The effect of shock absorbing sports surfaces in jumping
Juan V. Durá
Instituto de Biomecánica de Valencia
Abstract A
jumping movement is performed over five different sports surfaces within a wide
range of shock absorbency. The sports surfaces tested have an influence in performance
and in the accelerations measured on people. The subjects tested changed their
movements and adaptation to the surface has been observed. The surfaces with high
shock absorbency (more than 70% shock absorbency) do not improve protection significantly
and reduce performance in the jumping movement. Keywords Sports
Surfaces, Shock Absorption, Jumping Introduction The
shock absorbing property and the compliance of sports surfaces have been related
with injuries and performance in sports. It seems that there is an opposite relation
between the necessity to damp impacts to avoid injuries and performance in sports.
But some authors have shown the possibility of finding an optimal point for compliance
in sports surfaces (MacMahon 1979, Bosco 1985). There
are different techniques to measure the sports surface behaviour under impacts.
One of the easiest methods is to drop a weight with an attached accelerometer.
This technique may not be appropriate since it does not simulate the impact that
a sportsman could produce in jumping or running. Additionally, the results depend
on the weight dropped and the contact surface (Nigg 1987, Francis 1988, Maki 1990).
Nowadays,
one of the commonest standard test methods for multipurpose indoor surfaces is
DIN18032-2 (DIN 1991). This standard uses the "Artificial Berlin Athlete" machine
(Figure 1) to simulate the impacts that a person weighing 80-90 kg would produce
in a vertical jump. The Artificial Berlin Athlete has been accepted by the IAAF
and other international sports organisations to be the best practical solution
for measuring the shock absorbing property of the sports surfaces.
 | Figure 1: Artificial Berlin Athlete The
DIN method consists of measuring the maximum impact force over the sports surface
and calculating the force reduction percentage in comparison to a very rigid surface,
such as concrete. For
simulating the behaviour of people, the "Berlin Artificial Athlete" has a calibrated
spring. The purpose of the spring is to produce an impact similar to the impact
that a person would cause when jumping and falling on his or her feet, by increasing
the time of impact with the hip, knee and ankle flexion movements.
The
problem is to know how good is the simulation of a person’s behaviour and
to decide what the limits for a good or bad surface are regarding shock absorbency.
The
DIN18032-2 standard requirements are 51% of force reduction for ‘pointelastic’
surfaces and 53% for ‘areaelastic’ surfaces in multipurpose indoor
surfaces. Some elite sportsmen think that this shock absorption is excessive since
performance is highly reduced. FIBA (International Basketball Federation), for
example, recommends 40% for basketball courts. Although
footwear could be as important as the surface in shock absorption, the general
opinion is that a minimum of shock absorbency is necessary to assure comfort and
reduce overuse injuries in sports. The aim of this study is to find the relation
between the shock absorbing property of surfaces, measured with the DIN method,
the performance and the impacts in jumping movements. Methods Five
different surfaces were selected and tested according to DIN18032-2. The surfaces
are within a wide shock absorbency range, from 0 to 75% (Table 1).
Table
1: Surfaces tested | SURFACE | DIN FORCE REDUCTION PERCENTAGE |
DESCRIPTION | |
A |
0.0% | Rigid terrazzo pavement |
| B |
19.0% | Synthetic surface (PVC). 4 mm thick |
| C |
44.0% | Synthetic surface (Synthetic rubber). 16 mm
thick | |
D |
62.3% | Wood surface, beech parquet with crossbeams
and elastics pads | |
E |
75.1% | Synthetic surface. PVC top layer 4mm and a PU
base layer 70mm thick | Five
healthy young persons, non-elite sportsmen, were selected with the following characteristics:
|
|
from
17 to 24 years | |
|
from
64 to 69.5 kg | |
|
from
1.75 to 1.82 m | |
|
42
(French scale) | The
movement (Figure 2) consists in falling from a 42 cm high bench onto the surface.
They were asked to jump as high as possible after the first contact with the surface
and to keep their arms crossed on their chest. With the arms in this position
the variability of movement performance is reduced, since arm movement could help
to obtain more or less height by movement synchronisation.
| Figure 2: Movement and accelerometer position. Before
starting the measurements the subjects performed several jumps in order to adapt
their movements to the surface. The movement was then repeated 5 times on each
surface. There were 25 repetitions (5 persons by 5 times) on each sports surface.
The
test subjects wore the same sports shoes, since the objective was to find the
effect of the surface. If the worn shoes had been different, variability would
have increased and perhaps the effect of surface would have been hidden.
Two
extensometric accelerometers were attached to the subjects: one to the lower limb
and another to the forehead. The lower limb placement was chosen to be the proximal
anterior part of the tibia, 3-4 cm under the tibial tuberosity in the internal
part. The
accelerometer specifications are: - Forehead:
Range 20 g, resonance frequency 1200 Hz, sensitivity 2.1 mV/g, weight 0.3 grams.
- Lower
limb: Range 50 g, resonance frequency 1200 Hz, sensitivity 1.0 mV/g, weight 0.3
grams.
The accelerometers were attached to the skin by a
double sided adhesive tape and an aluminium support. The weight of the system
was less than 2.5 grams. An elastic bandage wrapped tightly around the shank and
forehead was used to fasten the accelerometer and to preload the skin (Figure
2). A
contact sensor was placed into the shoe sole for measuring the time that the subject
was on the surface and in the air. These times were used as a measurement of performance.
The
signals from the accelerometers and shoe sensor were acquired with a personal
computer with an A/D board. The sample frequency was 6000Hz (2000Hz per channel).
Eight
reflective markers were attached to define four segments (two for each segment)
and the movements were recorded in a KINESCAN-IBV video system at 50 Hz with one
camera. A 2D movement analysis was done, and the flexo-extension angles of the
hip, knee and ankle were calculated. The decision to do only a 2D analysis was
based on the opinion that in the jumping movement the flexo-extension movement
is the most relevant and the angles in other planes are not so important (Sussman
1988). The
subjects were recorded in standing position and the angles of the joints calculated.
The joint angles in standing position were used as the origin of the measure (0
degrees). Temporal
and kinematic parameters were obtained, and with each of these parameters a multifactor
analysis of variance of repeated measures was performed. Subject and surface were
considered as factors. A multiple range test of Least Squares Differences (LSD)
at 95% was used for post hoc analysis to determine on which surfaces the differences
were significant. The
temporal parameters studied were:
| tfloor | time that the person is in contact with the
floor between the first and the second impact. |
| tair | time that the person is in the air between the
first and the second impact. | The
kinematic parameters studied were:
 | maximum forehead acceleration in the first impact. |
 | maximum shank acceleration in the first impact. |
 | maximum ankle flexion. |
 | maximum knee flexion. |
 | maximum hip flexion. |
Results The
results obtained for the different parameters with regard to the surface factor
are shown in Table 2. The P value that appears in the table is for the surface
factor. The sports surface factor was always significative.
Table
2: Results of multifactor variance analysis *
The interaction surface-subject has been significant
| | | | SPORTS SURFACE |
| PARAMETER | P value | ERROR | A | B | C | D | E | | tfloor (s) | 0.000 | ± 0.006 | 0.387 | 0.427 | 0.390 | 0.413 | 0.434 | | tair (s) | 0.000 | ± 0.003 | 0.566 | 0.566 | 0.562 | 0.574 | 0.545 | (g) | 0.000 | ± 0.07 | 3.39 | 3.02 | 3.24 | 2.96 | 2.87 | (g) | 0.040 | ± 1.43 | 15.99 | 13.07 | 18.55 | 15.35 | 12.97 | * (º) | 0.000 | ± 0.34 | 29.71 | 29.25 | 29.01 | 34.84 | 26.50 | * (º) | 0.000 | ± 0.90 | 92.61 | 92.22 | 89.03 | 84.23 | 94.06 | * (º) | 0.000 | ± 1.02 | 90.47 | 94.28 | 89.18 | 98.40 | 93.47 | The
results of multiple range tests of Least Squares Differences (LSD) at 95% are
shown in Table 3.
Table
3 Homogenous groups. LSD method at 95%
| | A | B | C | D | E | | tfloor (s) | 1 | 2,3 | 1 | 2 | 3 | (s) | 12 | 1,2 | 1 | 3 | 1 | (g) | 2 | 2 | 2 | 1 | 1 | (g) | 1,2 | 1 | 2 | 1,2 | 1 | * (º) | 2 | 2 | 2 | 3 | 1 | * (º) | 2 | 2 | 2 | 1 | 3 | * (º) | 1 | 2 | 1 | 3 | 2 | The
multiple range tests classify the surfaces in homogeneous groups in function of
the parameter value. The numbers indicate the groups. Two numbers appear when
a surface could be classified in two different groups. For example, surface A
belongs to group 1 in the case of parameter, and surface B can belong to group
2 or group 3. Number 1 groups the surfaces with the minimum parameter value. Group
3 includes the maximum parameter values. Figures 4, 5, 6 and 7 show these results.
The
homogeneous groups for accelerations are shown in Figure 3. In the case of forehead
acceleration ( ), surfaces A and
C showed the greatest values, and surfaces B, and E the lowest. The highest value
of shank acceleration ( ) appeared on C surface. B and E showed the
lowest values. A and D showed intermediate values.
 |
Figure 3: Means and 95.0 LSD intervals for accelerations Although
the surfaces are very different according to the DIN 18032 test method, the differences
in accelerations do not permit to classify surfaces in more than two groups. The
low and high absorbing surfaces are mixed in the groups. The separates the surfaces in two groups: low (A,
B, C) and high (E, D) absorbing. The
homogeneous groups for times are shown in Figure 4. Time differences between surfaces
are bigger than those in accelerations. In this case it is possible to classify
surfaces in three groups. But the groups do not classify the surfaces in function
of the shock absorbing property measured by the DIN18032 test method.
 |
Figure 4: Means and 95.0 LSD intervals for times The
time that the subjects remain on the floor is higher when shock absorption increases,
except in the case of surface B (Figure 4 left).
 |  |
| Figure 5: Means and 95.0 LSD intervals for Knee flexion angle
| Figure 6: Means and 95.0 LSD intervals for ankle flexion angle
| | | Figure 7: Means and 95.0 LSD intervals for hip flexion angle
| The
time that the subjects remain in the air is more or less alike for surfaces A,
B and C. The three surfaces belong to the same group. It is slightly longer for
surface D and clearly shorter for surface E (Figure 4 right).
The
homogeneous groups for angles are shown in Figures 5, 6 and 7. Angle differences
between surfaces are bigger than acceleration differences and it is possible to
classify surfaces in three groups. But the groups do not classify the surfaces
in function of the shock absorbing property measured by the DIN18032 test method.
Surface
D shows the highest ankle and hip flexion, and the lowest knee flexion. Although
surface E is the most shock absorbent, it shows the highest knee flexion.
Discussion The
maximum acceleration could be interpreted as a measurement of the protection against
possible overuse injuries and the time values as a measurement of jump performance.
If contact time with the floor is low, the sportsmen need less time to perform
repeated jumps. If time in air is high, the jump is higher. These times could
be important in sports like basketball or volleyball. The
results show that surface E (with shock absorption of 75%) does not increase the
protection in comparison with other surfaces with less shock absorbency and reduces
jump performance. For surface E tfloor
is high and is low.
The
maximum jump performance,
high, appears for surface D (shock absorption of 65%) and it is coincident with
the minimum knee flexion angle, the maximum hip flexion angle and the maximum
ankle flexion angle. This surface also shows a low tfloor. When
tfloor is low, accelerations are higher.
The impact energy absorbed by the athlete body causes more acceleration if the
energy is dissipated in less time. Although
the interaction subject-surface is significant for the angle parameters, the tendency
observed in the five subjects is similar. Anyway in future research more subjects
are necessary because interaction could have influenced in the results obtained.
The
subjects perform more knee flexion on the surfaces with low shock absorption and
in the surface with very high shock absorption (E surface). In the case of low
shock absorption the reason could be the need of using the knee joint for reducing
impact levels. In the case of the E surface it is necessary to find another explanation.
One reason could be that the subjects remain more time over the E surface because
the surface deformation is longer along time. Then the elastic energy stored in
the muscles cannot be recovered in an elastic fashionand they need to flex more
the knee. More studies are necessary to confirm this hypothesis.
Discrepancies
have been found between surface B and C. Surface C shows higher impacts on the
leg than surface B, although it is more shock absorbent. But shock absorbency
has been measured using the force reduction percentage parameter used in DIN18032-2,
and this parameter does not consider other energy aspects that could explain this
different behaviour. Conclusions Different
shock absorbency levels create changes in joint flexion to maintain impacts (accelerations)
in acceptable levels. The athlete tries to adapt his or her movements to maintain
protection (impact levels) and performance (jump height) in surfaces with different
shock absorbing properties. This
adaptation is visible in the changes of flexion angles for the knee, hip and ankle.
When the surface is more rigid, knee flexion is higher to maintain impacts (accelerations)
in acceptable levels. As the objective of the movement studied was to jump as
high as possible, the changes in knee angles caused changes in the other joints
(ankle and hip) to maximise the jump height. But this tendency changes when shock
absorbency is very high (more than 70%). Very shock absorbing surfaces suffer
higher deformations for more time. Then the elastic energy stored in the muscles
cannot be recovered in an elastic fashion and they need to flex the knee
more. More studies are necessary to confirm this hypothesis.
The
results seem to show the need of fixing a shock absorbency limit for force reduction
parameter at about 70%, although it is necessary to validate it with studies with
other type of test subjects. The results with heavier people, such as elite basketball
players, could be different. Besides, other parameters, like absorbed energy,
should be considered in measuring deformation and force at the same time.
Acknowledgements This
work was supported by the Spanish Interministry Commission for Science and Technology
(Reference Number SAF94-0518) and JUNCKERS INDUSTRIER A/S.
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