The effect of normal load force and roughness on the dynamic traction developed at the shoe–surface interface in tennis
James Clarke
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1
Sharon J. Dixon
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Loic Damm
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Matt J. Carre
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S. J. Dixon L. Damm Exeter Biomechanics Research Team, University of Exeter
, St Lukes Campus, Heavitree Road, Exeter EX1 2LU,
UK
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J. Clarke M. J. Carre (&) Department of Mechanical Engineering, The University of Sheffield
, Mappin Street, Sheffield S1 3JD,
UK
During tennis-specific movements, such as accelerating and side stepping, the dynamic traction provided by the shoe-surface combination plays an important role in the injury risk and performance of the player. Acrylic hard court tennis surfaces have been reported to have increased injury occurrence, partly caused by increased traction that developed at the shoe-surface interface. Often mechanical test methods used for the testing and categorisation of playing surfaces do not tend to simulate loads occurring during participation on the surface, and thus are unlikely to predict the human response to the surface. A traction testing device, discussed in this paper, has been used to mechanically measure the dynamic traction force between the shoe and the surface under a range of normal loading conditions that are relevant to reallife play. Acrylic hard court tennis surfaces generally have a rough surface topography, due to their sand and acrylic paint mixed top coating. Surface micro-roughness will influence the friction mechanisms present during viscoelastic contacts, as found in footwear-surface interactions. This paper aims to further understand the influence microroughness and normal force has on the dynamic traction that develops at the shoe-surface interface on acrylic hard court tennis surfaces. The micro-roughness and traction of a controlled set of acrylic hard court tennis surfaces have been measured. The relationships between micro-roughness, normal force, and traction force are discussed.
1 Introduction
During tennis-specific movements the traction provided by
a shoesurface combination will influence a players injury
risk and performance [1, 2]. Excessive friction acting
between shoe and surface (referred elsewhere in this paper
as traction) can lead to injury caused by overloading in the
lower extremities [3]. Insufficient static traction can lead to
a slip (unwanted movement of the shoe relative to the
surface), which will result in a loss of performance or, if
the slip is severe, lead to a fall which may cause injury
itself [4]. Also, a player may choose to purposefully
perform a controlled slide on a tennis surface; a type of
movement that is common for clay surfaces, but is
becoming increasingly common at elite level on hard
courts as well. The success of this type of movement will
depend on the dynamic traction developed at the shoe
surface interface (the force acting to slow down a shoe
moving relative to the surface). The tractional properties of
a shoesurface combination must therefore be within an
optimal range [5].
Elite tennis is played on grass, clay and acrylic hard
court surfaces. Nigg [6] reported clay surfaces to have
traction/friction coefficients (ratio of horizontal traction
force and normal force) of between 0.5 and 0.7, whereas
the other surfaces tested had traction/friction coefficients
between 0.8 and 1.2. Clay surfaces have generally been
reported to have a lower occurrence of injury than acrylic
hard court surfaces [610]. The difference in injury
occurrence between surfaces has been partly attributed to
the inherent differing styles of play on each surface caused
by differences in ball speed and bounce [6]. However, the
differing tractional characteristics of the playing surfaces
also affect the risk of accidental injury occurrence [11].
This has lead to the hypothesis that surfaces which do not
allow sliding increase the potential to cause injury.
Despite the understanding that shoesurface traction can
influence performance and injury risk there remains a
requirement for improved understanding of the tribological
interactions at the shoesurface interface in sport [12]. The
aim of this paper is to present experimental data and further
investigate the influence the applied normal force and
surface roughness have on the dynamic traction developed
on acrylic hard court tennis surfaces. Understanding the
mechanisms of dynamic traction will aid the improvement
of playing surfaces and footwear constructions. Once
traction mechanisms are understood, surface properties
and/or footwear can be effectively changed to maximise
performance and/or minimise injury risk.
The dynamic traction force will be dependent on the
friction mechanisms developed between the footwear and
the playing surface. Acrylic hard court tennis surfaces are
constructed with a top coating of acrylic paint and silica
sand mixture. This gives acrylic hard court surfaces a rough
surface topography in comparison to other hard surface/
flooring systems. The roughness of acrylic hard courts will
be dependent on the paintsilicasand mixture which has
been reported to differ between surface manufacturers [13,
14]. Viscoelastic rubbers are generally used on the outsoles
of tennis shoes. In clean, dry conditions, sliding contacts
between viscoelastic rubbers and a hard solid substrate will
result in a combination of the following friction
mechanisms: adhesion and hysteresis [1518]. During
interactions where the shoe slides relative to the surface, the
micro-roughness of the surface will undoubtedly affect the
dynamic traction force developed.
During a horizontal sliding event the asperities of the
solid substrate will cause cyclic elastic deformation of the
viscoelastic rubber material. Internal damping causes
energy dissipation during the loading and unloading cycle
[16, 17, 19]. This loss is the hysteretic component of the
contributing friction mechanisms. If local stresses deform
the rubber beyond its elastic limit, it will be unable to
recover. This results in tearing of the material and leads to
additional friction forces at the interface between rubber
and surface. Tearing can result in wear and cause the
separation of fragments of material from the rubber, this is
termed abrasive wear.
Adhesion is the process of junctions forming, due to van
der Waals interaction, between the contacting surfaces and
the arising friction force is the force required for the
junctions to shear [1622]. Adhesion friction is more
prevalent when rubber slides over a smooth surface and
depends significantly on asperity contact and therefore the
loading conditions and the roughness characteristics of the
surface the rubber is sliding relative to. On increasingly
rough surfaces the contribution of the adhesive component
of traction has been found to decrease due to reduced
asperity contact [18, 20, 22].
Asperity contact is also dependent on the normal loading
applied during the dynamic sliding event [16, 22]. Figure 1
(adapted from [22]) illustrates how as the amplitude of the
surface roughness is decreased, under the same normal
loading conditions, surface contact will (...truncated)