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 />
Effects of Reduced Knee-bend on 100 Butterfly<br />
Performance: A Case Study Us<strong>in</strong>g the Men’s Asian<br />
<strong>and</strong> Japanese Record Holder<br />
Ide, t. 1 , Yoshimura, Y. 2 , Kawamoto, K. 3 , takise, s. 1 , Kawakami,<br />
t. 1<br />
1 Osaka University of Health <strong>and</strong> Sport Sciences, Osaka, Japan.<br />
2 Chuo University, Tokyo, Japan.<br />
3 Phoenix Swim Club, Phoenix, Arizona, USA<br />
This article analyzed the 30 year old Asian <strong>and</strong> Japanese record holder<br />
of the men’s 100 meter butterfly. In 2002, Kohei Kawamoto’s best time<br />
was 53.22 seconds, <strong>and</strong> he improved his time to 51.00 seconds <strong>in</strong> 2009.<br />
The most significant difference between Kohei <strong>in</strong> 2002 <strong>and</strong> 2009 was<br />
the focus on a straight leg butterfly kick technique. When compar<strong>in</strong>g<br />
his 2005 stroke to his 2009 stroke, we found that the extent of the<br />
straightness of his butterfly kick improved from 39% to 55% (of >170<br />
degrees knee-bend<strong>in</strong>g). Additionally, this swimmer improved his speed<br />
from 2.5m·s -1 to 2.7m·s -1 , <strong>and</strong> <strong>in</strong>creased his distance per stroke from<br />
1.894m±0.062 to 2.204m±0.131.<br />
Key words: tra<strong>in</strong><strong>in</strong>g, Asian <strong>and</strong> Japanese national record,<br />
Butterfly, straight kick, coach<strong>in</strong>g, swimm<strong>in</strong>g speed Meter.<br />
IntroductIon<br />
Butterfly swimmers should keep their body as horizontal as possible<br />
dur<strong>in</strong>g the propulsive phase of the arm stroke (Maglischo, 2003). In<br />
general, coaches use the technique of ‘wave butterfly’ ( Japan Swimm<strong>in</strong>g<br />
Federation, 2006), <strong>and</strong> the dolph<strong>in</strong> kick technique of bend<strong>in</strong>g the knees.<br />
The wave butterfly arises from body movement, arm-stroke tim<strong>in</strong>g <strong>and</strong><br />
kick tim<strong>in</strong>g (Yoshimura, 1996). Bend<strong>in</strong>g the knees dur<strong>in</strong>g the butterfly<br />
kick <strong>in</strong>creases the undulation of ‘wave butterfly’. Coaches still use the<br />
technique of bend<strong>in</strong>g the knees dur<strong>in</strong>g the butterfly kick, with the purpose<br />
of push<strong>in</strong>g back the water (Fig.2).<br />
S<strong>in</strong>ce 2006, we coached Kawamoto to change his butterfly technique,<br />
employ<strong>in</strong>g a straighter leg-kick. The result was a more horizontal<br />
stroke. Kawamoto’s <strong>in</strong>itial butterfly kick technique used a bend<strong>in</strong>g butterfly<br />
kick. We changed this to a straighter kick with less knee-bend<br />
(Yoshimura, 2008), which is imag<strong>in</strong>ed as ‘hold<strong>in</strong>g the water to the bottom<br />
the pool’ (Fig. 1).<br />
Figure 1. Straight kick.<br />
270<br />
Figure 2. Bend<strong>in</strong>g kick.<br />
Methods<br />
Kohei Kawamoto, 30 years old Asian <strong>and</strong> Japanese record holder of the<br />
men’s 100 meter butterfly (height; 174 cm, body weight; 64kg) volunteered<br />
to participate <strong>in</strong> this study. A comparison was made of Kawamoto’s<br />
performance <strong>in</strong> 2009 to his previous performance <strong>in</strong> 2005. He<br />
performed 4 times 25 meter butterfly swims, whilst be<strong>in</strong>g filmed, from<br />
a push start. The first 15 meters were completed under water us<strong>in</strong>g the<br />
butterfly kick <strong>and</strong> the f<strong>in</strong>al 10 meters swimm<strong>in</strong>g all out butterfly stroke.<br />
A Swimm<strong>in</strong>g Speed Meter (V<strong>in</strong>e, VMS-003, AC100V, 1/500s, 0.2mm/<br />
pulse) us<strong>in</strong>g a wire attached to the swimmer, exported the analogue signals<br />
via an RS232C post to a computer. These signals were used to calculate<br />
swimm<strong>in</strong>g speed (Microsoft W<strong>in</strong>dows Excel; Yoshimura, 2007).<br />
The wire l<strong>in</strong>e of the speed meter was attached to the swimmer by a<br />
belt <strong>and</strong> <strong>in</strong>tracyclic velocity changes were recorded precisely for several<br />
stroke cycles while swimm<strong>in</strong>g at maximum speed. The average velocity<br />
changes for one stroke cycle were calculated with data from all successive<br />
stroke curves. The average number of stroke cycles were compared<br />
(for the 2009 stroke <strong>and</strong> 2005 stroke). A Swimm<strong>in</strong>g Speed Meter, registered<br />
velocity when the subject was at maximum speed with<strong>in</strong> one<br />
stroke cycle, which is dur<strong>in</strong>g the second kick phase. Then comes the<br />
wave phase, <strong>and</strong> first kick phase, <strong>in</strong>sweep phase. Dur<strong>in</strong>g swimm<strong>in</strong>g, the<br />
subject was monitored from the side plane us<strong>in</strong>g an underwater video<br />
camera at a sampl<strong>in</strong>g frequency of 60Hz (Underwater monitor system<br />
2, YAMAHA, Shizuoka, Japan). The angle of the knee bend <strong>and</strong> upper<br />
body movement. were analyzed with the DartTra<strong>in</strong>er.<br />
results<br />
The Swimm<strong>in</strong>g Speed Meter showed that swimm<strong>in</strong>g speeds <strong>in</strong>creased<br />
from 2.5m·s -1 for 2005 to 2.7m·s -1 <strong>in</strong> 2009 (dur<strong>in</strong>g the second kick<br />
phase). Distance per stroke (DPS) <strong>in</strong>creased to 2.204m±0.131 for 2009,<br />
from 1.894m±0.062 <strong>in</strong> 2005 (m) Wicoxon.: p=0.006061, 1 stroke (velocity)<br />
Wicoxon.: p=0.7748) (Figure 3.). Four phases of the 2009 <strong>and</strong><br />
2005’s velocity results were not significantly different (the first kick<br />
phase Wilcoxon: p=0.64850, <strong>in</strong>sweep phase Wilcoxon: p=0.16360, upsweep<br />
<strong>and</strong> second kick phase Wilcoxon: p=0.00606, wave phase Wilcoxon:<br />
0.10910.