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 />
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>