Content uploaded by Keisuke Kobayashi Yamakawa
Author content
All content in this area was uploaded by Keisuke Kobayashi Yamakawa on Sep 24, 2018
Content may be subject to copyright.
NextPublishing Sample
Three-dimensional analysis of hip and knee joint movements during dolphin kicking and butterfly swimming 1
Three-dimensional analysis of hip and knee joint
movements during dolphin kicking and butterfly
swimming
Keisuke Kobayashi YAMAKAWA, Japan Women’s College of Physical Education, Tokyo, Japan
Hideki TAKAGI, University of Tsukuba, Ibaraki, Japan
Yasuo SENGOKU, University of Tsukuba, Ibaraki, Japan
Abstract̶The aims of this study were to clarify differences
in hip and knee joint movements during dolphin kick alone
and during butterfly stroke swimming, and to investigate which
parameter relates to swimming performance in each stroke.
Eight male swimmers performed three trials using dolphin kick
with a kick board (BD), underwater dolphin kick (UD), and but-
terfly swimming (Fly) at 80% maximal effort in a water flume.
Three-dimensional coordinates of the swimmers during the tri-
als were obtained using a motion capture system, and these
coordinates were used to calculate the horizontal velocity of
the hip (Vhip), the hip and knee joint angle, and the angular ve-
locity. Butterfly kicking motion was divided into first kick (Fly-
1st) and second kick (Fly-2nd) according to the stroke phase,
and the kinematic parameters during the 4 different kicks were
used for analysis. As the main results, it was indicated that the
peak hip flexion angle during Fly-2nd was significantly smaller
than that during BD and UD (BD, -27.8 ±9.7 deg; UD, -27.7
±10.5 deg; Fly-1st, -25.6 ±13.9 deg; Fly-2nd, -16.2 ±7.0
deg, p <.05) and the peak knee extension angle during Fly-
2nd was significantly smaller than that during BD, UD, and
Fly-1st (BD, -7.6 ±5.8 deg; UD, -4.4 ±5.7 deg; Fly-1st, -
7.4 ±4.9 deg; Fly-2nd, 2.0 ±6.6 deg, p <.05). The mean
Vhip during BD was significantly correlated with the peak hip
external rotation angle (r= -0.77), the peak knee extension
angle (r= -0.77), the peak hip external rotation angular veloc-
ity (r= -0.88) and the peak knee flexion angular velocity (r=
0.81). The mean Vhip during UD was significantly correlated
with the peak knee extension angle (r= -0.87), the peak hip
external rotation angular velocity (r= -0.73) and the peak knee
flexion angular velocity (r= 0.95). The mean Vhip during Fly
was not correlated with any of the kinematic parameters dur-
ing Fly-1st and Fly-2nd. Our results demonstrate that flexion/
extension movements of the hip and knee joint are different
between dolphin kick and butterfly swimming. Furthermore,
larger knee extension, greater hip external rotation velocity,
and greater knee flexion velocity may be important to increase
dolphin kick performance.
Key words: Swimming performance; Motion capture system;
Water flume
1. Introduction
Dolphin kicks are used in butterfly swimming, and gen-
erally swimmers perform two dolphin kicks during each
butterfly stroke cycle. According to Maglischo (2003),
The downbeat of the first kick takes place during the en-
try and catch of the arms, and the downbeat of the second
kick occurs during the upsweep if the underwater arm-
stroke. A previous study indicated differences in hip and
knee joint movements between the two dolphin kicks in
each stroke cycle (Barthels & Adrian, 1971). Therefore,
swimmers and coaches should be aware of the kine-
matic differences during the practice of dolphin kicks in
the butterfly stroke. However, that previous study inves-
tigated the sagittal movement only, and did not analyze
the coronal or cross-sectional movement. Thus to ob-
tain deeper understanding of the butterfly dolphin kick
technique, a three-dimensional analysis method should
be used.
On the other hand, there are many kinematic stud-
ies examining the underwater dolphin kick compared to
studies examining the dolphin kick used during butter-
fly swimming. While a previous study investigated the
kinematic difference in lower limb movements between
dolphin kicks when swimming with a board and butterfly
swimming (Barthels & Adrian, 1971) it remains unclear
whether there is a kinematic difference between move-
ments during the underwater dolphin kick and those
during the dolphin kick in butterfly swimming.
The purpose of this study was to clarify kinematic
differences in lower limb movements between dolphin
kicks when swimming with a board, underwater dolphin
kicks and during butterfly stroke swimming. Further-
more, to describe the characteristics related to swimming
performance, we investigated parameters that correlate
with swimming velocity in each stroke.
2. Methods
2.1. Participants
Eight male collegiate swimmers participated in this
study (age, 21.3 ±0.7 years; height, 1.73 ±0.05 m;
weight, 70.3 ±4.6 kg). All participants practiced 8
NextPublishing Sample
2
times each week with a collegiate swimming team. The
participants were fully informed of the risks, benefits,
and stresses of the study, and their informed consent was
obtained.
2.2. Swim trials
In a 50 m indoor pool, the participants performed three
25 m swimming trials: dolphin kick swimming with
board (BD), underwater dolphin kick swimming (UD),
and butterfly swimming (Fly). The participants were
instructed to execute each trial at maximal effort with
a push-off start. In the underwater dolphin kick swim-
ming, the participants swam approximately 1.0 m under
the water surface to exclude the effect of wave drag (Lyt-
tle, Blanksby, Elliott, & Lloyd, 2000). The swim-times
during the trials were measured using a manual stop
watch by the same examiner, and the average swimming
velocity between 15 m to 25 m were defined as the max-
imum swimming velocity (100%V) in each trial.
For analysis of the three-dimensional motion, the
participants performed BD, UD, and Fly in a water flume
(Igarashi Industrial Works Co. Ltd.). The flow velocity
during each trial was set at 80% velocity of 100%V. The
participants executed 10 stroke cycles during each trial.
2.3. Three-dimensional motion analysis
Three-dimensional motion analysis was conducted using
a motion capture system (VENUS 3D, Nobby tech Inc.).
As Figure 1, twenty cameras filmed swimmers above
the water flume or through the underwater window. For
measurement of lower limb motion, 15 landmark points
(left styloid process of ulna, lowest ribs, anterior superior
iliac spines, hip greater trochanters, lateral condyles of
the femur, medial condyles of the femur, lateral malle-
oli of the fibula, and medial malleoli of the tibia) on
the participants were marked with LED markers, and
the landmark points coordinates were used for analysis.
The right and left center of hip joint coordinates were
estimated from the anterior superior iliac spine coordi-
nates and the hip greater trochanter coordinates. The
right and left center of the knee joint coordinates were
estimated as the mid point between the lateral condyles
of the femur coordinates and the medial condyles of the
femur coordinates.
Figure 1. Experimental setting.
2.4. Calculation of kinematic parameters and joint
angles
In the present study, we defined one kick cycle as be-
ginning at the vertical highest peak of the left lateral
malleolus position and ending at the next vertical high-
est peak. Furthermore, one kick cycle was divided into
a downward kick (DK) phase and an upward kick (UK)
phase. We defined one butterfly stroke cycle as begin-
ning at left wrist entry and ending at the next left wrist
entry, and further, the one butterfly stroke cycle was
divided into five phases (entry and stretch, out-sweep,
in-sweep, up-sweep, and release and recovery) using the
trajectory of wrist coordinates according to Maglischo
(2003). The two dolphin kicks in each butterfly stroke
were separated into the first dolphin kick (Fly-1st) and
the second dolphin kick (Fly-2nd) corresponding to the
stroke phases. We defined that the DK of the first kick
takes place during the entry and catch of the arms, and
the DK of the second kick occurs during the upsweep.
Kick frequency (KF) was defined as the reciprocal of the
duration of one kick cycle. Kick amplitude (KA) was
defined as the vertical distance between the highest verti-
cal left lateral malleolus position and lowest vertical left
lateral malleolus position during one kick cycle. Swim-
ming velocity was defined as the horizontal velocity at
the mid-point between both centers of the hip joints, and
an average swimming velocity during one kick cycle
(Vhip) was estimated as swimming performance.
Hip and knee joint angles were calculated with
Cardan angles using MATLAB software (Math works
Inc.), whereby rotations about orthogonal local axes de-
NextPublishing Sample
Three-dimensional analysis of hip and knee joint movements during dolphin kicking and butterfly swimming 3
rived from swimmer’s body corresponding to flexion/
extension in the sagittal plane, adduction/abduction in
the coronal plane and internal/external rotation in the
cross-sectional plane, respectively. In the present study,
only the knee flexion/extension angle was used for anal-
ysis due to the joint movement of the knee in the coronal
and cross-sectional plane being small. From the joint
angle data, peak angle, range of motion (ROM), and
peak angular velocity were calculated for analysis. Con-
sidering the cyclic variation of the dolphin kicks, three
values were obtained for all kinematic variables, and the
mean of these values was used for statistical analysis.
2.5. Statistical analysis
All data are reported as the mean and standard devia-
tion (mean ±SD). Statistical analyses were conducted
using Bell Curve for Excel (SSRI Inc., Japan). All vari-
ables were compared between the 4 dolphin kicks using
repeated one-way ANOVA, followed by Sidak’s mul-
tiple comparison post-hoc tests. Furthermore, the re-
lationships between the swimming performance (Vhip)
and kinematic parameters was investigated using Pear-
son’s correlation coefficient. The threshold values of the
correlation coefficient that represented small, moderate,
large, very large, and nearly perfect correlations were
0.1, 0.3, 0.5, 0.7, and 0.9 according to recommenda-
tions in the literature (Hopkins, Marshall, Batterham, &
Hanin, 2009). The statistical significance level was set
at 5% in this study.
3. Results
The kinematic parameters of each dolphin kick are
shown in Table 1. There was a significant main ef-
fect for the Vhip, KF, KA, DK phase, and UK phase (all
p<.05). The time-course change of hip and knee joint
angles during one kick cycle in each kick is shown in
Figure 2. The results of peak angles, ROM, and peak
angular velocities are shown in Table 2. There was a sig-
nificant main effect for peak hip extension angle, peak
hip flexion angle, ROM of hip flexion-extension, peak
hip external rotation angle, peak knee extension angle,
ROM of knee flexion-extension, peak hip extension an-
gular velocity, peak hip flexion angular velocity, and
peak knee extension angular velocity (all p<.05).
The mean Vhip during BD correlated significantly
with the peak hip external rotation angle (r= -0.77),
the peak knee extension angle (r= -0.77), the peak hip
external rotation angular velocity (r= -0.88), and the
peak knee flexion angular velocity (r= 0.81). The mean
Vhip during UD correlated significantly with the peak
knee extension angle (r= -0.87), the peak hip external
rotation angular velocity (r= -0.73), and the peak knee
flexion angular velocity (r= 0.95). The mean Vhip dur-
ing Fly did not correlate significantly with any kinematic
parameter during Fly-1st and Fly-2nd.
Table 1. Kinematic parameters during each kick cycle.
4. Discussion
The purpose of this study was to clarify kinematic dif-
ferences in lower limb movements between dolphin kick
swimming with board, underwater dolphin kick and but-
terfly stroke swimming. Our results showed that the peak
hip flexion angle and the peak knee extension angle in
Fly-2ndwere significantly smaller than in the other 3
dolphin kicks. In contrast, there were no significant dif-
ferences in the peak hip adduction/abduction angle and
angular velocity, and in hip internal/external rotation
angle and angular velocity.
Barthels and Adrian (1971) used electrogoniometry
to analyze the hip and knee joint movements during dol-
phin kicks with a board and the butterfly stroke, and
they suggested that alternating major and minor kicks
occurred either temporally, spatially, or both temporally
and spatially in all subjects during butterfly swimming
trials. In the present study, the peak hip flexion angle
in Fly-2nd was significantly smaller than that in Fly-1st
(Table 2) while there was no significant difference in
KF between Fly-1st and Fly-2nd. Therefore, it was sug-
gested that the results in this study were different from the
previous study. Maglischo (2003) noted that the down-
beat of the second kick is generally shorter with less
hip flexion than the first kick. This may be explained
in the light of the findings of Sanders, Cappaert, and
Devlin (1995). Using Fourier analysis, they established
that the motion of elite butterfly swimmers is character-
ized by vertical undulations comprising two sinusoidal
body waves- a one beat wave (H1) and a two-beat wave
(H2)., The phase relationship between them causes the
amplitude of the vertical hip motions and the knees and
ankles to differ yielding a strong beat and a weaker beat
NextPublishing Sample
4
Figure 2. Change in hip and knee angles during each kick cycle in a typical subject (BD: Vhip=1.30 m ·s-1, UD: Vhip=1.35
m·s-1, Fly-1st: Vhip=1.21 m ·s-1, Fly-2nd: Vhip=1.53 m ·s-1)
(Sanders, 2007). In contrast, there was no difference
between Fly-1st and Fly-2nd in the variables related to
hip adduction/abduction and hip internal/external rota-
tion (Table 2). Furthermore, it was observed that there
were no major differences in the time-course changes of
hip adduction/abduction angle and hip internal/external
rotation angle. From these results, it was considered
that the hip and knee joint movements in the coronal and
cross-sectional plane during butterfly stroke swimming
were similar with that during dolphin kick swimming.
By investigating the angular characteristics (Table
2), there was no significant difference between the vari-
ables in UD and Fly-1st, while the peak hip extension
angle in UD was slightly smaller than that in Fly-1st. No
differences were observed in the time-course changes in
Figure 2. These results suggest that the hip and knee
joint movements in Fly-1st are similar to the movements
in UD. However, the peak hip extension, the peak hip
flexion angles, the peak knee extension angle, and the
ROM of knee flexion-extension in UD were significantly
different than those in Fly-2nd. These results suggest that
the second kick during the butterfly stroke may require
hip and knee joint movement whichis different from that
of the underwater dolphin kick.
In Fly-1st and Fly-2nd, Vhip showed no significant
correlation with any kinematic variable. The previ-
ous study indicated that the kick in butterfly swimming
produced large accelerations and suggested that more
propulsion comes from the kick than from the arms
(Sanders et al., 1995). From the results of this study,
it was considered that the swimming velocity during
both situations did not relate to the kick parameters di-
rectly because the arm stroke also contributes to the
propulsion. Furthermore, very large correlations be-
tween Vhip and the peak knee flexion angular velocity,
and the peak hip external rotation angular velocity in
both BD and UD were observed. A previous study re-
ported that swimming velocity during underwater dol-
phin kicks correlates to the vertical toe velocity during
the upward kick phase (Atkison, Dickey, Dragunas, &
NextPublishing Sample
Three-dimensional analysis of hip and knee joint movements during dolphin kicking and butterfly swimming 5
Table 2. The peak joint angle, range of motion, and peak angular velocity during each kick cycle.
Nolte, 2014). Therefore, the greater knee flexion angu-
lar velocity may contribute to the greater toe velocity
during the upward kick phase. As shown in Figure 4,
the hip joint rotated internally during the first half of DK
and externally in the last half of DK during each dolphin
kick. These hip internal-external rotational movements
may contribute to control the direction of the dorsal side
of the foot. However, the present study did not investi-
gate foot movement during the dolphin kick. Therefore,
future studies should examine foot movements during
the dolphin kick.
In conclusion, using three-dimensional analysis, it
was confirmed that the hip flexion/extension and knee
flexion movements in the second dolphin kick during
butterfly stroke were different from movements in the
first dolphin kick during the butterfly stroke and the un-
derwater dolphin kick, while there was no difference
in hip adduction-abduction and hip internal-external ro-
NextPublishing Sample
6
tation movements. Therefore, it was considered that
understanding the kinematic difference is important for
coaching and training to improve the dolphin kick tech-
nique during butterfly stroke.
References
Atkison, R. R., Dickey, J. P., Dragunas, A., & Nolte,
V. (2014). Importance of sagittal kick symmetry
for underwater dolphin kick performance. Human
movement science, 33, 298-311.
Barthels, K. M., & Adrian, M. J. (1971). Variability
in the dolphin kick under four conditions. Paper
presented at the First International Symposium on
“Biomechanics in Swimming, Waterpolo and Div-
ing.
Hopkins, W., Marshall, S., Batterham, A., & Hanin, J.
(2009). Progressive statistics for studies in sports
medicine and exercise science. Medicine Science
in Sports Exercise, 41(1), 3-12.
Lyttle, A. D., Blanksby, B. A., Elliott, B. C., & Lloyd,
D. G. (2000). Net forces during tethered simulation
of underwater streamlined gliding and kicking tech-
niques of the freestyle turn. J Sports Sci, 18(10),
801-807. doi:10.1080/026404100419856
Maglischo, E. W. (2003). Swimming fastest: Human
Kinetics.
Sanders, R. (2007). Rock and roll rhythms in swimming.
Paper presented at the ISBS-Conference Proceed-
ings Archive.
Sanders, R. H., Cappaert, J. M., & Devlin, R. K. (1995).
Wave characteristics of butterfly swimming. Jour-
nal of biomechanics, 28(1), 9-16.