PRINCIPLE AND TVVO FORMS OF SWIMMING PROPULSION

Transcrição

PRINCIPLE AND TVVO FORMS OF SWIMMING PROPULSION
PRINCIPLE AND TVVO FORMS OF SWIMMING PROPULSION
Falk Hildebrand, Volker Drenk, Dieter ~ l i c h e '
.Institute for Applied Training Science, Leipzig
1
Olympic Training Centre HamburglKiel, Germany
Propulsion in water is primarily done by generating torque in the shoulder, hip, knee, and
ankle. To do this water resistance is used as support. By the of arm movements the body
is pulled through the water, by the leg movements it is pushed. Locomotion is also found
without any direct backward motion of the water.
KEY WORDS: swimming, propulsion, water resistance, torque
I
!
INTRODUCTION: Analyses of swimming technique cover classical methods of threedimensional (3D) analyses (Deschodt, Rouard, Monteil, 1996) as well as complex studies
including the energy yielding process (Miyashita, 1996).
The swimmers move both in the water and above it: This makes the evaluation of the effect
of the body parts above the water on the remaining body more complicated. But there is a
trend in swimming, caused by a higher flexibility of all parts of the body, that all body parts
actively act on water resistance. Additionally, the swimmers set water as a wave in front of
them in motion.
Several authors have tried to define propulsion. Councilman (1968) described the Newton
principle "actio est reactio" as an impulse transfer from the moving water to the body. This
attitude has been revised ten years later by Schleihauf's studies showing that backward
moving water creates almost no hold for support (Councilman, 1980). He recommended an
S shaped path of the pulling arm. For an explanation the lift force, deduced from the
Bernoulli Principle, was introduced. Schleihauf concluded that both principles (IVewton and
Bernoulli) contribute to propulsion.
Maglischo (1993) again trusts in Newton: "Swimmers must push water back to go forward".
He considered the hydrostatic drag to be of secondary importance. But he introduced a new
idea: If the hand moves linearly the boundary layer flow is disrupted to produce turbulence
instead of laminar water flow.
In contradiction to this approach Colwin (1992) presented his vortex theory taking the water
turbulences into account. In his opinion vortexes create a compact support to prop against
(Fling-Ring-Mechanism). Colwin distinguished between three kinds of vortex: starting vortex,
bound vortex and shed vortex. Hollander and Berger (1997) speculated that propulsion
could be regained only from the water turbulences that are caused by the swimmer's propulsion.
In 1993 Prichard observed the active rolling of the hip in top swimmers. He explained a portion of the propulsion by the impulse generation caused by turning the hip is transferred to
the arms.
METHOD: Data on body motion are gained from video recordings above and under water.
All subjects are elite swimmers. The procedure is described in the paper by Drenk,
Hildebrand, Kindler and Kliche (ISBS 1999).
The calculated 3D coordinates form the basis for our analyses. Especially the velocity of the
centre of gravity is calculated (see lower curve in Figure 1). We try to relate the increase in
velocity to propulsion measures. According to our opinion the propulsion measure can only
be defined by water resistance. Below we will explain how it is possible to move without
impulse transfer, e.g. without moving the water backward. In training, swimming movements
are presented using animation programmes (chosen phases in FiguresI and 2).
ayl aleu!ysa 01 eaJe s!yl uo uo!paJ!p pue anleh A l ~ o l jo
a ~uo!lnqyls!p ayl pue w ~ ayl
e jo
eaJe paueaqsMoy ayl asn a M 'luauow ley1 lsnl u! JaleM ayl 1su!e6e p ~ e ~ y 3 e
6u!hou
q
aJaM a p ayl
~ Molaq
~
wJe ayl 40 syed a y l .ayoJls wJe l~e.13
~UOJ) e 6uunp we.16au!y
s,w~eue sluasa~dz a ~ n 6 ! .uo!paJ!p
j
6u!ww!~sayl 01 a~!soddoJaleM Gu!puelsl~!gsayl
lsu!e6e pahow aJe Apoq ayl jo syed y q y 6u!~np
~
saseyd uo!low ayl pasuape~ey3a M .t
'JaleM U! uo!slndo~d)O S U J O j luaJa))!p
s!sA~euea y l : N O I S S ~ ~ S
aN
I ~v S l i f l S 3 U
Allua~eddeo w u! pallnsaJ elep uo!low
a£ 40
-sa3~0)6uj~eaysou lnq 'sa3~o)IewJou Aluo aJe
aJayI passa~dwo3aq louum y q y JaleM
~
ay!l sp!ny ul puey a y l j o weJ60lalle~eda3~0)ayl
jo asne3aq uo!slndo~du! sso( e sasnw s A e ~ l euo!paJ!p 6u!ww!~sayI ueyl Jaylo uo!paJ!p
uo!low u! a6uey3 e ley$ auyapun Allp!ldxa a M .luawala aueld s!yl uo a3uels!sa~JaleM
JO) aJnseaw se luawala aueld al!u!)u! e )o uo!palo~dAl~olahayI )o a~enbsayl Aldde a M
' ( ~ L z'd ' ~ y a s w ! ~Apoq
~ ) ) a y l j o adeys ayl uo puadap osje ~uap!gao:, 6 e ~ ppue y!l ayl a ~ ! s
pale3!ldwor, aJow uaha aJe suo!l!puor, ayl lna -(uo!pa~!p6u!ww!~s01 ~e(n3!puad~ad)
a3~0)
U!I se -saJ (uo!pa~!p6u!ww!~su!) luauodwo3 uo!slndo~dse pauyap aJe sluauodwo3 asayl
fjney!aly3~) al6ue 6u!y3elle ayl 40 au!s .saJ au!so3 ayl 01 ~euo!yodo~d
lsowle pue Jaylo
y3ea 01 ~e(n3!puad~ad
aJe Aayl 'sa3~oj.saJ sluauodwo3 o m olu! pap!A!p aq 01 sey 6 e ~ p
UJO) uo!paJ!p uo!gow 01 al6ue ue l e 6u!y3elle s! puey ayl ase3 ul .lua6uel luauahour ayl
Aq palea~3aueld ayl 01 ~e(n3!puad~ad
6u!y3eve s A e ~ ( es! puey ayl ley$~ o y a3uayadx3
s
'Aprils s!4 u! leyl
JO) uo!lew~!)uo3e puno) !6eyel .Z ueyl Ja((awsaq plnoys Alpolah uo!low UOJ) A ~ a p u a d a p
s,a3uels!sa~)o ~uauodxaayl ' s n y l 'sa!lpolah ayl)o a~enbsayl 01 leuo!yodo~ds! a3uels!sa~
ayl lase3 s!yl u! uaha 'ley1 punoj aM sa!pnls .In0 ul .A6~aua3!gau!y )o l u a w a 6 u e ~ ~ e a ~
e 6u!snw Apoq ayl pu!yaq saxayoA spu!j auo :pajja olu! awo3 sMel Jaylo A l ~ o l alm!l!~=,
~
u!eya3 t3 Yl!M 6u!yels
JeU!Ut3( t3 01 anp A ~ U OS! y3eo~ddeS!yl ' ( ~ P z'd 'I~~su!JE))
s/U
P'O 01 Z'O )o Al!3o(ah e y l ! eaJe
~
3!lalpenb pasJaww! Alalaldwo3 e JO) 1.1 = 3 01 slunowe
luelsuo3 a3uels!sa~s!yl aldwexa JO j .eaJe leuo!pas-sso~:, pawea~ls-MO~
ayl jo uo!suaw!p
ayl pue UJO) ayl uo 'p!ny 6u!how jo lunowe ayl uo spuadap y 3 ! 4 ~',an(eh a3uels!sa~,ayl
'pa3npo~lu!s! luelsuo3 le3!~!dwaue a3uels1sa~ayl 6u!leln3le3 uayM '('3la loo) 'Japlnoys
'puey) Apoq ayl )o yed pahow ayl jo Alpolah ayl )o a~enbsayl se llaM palew!xo~dde
s! I! JaleM ayl 40 A6~aua3!gau!y aqI 01 S ~ U O ~ S ~ JAlpa~!p
J O ~ 6 e ~ payl a3u!s zaJe leuo!pas
-SSOJ3 paUJt3aJIS-MOl) pue Al!suap JaleM O l leuo!yodo~dS! 6eJp U J O j .,6E?Jp WJOj, pallm S!
a3uels1sa~
s ! y l 'A6~auaalau!y olu! pauJojsueJl s! JauJw!Ms ayl Aq pale~aua6~ J O Mayl a 3 ~ o j
le!yau! ~ U ! W O ~ Aa
J ~ .uo!gow
AO
s'hpoq ayl Aq pahow aJe sa~n~alow
JaleM '6u!ww!~suayM
Ja)aM ay) )su!a6e p ~ a q 3 a q
anow a p ~ aq)
p Molaq svad 'ayo~qs
wa~6au!y- a ~ n 6j!
U J I~ M ~ 6uunp
J ~
z
J O )
~3 jo Aqpolan :Mollaq
alqua uo A)polan jo
~ ~pua
A qqad :anoqa Gu!ww!~s
A~yavnqu! quawanow 6a1- c a~n6!d
integral of that area as a measure for water resistance. Water resistance creates a
support for hands and arms which is applied to generate torque in the shoulder ankle
pulling the trunk forward. It becomes especially obvious in modern breast stroke
swimming with the hands and moving backward arms only for a very short time.
2. When applying this procedure to leg movements in butterfly swimming - the subjects
were swimming underwater and without using their arms - we found evidence for a
second form of propulsion. Especially in skilled swimmers the resistance parameter has
never been positive. Figure 1 shows that all parts of the body are moved against the
flow though the swimmer moves forward (compare velocity curve of centre of gravity).
Our explanation is as follows: Leg movement in butterfly swimming is characterised by an
upward res. downward movement of the lower leg res. of the more or less stretched legs.
Synchronous to that movement pattern we find an increase and decrease of the centre of
gravity's velocity in our animation programme. Velocity vectors are almost constantly
pointing (exception and then only for a short time are foot portions) in the swimming
direction (Figure 1). Thus water is never moved backward, the body is exclusively faced with
resistance.
The resistance which originally is breaking propulsion is applied as support to generate
torque in knee and hip. This makes it possible to stretch the ankles without working in
accordance with the angular momentum conservation law. According to this law a
movement of the centre of gravity with only such movements would be impossible in quasi
airborne conditions. Consequently, the centre of gravity is moved forward by stretching the
knee and hip ankle.
CONCLUSION: The question for real propulsion force values is still insufficiently answered
(compare even Rouard et al.). This will be possible only after having a good procedure to
determine the resistance coefficients.
REFERENCES
Berger, M. & Hollander, P. (1997). Internet Sportsci.org-news-news0709. XI1 FINA World
Congress on Swimming Medicine, Goteborg.
Colwin, C.M. (1992). Swimming into the 2 1st Century. Champain, Illinois: Leisure Press.
Councilman, J.E. (1968). The Science of swimming. Englewood Cliffs, New Jersey: Prentice-Hall.
Councilman, J.E. (1980). Handbuch des Sportschwimmens fiir Trainer, Lehrer und Athleten.
zur schwimmsportlichen Trainings- und Bewegungslehre. Bockenem Harz: Schwimmsport
Fahnemann.
Deschodt, V.J. ,Rouard, A.H. & Monteil, K.M. (1996). Relative displacements of the wrist,
elbow and shoulder. In Biomechanics and medicine in swimming VII (S. 52-58). London: E
& FN Spon.
Grimsehl (1954). Lehrbuch der Physik. In W. Schallreuter (Hrsg.) Mechanik - Warmelehre Akustik, Erster Band. Leipzig: B.G. Teubner.
Maglischo, E.W. (1993). Swimming even faster. Mountain View: Mayfield Publishing Company.
Miyashita, M. (1996). Critical aspects of biomechanics in swimming. In Biomechanics and
medicine in swimming VII (S. 17-22). London: E & FN Spon.
Rouard, A.H., Schleihauf, R.E. & Troup, J.P. (1996). Hand forces and phases in freestyle
stroke. In Biomechanics and medicine in swimming VII (S. 34-44). London: E & FN Spon.
Schleihauf, R.E. (1979). A hydrodynamic analysis of swimmimg propulsion. In Swimming 111,
International Series on Sport Sciences 8, 70-109
Takagi, H. (1997). Internet Sportsci.org-news-news0709. XI1 FINA World Congress on
Swimming Medicine, Goteborg.

Documentos relacionados