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Biomechanics and Medicine in Swimming XI

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may be assumed that the most difficult element of monof<strong>in</strong> swimm<strong>in</strong>g<br />

is the proper range of motion <strong>in</strong> the ankle jo<strong>in</strong>ts; (4) an analysis of the<br />

differences between value of errors performed, suggests the parameter<br />

most differentiat<strong>in</strong>g the fastest from the slowest swimmer, is the angle<br />

of bend of the feet <strong>in</strong> relation to the shanks (19.5%). The angle of attack<br />

of distal part of the f<strong>in</strong> (11.5%) placed second <strong>in</strong> the rank<strong>in</strong>g mentioned.<br />

The differences between values of errors <strong>in</strong> terms of the angle of bend <strong>in</strong><br />

the proximal part of the f<strong>in</strong> (7.3%) <strong>and</strong> angle of attack of the entire f<strong>in</strong><br />

(6.8%) was the lowest, even when most similar. (5) The errors estimated<br />

high correlated to swimm<strong>in</strong>g <strong>in</strong>tracycle velocity.<br />

Angular Displacement [deg]<br />

220<br />

200<br />

180<br />

160<br />

140<br />

M900 4 16 20 30<br />

ERROR ERROR<br />

M600 5 17 27 29<br />

ERROR ERROR<br />

120<br />

M300 4 21 24 33<br />

TIME [s] (Sampl<strong>in</strong>g frequency 50Hz)<br />

ERROR ERROR<br />

100<br />

1 3 5 7 9 11 13 15 17 19 21 23 25 27 29 31 33 35 37<br />

KAT1ER<br />

KAT6ER<br />

KAT1COR<br />

KAT6COR<br />

KAT3ER<br />

KAT9ER<br />

KAT3COR<br />

KAT9COR<br />

Ma M100 4<br />

ERROR<br />

17 19<br />

ERROR<br />

33<br />

M-HIGHEST SPEED<br />

SUMM OF ERRORS [%]<br />

M-LOWEST SPEED AVERAGE SD<br />

KAT<br />

58,1<br />

77.6<br />

71,5<br />

8,4<br />

ATM<br />

26,4<br />

33,7<br />

34,6<br />

6,1<br />

HME<br />

22,4<br />

33,6<br />

34,6<br />

6,1<br />

HTE<br />

29,8<br />

36,6<br />

42,5<br />

8,5<br />

Figure 2. Graph illustrat<strong>in</strong>g scope of errors (ER) <strong>in</strong> angle of the foot<br />

flexion <strong>in</strong> relation to shank (KAT) <strong>in</strong> time function. At left are sequences<br />

of movement illustrat<strong>in</strong>g the range of errors showed <strong>in</strong> the graph.<br />

Sum of errors by fastest <strong>and</strong> slowest swimmers compared to average<br />

value calculated for all swimmers.<br />

Table 1. Pearson’s correlation coefficients between value of error <strong>in</strong> cycle<br />

made by all subjects on 100-m sections, <strong>and</strong> average velocity (ranked by<br />

average velocity). (KAT) – angle of bend <strong>in</strong> foot at ankle jo<strong>in</strong>t; (ATM) –<br />

angle of bend <strong>in</strong> tail of monof<strong>in</strong>; (HME) – angle of attack of distal part<br />

of f<strong>in</strong>, (HTE) – angle of attack of entire surface of f<strong>in</strong>.<br />

SUBJECT KAT ATM HME HTE SUBJECT KAT ATM HME HTE<br />

M -0,94 -0,99 -0,62 -0,99 P -0,66 -0,88 -0,90 -0,89<br />

A -0,99 -0,55 -0,72 -1,00 S -0,79 -0,96 -0,85<br />

B -0,71 -0,94 -1,00 -0,70 N -0,77 -0,52<br />

The follow<strong>in</strong>g determ<strong>in</strong>ant movement sequences were estimated. The<br />

end of the downbeat movement, where the knee jo<strong>in</strong>ts straighten, the<br />

legs are straight, the feet are <strong>in</strong> their lowest downbeat position, the tail<br />

is at maximum bent at the maximum angle of attack of the entire surface<br />

of the f<strong>in</strong> (Table 2(1)). The change ankle jo<strong>in</strong>t angle <strong>and</strong> the angle<br />

between proximal part of the f<strong>in</strong> <strong>and</strong> the feet is dur<strong>in</strong>g the downbeat<br />

– beg<strong>in</strong>n<strong>in</strong>g of the phase where the legs are maximally flexed <strong>and</strong> the<br />

segments of the f<strong>in</strong> are more or less parallel (Table 2(3)) <strong>and</strong> f<strong>in</strong>ally, dur<strong>in</strong>g<br />

upbeat – the last part of upward movement, with legs straightened,<br />

just before flex<strong>in</strong>g at the knees, at the maximum bend of the tail of the<br />

f<strong>in</strong> (Table 2(2)). The determ<strong>in</strong>ant movement sequence referr<strong>in</strong>g to the<br />

change of angle of the distal part of the f<strong>in</strong> <strong>and</strong> its entire surface is <strong>in</strong> the<br />

downbeat - the second part of legs straighten<strong>in</strong>g at the knees, where the<br />

shanks are more or less parallel to the direction of swimm<strong>in</strong>g <strong>and</strong> the<br />

monof<strong>in</strong> is more or less straight <strong>in</strong> the maximum angle of attack (Table<br />

2(4)). Dur<strong>in</strong>g upbeat – the second part of the lifted legs straightened<br />

with the knees up, until the legs are placed more or less parallel to direction<br />

of swimm<strong>in</strong>g <strong>and</strong> the monof<strong>in</strong> is at maximum bend <strong>in</strong> the middle<br />

(Table 3(5)). The key elements <strong>in</strong> the movement structure of legs <strong>and</strong><br />

monof<strong>in</strong> were also described (Table 1).<br />

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

Table 2. The determ<strong>in</strong>ant sequence of leg movements <strong>and</strong> monof<strong>in</strong><br />

(1,2,3,4,5) arranged with the key elements <strong>in</strong> the structure of monof<strong>in</strong><br />

<strong>and</strong> leg movements (A,B,C,D).related to occurrence of errors.<br />

dIscussIon<br />

Errors <strong>in</strong> propulsive movement structure <strong>and</strong> their impact on swimm<strong>in</strong>g<br />

speed, are relevant to the pr<strong>in</strong>ciple of equilibrium of momentum<br />

due to the <strong>in</strong>teraction between the water <strong>and</strong> swimmer. Without errors<br />

momentum transfer between the subsequent leg segments <strong>and</strong> the<br />

monof<strong>in</strong>, is most effective (Rejman, 2006). Therefore, the determ<strong>in</strong>ant<br />

sequence <strong>in</strong>itiated <strong>in</strong> the category of quality of momentum transfer, occurs<br />

between subsequent elements of the feet - parts of the monof<strong>in</strong>‘s<br />

cha<strong>in</strong>.<br />

The swimmers tested <strong>in</strong> this study show a low level of control over<br />

feet movement while execut<strong>in</strong>g propulsion actions. The angle of bent<br />

of the feet <strong>in</strong> relation to the shanks is the most difficult element of the<br />

movement structure (Figure 2). Additionally, chang<strong>in</strong>g this angle <strong>in</strong><br />

the function of time <strong>and</strong> layout of errors, demonstrates the least mutual<br />

similarity among the parameters tested. The dom<strong>in</strong>ant role of foot<br />

movement <strong>in</strong> generat<strong>in</strong>g propulsion is revealed <strong>in</strong> results ga<strong>in</strong>ed from<br />

the construction of a neural network (Rejman <strong>and</strong> Ochmann, 2009) as<br />

well as research on factors support<strong>in</strong>g ma<strong>in</strong>tenance of consistent high<br />

<strong>in</strong>fracycle monof<strong>in</strong> swimm<strong>in</strong>g velocity (Rejman, 2006). The aim of<br />

these suggestions was to avoid plac<strong>in</strong>g the f<strong>in</strong> parallel to the direction of<br />

swimm<strong>in</strong>g. The results confirmed that, the feet as an active (under total<br />

control of the swimmer) element <strong>in</strong> the biomechanical cha<strong>in</strong> are the<br />

f<strong>in</strong>al l<strong>in</strong>k of torque transfer from the legs to the surface of the f<strong>in</strong> (Rejman,<br />

2006). Hence, correct movement <strong>in</strong> this element of the sequence<br />

structure of propulsion seems to be important. Cognitive control of foot<br />

movement allows for self-correction of swimm<strong>in</strong>g technique. The tendency<br />

toward excessive plantar flexion of the feet (observed generally,<br />

not only <strong>in</strong> the research group) thus seems unjustified from the po<strong>in</strong>t of<br />

view of swimm<strong>in</strong>g efficiency<br />

An analysis of the value of sum of errors made by swimmers <strong>in</strong>dicated<br />

similarities between angle of bend <strong>in</strong> the tail of the monof<strong>in</strong><br />

(ATM) <strong>and</strong> angle of attack of the distal part of the f<strong>in</strong> (HME) (Figure<br />

2). Similarities were also noted when compar<strong>in</strong>g the values of difference<br />

between angle of bend <strong>in</strong> the tail of the monof<strong>in</strong> (ATM) <strong>and</strong> angle of<br />

attack of the entire surface of the f<strong>in</strong> (HTE) This may <strong>in</strong>dicate that<br />

the bend<strong>in</strong>g of the tail of the f<strong>in</strong>, <strong>in</strong>fluences the change <strong>in</strong> shape of the<br />

monof<strong>in</strong>’s surface. It is accepted that the tail is the place where transfer<br />

of torque, generated by the legs, to the surface of the f<strong>in</strong> is performed<br />

(Rejman, 2006). With this <strong>in</strong> m<strong>in</strong>d, the tail is the key element <strong>in</strong> analyz<strong>in</strong>g<br />

the biomechanical cha<strong>in</strong>, divid<strong>in</strong>g it <strong>in</strong>to parts consist<strong>in</strong>g of leg segments<br />

<strong>and</strong> monof<strong>in</strong> segments. Support<strong>in</strong>g this thesis are results show<strong>in</strong>g<br />

that the optimal plantar flexion dur<strong>in</strong>g downbeat, limits the bend of the<br />

tail, as a result optimiz<strong>in</strong>g the angle of attack of the proximal part of<br />

the f<strong>in</strong>. Optimal dorsal flexion of the feet dur<strong>in</strong>g upbeat causes greater<br />

tail bend<strong>in</strong>g <strong>and</strong> consequently, the angle of attack of the distal part <strong>and</strong><br />

entire f<strong>in</strong>, achieves optimum range <strong>in</strong> both phases of the cycle (Rejman<br />

<strong>and</strong> Ochmann, 2009). These suggestions are confirmed <strong>in</strong> the present<br />

work. Greater optimization of tail bend, with<strong>in</strong> limits established <strong>in</strong> the<br />

161

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