong> both k<strong>in</strong>ematic <strong>and</strong> dynamic factors. The level of significance<br />

was set at 95 % (p

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