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 />
The protocol consisted of five bouts of 16 repetitions perform<strong>in</strong>g the basic<br />
head-out aquatic exercise “rock<strong>in</strong>g horse” at the “water tempo” immersed<br />
to the xiphoid process (i.e., breast). Bouts <strong>in</strong>tensity were 80 %, 90 %, 100<br />
%, 110 % <strong>and</strong> 120 % of the cadence reported by Barbosa et al. (2009b) to<br />
achieve a 4 mmol.l -1 of blood lactate, represent<strong>in</strong>g respectively 120 b.m<strong>in</strong> -1 ,<br />
135 b.m<strong>in</strong> -1 , 150 b.m<strong>in</strong> -1 , 165 b.m<strong>in</strong> -1 <strong>and</strong> 180 b.m<strong>in</strong> -1 cadences. Musical cadence<br />
was controlled electronically by a metronome (Korg, MA-30, Tokyo,<br />
Japan) connected to a sound system.<br />
The protocol was videotaped <strong>in</strong> sagital plane with a pair of cameras provid<strong>in</strong>g<br />
a dual projection from both underwater (GR-SXM25 SVHS, JVC,<br />
Yokoama, Japan) <strong>and</strong> above (GR-SX1 SVHS, JVC, Yokoama, Japan) the<br />
water surface. The images of both cameras were recorded <strong>in</strong>dependently.<br />
The study comprised the k<strong>in</strong>ematical analysis of the full cycles (Ariel Performance<br />
Analysis System, Ariel Dynamics Inc., USA) through a VCR<br />
(Panasonic, AG 7355, Japan) at a frequency of 50 Hz. Zatsiorsky’s model<br />
with an adaptation by de Leva (1996) was used with the division of the<br />
trunk <strong>in</strong> two articulated parts. To create a s<strong>in</strong>gle image of dual projection as<br />
described previously (Vilas-Boas et al., 1997; Barbosa et al., 2005), the <strong>in</strong>dependent<br />
digitalization from both cameras was reconstructed with the help<br />
of a calibration object (0.675 x 0.855 m; 6 control po<strong>in</strong>ts) <strong>and</strong> a 2D-DLT<br />
algorithm (Abdel-Aziz <strong>and</strong> Karara, 1971). For the analysis of the curve of<br />
the centre of mass’s k<strong>in</strong>ematics a filter with a cut-off frequency of 5 Hz was<br />
used, as suggested by W<strong>in</strong>ter (1990). For the segmental k<strong>in</strong>ematics a cut-off<br />
frequency of 9 Hz was used, near to the value proposed by W<strong>in</strong>ter (1990). A<br />
double-passage filter<strong>in</strong>g for the signal process<strong>in</strong>g was used.<br />
The follow<strong>in</strong>g variables were analysed: (i) cycle period; (ii) 2D l<strong>in</strong>ear<br />
position ranges (foot, h<strong>and</strong> <strong>and</strong> centre of mass), <strong>and</strong> (iii) 2D l<strong>in</strong>ear velocity<br />
ranges (foot, h<strong>and</strong> <strong>and</strong> centre of mass).<br />
The normality of the distributions was assessed with the Shapiro-Wilk<br />
test. L<strong>in</strong>ear regression equations models <strong>and</strong> its coefficients of determ<strong>in</strong>ation<br />
were used to describe the relationships between musical cadence <strong>and</strong> biomechanical<br />
variables. The level of statistical significance was set at p ≤ 0.05.<br />
results<br />
Figure 1 presents a qualitative analysis from the centre of mass k<strong>in</strong>ematics<br />
from a s<strong>in</strong>gle subject dur<strong>in</strong>g the second bout at 135 b.m<strong>in</strong>-1 . Figure 2 displays<br />
the simple scatter gram from the cycle period accord<strong>in</strong>g to the musical<br />
cadence imposed. There was a decrease of the cycle period throughout the<br />
experimental protocol (R2 = 0.83; P < 0.01). Figure 3 <strong>and</strong> 4 presents respectively<br />
the overlay scatter gram for 2D displacement <strong>and</strong> 2D velocity accord<strong>in</strong>g<br />
to the musical cadence imposed. There were non-significant relationship<br />
between horizontal (0.01 < R2 < 0.31) or vertical (0.01 < R2 < 0.03) displacements<br />
with the cadence imposed. On the other h<strong>and</strong>, for the horizontal <strong>and</strong><br />
vertical velocities there were several significant relationships with the musical<br />
cadence. Increased cadence imposed <strong>in</strong>creased centre of mass’ velocities<br />
for its horizontal (R2 = 0.26; P < 0.01) <strong>and</strong> vertical components (R2 = 0.41; P<br />
< 0.01), h<strong>and</strong>’s horizontal velocity (R2 = 0.26; P < 0.01), foot’s horizontal (R2 = 0.23; P = 0.02) <strong>and</strong> vertical (R2 <strong>Biomechanics</strong> <strong>and</strong> <strong>Medic<strong>in</strong>e</strong> <strong>in</strong> Swimm<strong>in</strong>g <strong>XI</strong> Chapter 2 <strong>Biomechanics</strong> b 65<br />
<strong>and</strong> 4 presents respectively the overlay scatter gram for 2D displacement <strong>and</strong> 2D<br />
velocity accord<strong>in</strong>g to the musical cadence imposed. There were non-significant<br />
relationship between horizontal (0.01 < R<br />
= 0.23; P = 0.01) velocities.<br />
2 < 0.31) or vertical (0.01 < R 2 < 0.03)<br />
displacements with the cadence imposed. On the other h<strong>and</strong>, for the horizontal <strong>and</strong><br />
vertical velocities there were several significant relationships with the musical cadence.<br />
Increased cadence imposed <strong>in</strong>creased centre of mass’ velocities for its horizontal (R 2 =<br />
0.26; P < 0.01) <strong>and</strong> vertical components (R 2 = 0.41; P < 0.01), h<strong>and</strong>’s horizontal<br />
velocity (R 2 = 0.26; P < 0.01), foot’s horizontal (R 2 = 0.23; P = 0.02) <strong>and</strong> vertical (R 2 =<br />
0.23; P = 0.01) velocities.<br />
A B<br />
C D<br />
Figure 1. Qualitative analysis from the centre of mass’ horizontal displacement (panel<br />
A), vertical displacement (panel B), horizontal velocity (panel C) <strong>and</strong> vertical velocity<br />
(panel D) from a s<strong>in</strong>gle subject perform<strong>in</strong>g the second bout at 135 b.m<strong>in</strong> -1 Figure 1. Qualitative analysis from the centre of mass’ horizontal displacement<br />
(panel A), vertical displacement (panel B), horizontal velocity . (panel<br />
C) <strong>and</strong> vertical velocity (panel D) from a s<strong>in</strong>gle subject perform<strong>in</strong>g the second<br />
bout at 135 b.m<strong>in</strong>-1 .<br />
138<br />
Figure 2. Simple scatter gram from the cycle period accord<strong>in</strong>g to the<br />
cadence imposed.<br />
Figure 3. Overlay scatter gram from horizontal displacement <strong>and</strong> vertical<br />
displacement accord<strong>in</strong>g to the cadence imposed.