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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 />

all particles set <strong>in</strong> motion. Momentum is a vector; the magnitude is the<br />

product of mass (m) times its velocity (v): [m*v] = kgm/s = Ns <strong>and</strong> its<br />

direction co<strong>in</strong>cides with the direction of the velocity.<br />

The momentum approach allows for application of the law of conservation<br />

of momentum (orig<strong>in</strong>al enunciation: René Descartes (1596-<br />

1650). Accord<strong>in</strong>g to this pr<strong>in</strong>ciple the total momentum is constant – provided<br />

a closed system is considered (which is not subject to external<br />

<strong>in</strong>fluence). If two (or more) masses belong to a closed system (Figure<br />

2) <strong>and</strong> one mass changes velocity, simultaneously the other masses will<br />

adapt their momentum (<strong>in</strong> the opposite direction), hence, any <strong>in</strong>teraction<br />

between body <strong>and</strong> surround<strong>in</strong>g water gives a reaction. The actions of<br />

(parts of ) any body <strong>in</strong> aquatic space transmit energy while chang<strong>in</strong>g the<br />

motion of water-mass over a period of time. The simultaneous reaction<br />

has an effect <strong>in</strong> <strong>and</strong> aga<strong>in</strong>st the swimm<strong>in</strong>g direction at the same time. If<br />

<strong>in</strong>creas<strong>in</strong>g speed of a whole body is observed, there will be a zero “nett”<br />

effect <strong>in</strong> swimm<strong>in</strong>g direction.<br />

The pr<strong>in</strong>ciple of momentum claims that if the momentum before<br />

<strong>and</strong> after an <strong>in</strong>teraction of limbs <strong>and</strong> water-mass differs this difference<br />

is <strong>in</strong>duced by the <strong>in</strong>teraction. This concept is elegantly applied to determ<strong>in</strong>e<br />

effects of a “displac<strong>in</strong>g” rigid total body on a flow of constant speed,<br />

either <strong>in</strong> steady or unsteady conditions. Based on the law of conservation<br />

of momentum it is evident that momentum <strong>in</strong> front of the whole<br />

body must be equal to the momentum <strong>in</strong> the wake plus all momentum<br />

changes produced by the <strong>in</strong>teraction between total body <strong>and</strong> particles<strong>in</strong>-motion.<br />

The difference <strong>in</strong> momentum over time <strong>in</strong> steady flow is called<br />

drag or propulsion (Figure 3).<br />

Figure 2 Momentum change due to the total body action of the fish<br />

result<strong>in</strong>g <strong>in</strong> thrust<br />

Jet-propulsion <strong>in</strong> aquatic space: In context with <strong>in</strong>duced water motion<br />

it was po<strong>in</strong>ted out that body actions change the motion of water-mass<br />

due to <strong>in</strong>teraction of the limbs <strong>and</strong> water-mass. The effect of the <strong>in</strong>teraction<br />

of limbs <strong>and</strong> water-mass is a change of momentum. From this it<br />

follows that the change of momentum of particles (m’*v’) are comb<strong>in</strong>ed<br />

with a change of momentum of the total body mass (m’’*v’’), <strong>in</strong> the opposite<br />

direction. From the swimmers view the reaction (m’’*v’’) provides<br />

components <strong>in</strong> <strong>and</strong> aga<strong>in</strong>st the swimm<strong>in</strong>g direction (called drag or<br />

thrust). If the momentum of particles (m’*v’) is totally directed aga<strong>in</strong>st<br />

the swimm<strong>in</strong>g direction of the total body, the reaction results <strong>in</strong> a 100<br />

% effect. Water mov<strong>in</strong>g backwards is thrust<strong>in</strong>g the whole body forward.<br />

However, this does not suggest that one should move the h<strong>and</strong> or leg<br />

backwards to ga<strong>in</strong> an effective thrust. The most effective <strong>and</strong> efficient<br />

way to ga<strong>in</strong> maximum thrust for a given energy-<strong>in</strong>put is a jet-flow, used<br />

by squids or jelly fish (Fig . 3).<br />

Figure 3 Vortex <strong>in</strong>duced jet by a jelly fish<br />

176<br />

Jet-flow is a powerful stream of mass carry<strong>in</strong>g high momentum. Jetpropulsion<br />

exists also <strong>in</strong> the swimm<strong>in</strong>g of the skilled human. Matsuuchi<br />

et al. (2004) published research data for the first time based on the PIVmethod<br />

(Particle Image Velocimetry), demonstrat<strong>in</strong>g the existence of<br />

<strong>in</strong>termittent jet-flow. Close scrut<strong>in</strong>y revealed that first a vortex-r<strong>in</strong>g had<br />

to be produced by the action of the swimmer’s h<strong>and</strong> <strong>and</strong> <strong>in</strong> its wake.<br />

The rotation of the vortex r<strong>in</strong>gs cause a particle drift <strong>in</strong> one direction.<br />

The shape <strong>and</strong> rotation of the vortex r<strong>in</strong>g determ<strong>in</strong>es the jet length-todiameter-ratio<br />

<strong>and</strong> thus the momentum. Hence, the orientation of the<br />

jet-flow relative to swimm<strong>in</strong>g direction determ<strong>in</strong>es the contribution<br />

to thrust<strong>in</strong>g the body.<br />

Figure 4 Vortex-<strong>in</strong>duced jet-flow of a h<strong>and</strong> while swimm<strong>in</strong>g freestyle<br />

dIscussIon<br />

Concentration on the <strong>in</strong>teraction of limbs <strong>and</strong> water-mass <strong>in</strong>stead of<br />

limit<strong>in</strong>g oneself to the mere action of limbs or bodies, augments the<br />

underst<strong>and</strong><strong>in</strong>g of reality. The act of underst<strong>and</strong><strong>in</strong>g is a dynamic process<br />

<strong>and</strong> prone to verification / falsification of theories. The say<strong>in</strong>g, noth<strong>in</strong>g<br />

is more practical than a good theory, is valid when theory mirrors reality.<br />

Sometimes a change <strong>in</strong> theory means that already exist<strong>in</strong>g, but not<br />

established concepts survive; e.g. Berger (1996, 95) found that high propulsive<br />

forces cannot be based solely on lift <strong>and</strong> drag of an act<strong>in</strong>g h<strong>and</strong><br />

<strong>and</strong> concluded “the key to produc<strong>in</strong>g effective propulsion at low energy<br />

cost may be the creation of vortices of a special form”.<br />

The research of jet-flow requires a water-related view of both the<br />

motion of the limbs <strong>and</strong> of the water-<strong>in</strong>-motion <strong>in</strong> aquatic space. Most<br />

of the exist<strong>in</strong>g studies on swimm<strong>in</strong>g use a body related approach focuss<strong>in</strong>g<br />

on the velocity of body actions. In most studies related to swimm<strong>in</strong>g<br />

the underst<strong>and</strong><strong>in</strong>g of the movement of the surround<strong>in</strong>g water is<br />

limited to the lift <strong>and</strong> drag approach, established <strong>in</strong> 1970 by Counsilman.<br />

Already <strong>in</strong> 1986 Counsilman said <strong>in</strong> personal communication: “I<br />

can’t help it if people still refer to my publications of the end of the<br />

sixties”. He was aware that the drag <strong>and</strong> lift approach was not applicable<br />

to an unsteady swimm<strong>in</strong>g situation. In that time the vortex <strong>in</strong>duced<br />

propulsion concept <strong>and</strong> <strong>in</strong>fluence of added mass to swimm<strong>in</strong>g<br />

bodies started to attract the <strong>in</strong>terest of (a few) swimm<strong>in</strong>g researchers.<br />

Ungerechts (1988) published the idea that breaststrokers’ leg actions<br />

lead to rotat<strong>in</strong>g water forms by which “momentum is transferred to the<br />

fluid <strong>and</strong> <strong>in</strong> reaction, its “impulse” accelerates the body.” Van Tilborg et<br />

al. (1988) presented data of “impulses”, measured <strong>in</strong> Ns, result<strong>in</strong>g from<br />

the difference between propulsion <strong>and</strong> resistance for different phases<br />

<strong>in</strong> breaststroke. They po<strong>in</strong>ted out that “impulses are more reliable than<br />

forces”. Ungerechts (1992), calculated momentum needed to change<br />

hip motion (Δv) dur<strong>in</strong>g the arm stroke <strong>in</strong>clud<strong>in</strong>g an <strong>in</strong>ertial term due<br />

to acceleration based on experimental data of eight breaststrokers <strong>and</strong><br />

compared the data with forces due to the h<strong>and</strong>s’ actions. It was shown<br />

that momentum =|16.5 – 45.9| Ns will expla<strong>in</strong> (Δv) = |0.27 – 0.76| m/s<br />

with 93 % confidence. Ungerechts & Klauck (2006) presented the flow<br />

physical laws which are relevant for unsteady flow <strong>in</strong> conjunction with<br />

added mass effects.<br />

A change of paradigm from a body related to a water related view

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