16.11.2012 Views

Biomechanics and Medicine in Swimming XI

Biomechanics and Medicine in Swimming XI

Biomechanics and Medicine in Swimming XI

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<strong>Biomechanics</strong><strong>and</strong>medic<strong>in</strong>e<strong>in</strong>swimm<strong>in</strong>gXi<br />

Mechanical <strong>and</strong> Propulsive Efficiency of Swimmers<br />

<strong>in</strong> Different Zones of Energy Supply<br />

Kolmogorov, s.V. 1,2 , Vorontsov, A.r. 2 , rumyantseva, o.A. 1 ,<br />

Kocherg<strong>in</strong>, A.B. 2<br />

1 Pomor State University, Arkhangelsk, Russia<br />

2 All-Russian Swimm<strong>in</strong>g Federation, Moscow, Russia<br />

Dimensionless coefficients for mechanical <strong>and</strong> propulsive efficiency (e g ,<br />

e p ) have been studied us<strong>in</strong>g physiological <strong>and</strong> biomechanical methods <strong>in</strong><br />

swimm<strong>in</strong>g various strokes. The research has been conducted <strong>in</strong> the three<br />

zones of energy supply: below the threshold of anaerobic metabolism<br />

(AT), above the zone of maximal oxygen consumption (VO 2 max ) <strong>and</strong><br />

<strong>in</strong> the zone between AT <strong>and</strong> VO 2 max . The highest values of e g <strong>and</strong> e p for<br />

male <strong>and</strong> female swimmers have been revealed <strong>in</strong> the zone between AT<br />

<strong>and</strong> VO 2 max . In all the three zones of energy supply the values of e g are<br />

higher for male swimmers. At the same time the values of e p are equal<br />

for male <strong>and</strong> female swimmers.<br />

Key words: Metabolic <strong>and</strong> mechanical power, efficiency, velocity<br />

IntroductIon<br />

Development of efficient technologies to tra<strong>in</strong> swimmers assumes<br />

solv<strong>in</strong>g of an important theoretical <strong>and</strong> practical problem of <strong>in</strong>terdependence<br />

between energy supply, on the one h<strong>and</strong>, <strong>and</strong> swimm<strong>in</strong>g<br />

biomechanics, on the other one. In case of biological objects’ steady<br />

non-stationary motion <strong>in</strong> water, at the first stage metabolic energy is<br />

transformed with losses <strong>in</strong>to mechanical one, which at the second stage<br />

is transformed with additional losses <strong>in</strong>to useful activity result, i.e. <strong>in</strong>to<br />

swimm<strong>in</strong>g velocity. To describe precisely basic mechanisms of the phenomenon<br />

under study, this process of human swimm<strong>in</strong>g was formalised<br />

<strong>in</strong> form of mathematic model (Kolmogorov, 1997):<br />

v 0 =P ai × e g × e p /Fr �<br />

110<br />

f .d .�<br />

, (1)<br />

<strong>in</strong> which v 0 is mean swimm<strong>in</strong>g velocity at the competition or tra<strong>in</strong><strong>in</strong>g<br />

distance (m·s -1 ); P ai is power of active energetic metabolism (W);<br />

e g is dimensionless coefficient of mechanical efficiency, i.e. ratio of total<br />

external mechanical power (P to ) to P ai ; e p is dimensionless coefficient of<br />

propulsive efficiency, i.e. ratio of useful external mechanical power (P uo )<br />

to P to ; F r(f.d.) is frontal component of active drag force (N).<br />

Hence, the goal of this research has been to <strong>in</strong>vestigate experimentally<br />

regularities of metabolic energy transformation <strong>in</strong>to swimm<strong>in</strong>g<br />

velocity at different zones of energy supply on the basis of equation 1.<br />

Methods<br />

The research was conducted at the period of spr<strong>in</strong>g tra<strong>in</strong><strong>in</strong>g mesocycle<br />

last<strong>in</strong>g from January to April. Twenty-n<strong>in</strong>e university swimmers (15<br />

female subjects aged from 17 to 22 <strong>and</strong> 14 male subjects aged from<br />

18 to 23) took part <strong>in</strong> the research. Correct study<strong>in</strong>g of regularities of<br />

metabolic energy transformation <strong>in</strong>to useful activity result is possible<br />

only <strong>in</strong> conditions when character <strong>and</strong> direction of tra<strong>in</strong><strong>in</strong>g load carried<br />

out by the subjects dur<strong>in</strong>g the tra<strong>in</strong><strong>in</strong>g mesocycle, are taken <strong>in</strong>to<br />

consideration. Therefore, the time of experimental <strong>in</strong>vestigation of this<br />

process <strong>in</strong> the three different zones of energy supply was coord<strong>in</strong>ated<br />

with certa<strong>in</strong> periods of purposeful technical <strong>and</strong> functional tra<strong>in</strong><strong>in</strong>g. It is<br />

this circumstance that expla<strong>in</strong>s the order of tests.<br />

In February the first test was conducted <strong>in</strong> the zone of energy supply<br />

below the threshold of anaerobic metabolism (AT). Test 1 was carried<br />

out <strong>in</strong> a swimm<strong>in</strong>g pool on the basis of tra<strong>in</strong><strong>in</strong>g series of 8×200 m by the<br />

basic stroke with 45 s breaks.<br />

In March the second test was conducted <strong>in</strong> the zone of energy supply<br />

above the maximal oxygen consumption (VO 2 max ). Test 2 was carried<br />

out <strong>in</strong> the flume, with peri-limit<strong>in</strong>g metabolic power be<strong>in</strong>g applied <strong>in</strong><br />

swimm<strong>in</strong>g by the basic stroke. The work lasted one m<strong>in</strong>ute for spr<strong>in</strong>ters<br />

<strong>and</strong> two m<strong>in</strong>utes for medium distance swimmers.<br />

In April the third test was conducted <strong>in</strong> the zone of energy supply<br />

between AT <strong>and</strong> VO2 max . Test 3 was carried out <strong>in</strong> the flume <strong>in</strong> the<br />

course of tra<strong>in</strong><strong>in</strong>g series of 3×1 m<strong>in</strong>utes (for spr<strong>in</strong>ters) <strong>and</strong> 3×2 m<strong>in</strong>utes<br />

(for medium distance swimmers) by basic stroke, <strong>in</strong>tervals of work <strong>and</strong><br />

rest be<strong>in</strong>g altered as 1:1.<br />

Prelim<strong>in</strong>ary, <strong>in</strong>dividual swimm<strong>in</strong>g velocities <strong>in</strong> all the three zones<br />

of energy supply were calculated for each subject on the basis of special<br />

tests <strong>in</strong> the swimm<strong>in</strong>g pool.<br />

To def<strong>in</strong>e experimentally variables <strong>in</strong> equation 1, a complex of physiological<br />

<strong>and</strong> biomechanical research methods was applied.<br />

The power of active energetic metabolism (Pai , W) <strong>in</strong> all the three<br />

tests was calculated as a ratio of energetic expenditures at the test distance<br />

(E, J) to work time at this distance (t, s). Energetic expenditures<br />

were def<strong>in</strong>ed experimentally by the method of <strong>in</strong>direct calorimetry. For<br />

this purpose, all necessary gaseous parameters of the ventilation air were<br />

measured with the help of the mobile system “MetaMax” <strong>and</strong> lactate<br />

concentration was determ<strong>in</strong>ed <strong>in</strong> capillary blood before <strong>and</strong> after the<br />

test. When the research was conducted <strong>in</strong> the swimm<strong>in</strong>g pool (test<br />

№ 1), gas analytical measurements were taken dur<strong>in</strong>g rest breaks between<br />

tra<strong>in</strong><strong>in</strong>g distances. When the research was conducted <strong>in</strong> the flume<br />

(tests № 2 <strong>and</strong> № 3), gas analytical measurements were taken before,<br />

dur<strong>in</strong>g <strong>and</strong> after the test. All experimental results were reduced to conditions<br />

of STPD. Quantitative values of E were calculated on the basis<br />

of special equations (Capelli et al., 1998; Zamparo et al., 1999), which<br />

correspond entirely to the three studied zones of energetic supply <strong>and</strong><br />

are described <strong>in</strong> detail <strong>in</strong> the specified papers.<br />

Total external mechanical power (Pto ), frontal component of active<br />

drag force (Fr(f.d.) ) <strong>and</strong> useful external mechanical power (Puo ) were<br />

def<strong>in</strong>ed us<strong>in</strong>g a biohydrodynamic method (Kolmogorov, 2008), which<br />

consists of a complex of <strong>in</strong>dependent biomechanical <strong>and</strong> hydrodynamic<br />

methods to measure necessary physical values. At first, total external<br />

mechanical power (Pto max ) was def<strong>in</strong>ed by the method of small perturbations<br />

at the maximal swimm<strong>in</strong>g velocity (v0 max ) (Kolmogorov et.<br />

al., 1997). Afterwards, the correspond<strong>in</strong>g value of Pto exp was calculated<br />

for every experimental swimm<strong>in</strong>g velocity <strong>in</strong> the studied zones of energetic<br />

metabolism (v0 exp ) on the basis of the well-known (Touissant <strong>and</strong><br />

Truijens, 2005) <strong>and</strong> verified experimentally dependence between these<br />

parameters (Kolmogorov <strong>and</strong> Koukovyak<strong>in</strong>, 2001):<br />

3 3<br />

Pto exp =Pto max /v0max× v0exp . (2)<br />

The frontal component of active drag force under conditions of swimmer’s<br />

steady non-stationary forward motion (Fr(f.d.) ) was def<strong>in</strong>ed experimentally<br />

for every experimental swimm<strong>in</strong>g velocity (v0 exp ) us<strong>in</strong>g the<br />

correspond<strong>in</strong>g hydrodynamic method (oriented specially to measure<br />

this physical value) (Kolmogorov, 2008). This paper describes <strong>in</strong> detail<br />

the theory, necessary mathematic models <strong>and</strong> practical technology to<br />

def<strong>in</strong>e Fr(f.d.) with<strong>in</strong> the whole range of v0 exp relevant for the research.<br />

Useful external mechanical power (Puo ) was def<strong>in</strong>ed from the follow<strong>in</strong>g<br />

equation:<br />

P uo = Fr (f.d.) × v0exp.<br />

(3)<br />

When the parameters, <strong>in</strong>dicated above, were def<strong>in</strong>ed for every experimental<br />

swimm<strong>in</strong>g velocity <strong>in</strong> the studied zones of energetic metabolism<br />

(v 0 exp ), dimensionless coefficients of mechanical (e g =P to exp /P ai ) <strong>and</strong> propulsive<br />

(e p = P uo / P to exp ) efficiency were calculated.<br />

results<br />

Tables 1 <strong>and</strong> 2 represent experimental results of the studied process <strong>in</strong><br />

dolph<strong>in</strong> swimm<strong>in</strong>g by a female subject <strong>and</strong> <strong>in</strong> brass by a male subject,<br />

correspond<strong>in</strong>gly. These tables give only key parameters of P ai , e g , e p , F r(f.d.)<br />

<strong>and</strong> v 0 exp which are necessary to solve quantitatively equation (1) <strong>and</strong>

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!