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Biomechanics and Medicine in Swimming XI

Biomechanics and Medicine in Swimming XI

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for displac<strong>in</strong>g the body over a given unit of distance (Zamparo et al, 2005).<br />

Furthermore, it is accepted as an important bioenergetical determ<strong>in</strong>ant<br />

of swimm<strong>in</strong>g performance (Wakayoshi et al, 1995; Kjendlie et al., 2004;<br />

Fern<strong>and</strong>es et al., 2006). However, the body of scientific literature needs<br />

approaches on the relationships between the IdC <strong>and</strong> the C <strong>in</strong> try<strong>in</strong>g to<br />

underst<strong>and</strong> how these two variables may be connected. The present study<br />

aimed at assess<strong>in</strong>g relationships between the IdC <strong>and</strong> the C <strong>in</strong> front crawl,<br />

especially at <strong>in</strong>tensities rang<strong>in</strong>g between ~70 % <strong>and</strong> 100% of the maximal<br />

oxygen consumption ( V � O 2 max). We hypothesised that if velocity is<br />

controlled, IdC <strong>and</strong> C are <strong>in</strong>versely related.<br />

Methods<br />

Seven high-level swimmers (17.0 ± 1.8 years; 168.0 ± 8.8 cm; 58.4 ± 8.2<br />

kg) participant <strong>in</strong> national swimm<strong>in</strong>g championships were tested. Mean<br />

(± SD) ma<strong>in</strong> physiological characteristics were: 18.0 (6.9) % of fat mass,<br />

54.9 (10.1) ml.kg -1 .m<strong>in</strong> -1 of V � O 2 max <strong>and</strong> 7.5 (2.4) of blood lactate<br />

concentrations ([La - ]) at <strong>in</strong>tensities correspond<strong>in</strong>g to V � O 2 max. In an<br />

<strong>in</strong>door 25 m swimm<strong>in</strong>g pool, the participants performed an <strong>in</strong>termittent<br />

<strong>in</strong>cremental protocol, with <strong>in</strong>crements of 0.05 m·s -1 each 200 m stage (<strong>and</strong><br />

30 s <strong>in</strong>tervals), until exhaustion (Fern<strong>and</strong>es et al., 2003). Initial velocity<br />

was established accord<strong>in</strong>g to the <strong>in</strong>dividual level of fitness <strong>and</strong> was set<br />

at the swimmer’s <strong>in</strong>dividual performance on the 400 m freestyle m<strong>in</strong>us<br />

seven <strong>in</strong>crements of velocity. Swimm<strong>in</strong>g velocity was controlled us<strong>in</strong>g a<br />

visual pacer (TAR 1.1, GBK-electronics, Aveiro, Portugal) with successive<br />

flash<strong>in</strong>g lights, 2.5 m apart, on the bottom of the pool.<br />

V � O 2 was measured through direct breath-by-breath oximetry (K4<br />

b 2 , Cosmed, Rome, Italy) connected to the swimmer by a respiratory snorkel<br />

<strong>and</strong> valve system (Kesk<strong>in</strong>en et al., 2003). Capillary blood samples (25<br />

µl) for [La - ] analysis were collected from the earlobe at rest, <strong>in</strong> the 30 s rest<br />

<strong>in</strong>terval, at the end of exercise <strong>and</strong> dur<strong>in</strong>g the recovery period (YSI1500L-<br />

Sport auto-analyser, Yellow Spr<strong>in</strong>gs Incorporated, Ohio, USA). The C was<br />

calculated by divid<strong>in</strong>g total energy expenditure (Ė) by velocity (v) <strong>and</strong><br />

converted to SI units, were 1 mlO 2 is equivalent to 20.1 J (Zamparo et al.,<br />

2005; Fern<strong>and</strong>es et al., 2006):<br />

C = Ė /v (1)<br />

The Ė corrected for body mass was calculated us<strong>in</strong>g the V � O 2 net (difference<br />

between the value measured <strong>in</strong> the end of the stage <strong>and</strong> the rest<br />

value), <strong>and</strong> the blood lactate net (difference between the value measured<br />

<strong>in</strong> two consecutive stages) transformed <strong>in</strong>to V � O 2 equivalents us<strong>in</strong>g a<br />

2.7mlO 2 kg -1 mmol -1 proportionality constant <strong>and</strong> by Equation (2) (cf.<br />

Fern<strong>and</strong>es et al., 2006)<br />

Ė = V� O2net + [La-]net (2)<br />

Two video cameras (JVC GR-SX1 SVHS <strong>and</strong> JVC GR-SXM 25 SVHS)<br />

were fixed on the lateral wall of the pool at a 10 m distance perpendicular<br />

to the swimmers’ plane of movement. The cameras were connected to<br />

a double entry <strong>and</strong> edited on a mix<strong>in</strong>g table (Panasonic Digital Mixer<br />

WJ-AVE55 VHS), provid<strong>in</strong>g a dual-media image (Panasonic AG 7355),<br />

below <strong>and</strong> above the water surface (Vilas-Boas et al., 2006), at a frequency<br />

of 50 Hz (1:250/s shutter speed).<br />

For each step of the <strong>in</strong>cremental protocol, two arm strokes were analysed<br />

<strong>in</strong> every 50 m of the 200 m. Arm strok<strong>in</strong>g coord<strong>in</strong>ation was obta<strong>in</strong>ed<br />

through IdC (Chollet et al., 2000), be<strong>in</strong>g each arm stroke broken down<br />

<strong>in</strong>to four phases: (i) entry <strong>and</strong> catch (correspond<strong>in</strong>g to the time between<br />

the entry of the h<strong>and</strong> <strong>in</strong>to the water <strong>and</strong> the beg<strong>in</strong>n<strong>in</strong>g of its backward<br />

movement); (ii) pull (correspond<strong>in</strong>g to the time between the beg<strong>in</strong>n<strong>in</strong>g<br />

of the h<strong>and</strong>’s backward movement <strong>and</strong> its arrival <strong>in</strong> a vertical plane to the<br />

shoulder); (iii) push (correspond<strong>in</strong>g to the time from the position of the<br />

h<strong>and</strong> below the shoulder to its release from the water) <strong>and</strong> (iv) recovery<br />

(correspond<strong>in</strong>g to the po<strong>in</strong>t of water release to water re-entry of the arm,<br />

i.e., the above water phase). The duration of each phase was measured<br />

for each arm-stroke cycle with a precision of 0.02 s. The duration of the<br />

propulsive phases was the addition of the pull <strong>and</strong> the push phases, <strong>and</strong><br />

the duration of the non-propulsive phases was obta<strong>in</strong>ed by the sum of<br />

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

the catch <strong>and</strong> the recovery phases (the duration of a complete arm-stroke<br />

was the sum of the propulsive <strong>and</strong> non-propulsive phases). The IdC was<br />

calculated as the time gap between the propulsion of the two arms as a<br />

percentage of the duration of the complete arm stroke cycle. Higher negative<br />

percentage values expressed an evident discont<strong>in</strong>uity <strong>in</strong> the <strong>in</strong>ter-arm<br />

propulsion, tend<strong>in</strong>g to IdC=0% as the time gap was dim<strong>in</strong>ish<strong>in</strong>g.<br />

Mean ± SD computations for descriptive analysis were obta<strong>in</strong>ed <strong>in</strong><br />

each stage for all variables (all data were checked for distribution normality<br />

with the Shapiro-Wilk test). Pearson correlation coefficient <strong>and</strong> partial<br />

correlation were applied. Level of significance was established at 5%.<br />

results<br />

The mean ± SD values of velocity, % V � O 2 max, C, <strong>and</strong> IdC, obta<strong>in</strong>ed <strong>in</strong><br />

each step dur<strong>in</strong>g the <strong>in</strong>termittent <strong>in</strong>cremental test, are presented <strong>in</strong> Table<br />

1. An <strong>in</strong>crease of swimm<strong>in</strong>g <strong>in</strong>tensity implies an <strong>in</strong>crease of both C <strong>and</strong><br />

IdC (Table 1).<br />

Table 1. Mean values of velocity, % V� O2max, IdC <strong>and</strong> C obta<strong>in</strong>ed <strong>in</strong><br />

each 200 m step of the <strong>in</strong>cremental protocol (n=7).<br />

Step velocity (m·s-1 ) % V� O2max C ( J·kg-1 ·m-1 1 1.15 ± 0.1 72.1 ± 8.7<br />

)<br />

9.4 ± 2.5<br />

IdC (%)<br />

-12.5 ± 2.5<br />

2 1.20 ± 0.1 76.5 ± 9.1 10.3 ± 2.8 -12.1 ± 2.7<br />

3 1.25 ± 0.1 77.8 ± 5.3 10.1 ± 3.0 -11.8 ± 2.6<br />

4 1.30 ± 0.1 85.5 ± 3.3 11.5 ± 3.2 -10.9 ± 2.6<br />

5 1.35 ± 0.1 90.9 ± 3.2 12.7 ± 2.8 -9.7 ± 2.7<br />

6 1.40 ± 0.1 97.3 ± 3.2 13.7 ± 2.4 -8.2 ± 2.7<br />

7 1.45 ± 0.1 100.0 ± 0.0 14.0 ± 4.2 -6.8 ± 2.5<br />

The relationships between velocity <strong>and</strong> C, <strong>and</strong> velocity <strong>and</strong> IdC are<br />

shown <strong>in</strong> Fig. 1 (left panel), be<strong>in</strong>g possible to observe a high correlation<br />

value between these variables (r=0.98 <strong>and</strong> r=0.99, respectively, both for<br />

p

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