Biomechanics and Medicine in Swimming XI
Biomechanics and Medicine in Swimming XI
Biomechanics and Medicine in Swimming XI
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AcKnoWledGeMents<br />
Esther Morales would like to thank the University of Granada for the<br />
grant that enabled her to carry out this research. She would also like to<br />
thank the Physical Education <strong>and</strong> Sports Department <strong>and</strong> the Research<br />
Group “CTS-527: Physical Activity <strong>and</strong> Sports <strong>in</strong> Aquatic Environment”<br />
of the University of Granada for the use of equipment <strong>and</strong> help<br />
<strong>in</strong> prepar<strong>in</strong>g this paper <strong>and</strong> the research on which it is based.<br />
132<br />
Advanced Biomechanical Simulations <strong>in</strong> Swimm<strong>in</strong>g<br />
Enabled by Extensions of Swimm<strong>in</strong>g Human<br />
Simulation Model “SWUM”<br />
nakashima, M. 1 , Kiuchi, h. 1 , Maeda, s. 1 , Kamiya, s. 1 , nakajima,<br />
K. 1 , takagi, h. 2<br />
1 Tokyo Institute of Technology, Tokyo, Japan<br />
2 University of Tsukuba, Tsukuba, Japan<br />
S<strong>in</strong>ce the authors presented the simulation model “SWUM” <strong>and</strong> its<br />
implementation software “Swumsuit” <strong>in</strong> BMS-2006, major extensions<br />
have been successively made on SWUM, such as optimiz<strong>in</strong>g calculation,<br />
musculoskeletal simulation, <strong>and</strong> multi agent/object simulation, <strong>in</strong> order<br />
to extend its capability of analysis. In this paper, these three extensions<br />
are expla<strong>in</strong>ed <strong>and</strong> the various recent results from their implementation<br />
presented. The usefulness of the extensions was confirmed s<strong>in</strong>ce many<br />
reasonable results were obta<strong>in</strong>ed.<br />
Key words: Biomechanical Simulation, Optimization, Musculoskeletal<br />
model, SWUM<br />
IntroductIon<br />
There are many biomechanical problems to be solved <strong>in</strong> human swimm<strong>in</strong>g.<br />
In order to discuss such problems quantitatively, numerical<br />
simulation is becom<strong>in</strong>g a powerful <strong>and</strong> useful tool. The authors have<br />
developed a simulation model, “SWUM,” (SWimm<strong>in</strong>g hUman Model)<br />
(Nakashima et al., 2007b) <strong>and</strong> a free software, “Swumsuit,” as the implementation<br />
of SWUM (Nakashima, 2005, 2006). By SWUM, it is possible<br />
to analyze the dynamics of the whole swimmer’s body with a short<br />
computation time due to model<strong>in</strong>g the fluid force act<strong>in</strong>g on the swimmer.<br />
S<strong>in</strong>ce it was reported <strong>in</strong> the last symposium (Nakashima 2006),<br />
major extensions have been successively made on SWUM, such as optimiz<strong>in</strong>g<br />
calculation, musculoskeletal simulation, <strong>and</strong> multi agent/object<br />
simulation, <strong>in</strong> order to extend the capability of analysis. In this paper,<br />
these extensions are expla<strong>in</strong>ed <strong>and</strong> the various recent results by them are<br />
presented <strong>in</strong> order to exam<strong>in</strong>e their usefulness.<br />
Methods<br />
All analyses <strong>in</strong> this paper were carried out us<strong>in</strong>g SWUM. It was designed<br />
to solve the six degrees-of-freedom absolute movement of the whole<br />
swimmer’s body as a s<strong>in</strong>gle rigid body by the time <strong>in</strong>tegration method, us<strong>in</strong>g<br />
the <strong>in</strong>puts of the swimmer’s body geometry <strong>and</strong> relative jo<strong>in</strong>t motion.<br />
The swimm<strong>in</strong>g speed, roll, pitch <strong>and</strong> yaw motions, propulsive efficiency,<br />
jo<strong>in</strong>t torques <strong>and</strong> so on, are computed as the output data. The swimmer’s<br />
body is represented by a series of 21 rigid body segments. Each body segment<br />
is represented by a truncated elliptic cone. The unsteady fluid force<br />
<strong>and</strong> gravitational force are taken <strong>in</strong>to account as the external forces act<strong>in</strong>g<br />
on the whole body. The unsteady fluid force is assumed to be the sum<br />
of the <strong>in</strong>ertial force due to the added mass of the fluid, normal <strong>and</strong> tangential<br />
drag forces <strong>and</strong> buoyancy. These components are also assumed to<br />
be computable, without solv<strong>in</strong>g the flow, from the local position, velocity,<br />
acceleration, direction, angular velocity <strong>and</strong> angular acceleration for each<br />
part of the swimmer’s body at each time step. The coefficients <strong>in</strong> this fluid<br />
force model were identified us<strong>in</strong>g the results of an experiment with a limb<br />
model <strong>and</strong> measurements of the drag act<strong>in</strong>g on swimmers tak<strong>in</strong>g a glide<br />
position <strong>in</strong> the previous studies (Nakashima et al., 2007b). For the simulation<br />
example of six beat crawl stroke <strong>in</strong> the previous study, the swimm<strong>in</strong>g<br />
speed of the simulation became a reasonable value, <strong>in</strong>dicat<strong>in</strong>g the validity<br />
of the simulation model. With respect to the six beat crawl stroke, the authors<br />
have already analyzed contributions of each fluid force component<br />
<strong>and</strong> of each body part to the thrust, effect of the flutter kick, estimation of<br />
the active drag, roll motion, <strong>and</strong> propulsive efficiency (Nakashima, 2007a).<br />
Analyses of the other three strokes <strong>and</strong> comparison among four strokes