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Biomechanics of Musculoskeletal System andIts Biomimetic Implications: A Review
Article in Journal of Bionic Engineering · April 2014
Impact Factor: 1.63 · DOI: 10.1016/S1672-6529(14)60033-0
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Corresponding author: Lei RenE-mail: [email protected]
Journal of Bionic Engineering 11 (2014) 159–175
Biomechanics of Musculoskeletal System and Its Biomimetic
Implications: A Review
Lei Ren1,2
, Zhihui Qian2, Luquan Ren
2
1. School of Mechanical, Aerospace and Civil Engineering , University of Manchester , Manchester M 13 9 PL, UK
2. Key Laboratory of Bionic Engineering ( Ministry of Education, China), Jilin University, Changchun 130022, P . R. China
Abstract
Biological musculoskeletal system (MSK), composed of numerous bones, cartilages, skeletal muscles, tendons, ligaments
etc., provides form, support, movement and stability for human or animal body. As the result of million years of selection and
evolution, the biological MSK evolves to be a nearly perfect mechanical mechanism to support and transport the human or
animal body, and would provide enormously rich resources to inspire engineers to innovate new technology and methodology todevelop robots and mechanisms as effective and economical as the biological systems. This paper provides a general review of
the current status of musculoskeletal biomechanics studies using both experimental and computational methods. This includes
the use of the latest three-dimensional motion analysis systems, various medical imaging modalities, and also the advanced
rigid-body and continuum mechanics musculoskeletal modelling techniques. Afterwards, several representative biomimetic
studies based on ideas and concepts inspired from the structures and biomechanical functions of the biological MSK are dis-
cussed. Finally, the major challenges and also the future research directions in musculoskeletal biomechanics and its biomimetic
studies are proposed.
Keywords: musculoskeletal system, biomechanics, multi-scale, biomimetics, biologically inspired robots and mechanisms
Copyright © 2014, Jilin University. Published by Elsevier Limited and Science Press. All rights reserved.
doi: 10.1016/S1672-6529(14)60033-0
1 Introduction
A musculoskeletal system (MSK) is a biological
system composed of bones, cartilages, skeletal muscles,
tendons, ligaments and other connective tissues (see
Fig. 1). The major function of the MSK is to provide
form, support, movement and stability for the human or
animal body. The MSK can be roughly considered to
have two constituent sub-systems: the skeletal system
and the muscular system.
The skeletal system consists of all the bones in the body and also the connecting tissues, e. g . cartilages and
ligaments. The skeletal system provides the fundamental
framework for body shape and load bearing, and also
protects internal organs, e. g . brain, heart, lungs and liver
etc., from external impacts. In the skeletal system, bones
are connected to each other by joints, which provide
articulations in MSK. The most common type of joint is
synovial joint, which consists of fibrous connective
tissue capsule (ligaments) and the periosteum of the
connecting bones lubricated by synovial fluid inside of
the joint.
The muscular system is the prime mover of human
or animal body. For humans, there are approximately
Fig. 1 The musculoskeletal system of human body[1].
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Journal of Bionic Engineering (2014) Vol.11 No.2 160
over 430 skeletal muscle groups accounting for up to
40% of body weight[2]
. The skeletal muscles are made up
of hundreds, or even thousands of muscle fibers, which
range in thickness from approximately 10 μm to 100 μm
and in length from about 1 cm to 30 cm[2]
. Skeletal
muscles are also arranged in layers over the bones, and
they are normally attached to bones through tendons so
that the forces generated by the contractile elements of
the muscle fibers can drive body motions.
As the result of million years of selection and evo-
lution, the biological MSK evolves to be a highly effi-
cient and economic mechanical mechanism to support
and transport the human or animal body with many ex-
traordinary characteristics compared to their man-made
counterparts. For example, cheetah is known as the
fastest living land quadrupedal animal, which can reach
to a speed of 29 m·s−1[3]
. Some special features of chee-
tahs’ MSK have been reported probably contributing to
attaining such a high speed. For example, their divergent
talar ridges may help to avoid limb interference in the
aerial phase of galloping. Their long hindlimb bones
may potentially assist them in making large stride length.
Moreover, their particularly large psoas muscles may
help them to rapidly protract the hindlimbs and also to
resist pitching moments around the hip during acceler-
ating[4]. Another example is horses, a representativeathletic ungulate land animal with excellent locomotor
capacity. Their third metacarpus bone has a small hole
where blood vessels enter the bone[5]
. As common
knowledge from mechanical engineering, holes nor-
mally weaken structures by increasing dramatically the
stresses near the holes as a result of stress concentration[5]
(see Fig. 2). However, the holes at the third metacarpus
bones of horses do not appear to cause bone fractures
even for racing horses. This is probably due to an in-
creased compliance near the foramen[5]
. The sharp dis-
continuity in geometry due to the hole is softened by an
embedded compliant region[5]
. A reinforcing ring with
increased stiffness, together with the ring of lamellar
bone along the foramen’s inner edges, might help to
reduce the possibility of cracking[5]
. The special con-
figuration of the hole helps to move the highest stresses
away from the foramen to regions with higher material
strength[5]
(see Fig. 2).
The human foot complex is another good example
of highly efficient mechanical mechanism from the
biological world. The human foot is a complicated
structure comprising numerous bones, muscles, tendons,
ligaments, synovial joints and other tissues. It has been
found recently that such a small body component de-
livers multiple critical biomechanical functions in at-
tenuating ground impact, supporting body against grav-
ity, maintaining locomotor stability, generating and
transmitting propulsive power during locomotion[6–8]
.
The fascinating structure and characteristics of the
biological MSK, which has been optimally selected after
million years’ evolution, would provide enormously rich
resources to inspire engineers to innovate new technol-
ogy and methodology to develop mechanisms and ma-chineries as effective and economical as the biological
systems. For example, legged locomotion, as a biologi-
cal transportation solution over rough terrain, has been
attracting intensive researches from mechanical engi-
neering and robotics field[9–13]
. This may greatly facili-
tate the development of legged robots with high agility,
stability and energy efficiency.
Δ =1 . 5 MP a
Fig. 2 The foramen in horse third metacarpus bone and its stress analysis[5].
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Ren et al .: Biomechanics of Musculoskeletal System and Its Biomimetic Implications: A Review 161
This paper starts with a brief introduction of the
MSK and the biomechanics of its constituent compo-
nents. Afterwards, a general review of the current status
of the MSK biomechanics, including both experimental
and computational studies, is provided. Several repre-sentative biomimetic examples based on inspired ideas
from MSK biomechanics are discussed. Finally, the
major challenges and also the future research directions
in MSK biomechanics and its biomimetic studies are
proposed.
2 Experimental studies of MSK biomechanics
2.1 Motion capture
In the past decades, motion capture technique has
been increasingly used in recording the two-dimensional
(2D) or three-dimensional (3D) human/animal motion,
which is characterized by the time histories of segmental
or joint angles. Generally, optoelectronic motion analy-
sis systems are employed by using infrared camera ar-
rays to track the positions of active or passive markers
placed on the body segments of interest[14–22]
(see Fig. 3).
Although the optoelectronic motion capture technique
has now been widely used in human/animal movement
studies, the collected data normally suffer from some
technical problems, e. g . skin artifact (due to the relative
movement of skin mounted markers with respect to the
underlying bones)[16,23–25]
, light reflections and marker
occlusions[26]
. Markerless motion tracking method based
on computer vision provides a new promising motion
capture technique[27]
. Currently, the markerless systems
can work with large, obvious movements, while the
measure of more subtle movements still remains chal-
lenging.
To complement the motion capture, many biome-
chanics labs are also equipped with force sensing de-
vices to record the simultaneous kinematic and kinetic
data associated with human/animal motions. 3D force platforms are normally used to measure the ground re-
action forces and moments induced by human/animal
motions. Integrated with the simultaneous motion data,
joint kinetic analysis can normally be conducted by
using the inverse dynamics method[17,28–30]
. Additionally,
pressure plates are often employed to record the foot
pressure distribution during human/animal motions[31 – 34]
.
In addition to multi-camera systems, portable motion
sensors are also used to capture human/animal body
motions, e. g . inertia sensors (i.e. accelerometers, gyro-
scopes etc.) and magnetometers etc.[35 – 38]
. This offers an
alternative way to measure the human/animal motions
outdoors without the constraints of the indoor equip-
ments[39,40]
.
2.2 Surface electromyography
Human or animal electromyography signals at dif-
ferent motor activities can be recorded using invasive or
non-invasive methods. Surface electromyography
(sEMG) is a non-invasive technique widely used for
detecting and recording muscle electrical activity that
occurs during muscle contraction and relaxation cycles
by using surface electrodes. The sEMG signal is nor-
mally used in musculoskeletal biomechanics studies as
an indicator of the initiation of muscle activation, as an
estimator of the force produced by a contracting muscle,
or as an index of the fatigue occurring within a mus-
cle[28,41,42]
. In other words, sEMG signals may contain
information about whether a muscle is active or not, if a
muscle is more or less active, when it is on and/or off,
and also if it fatigues[43]
. However, raw sEMG data maycontain mixed electrical signals from multiple muscles
nearby the electrodes and/or noisy signals due to
movement artifact, so dedicated signal processing is
normally needed before useful information can be ob-
tained to interpret the muscle functions[28,44,45]
.
2.3 Medical imaging
Medical imaging domains, e. g . Computed Tomo-
graphy (CT), Magnetic Resonance Imaging (MRI), ul-
trasound, are very useful techniques to examine theanatomy, geometry and structure of a MSK. Among
Head
Humerus
Forearm+hand
Thigh
Shank
Foot
Pelvis
gr F gr
gl
gl F
X
Y
Z
Torso
Fig. 3 The three-dimensional whole body model with 13 seg-ments and 12 connecting joints. A specially designed marker
cluster system mounted on plastic plates was used to capture thesegmental motions[17].
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Journal of Bionic Engineering (2014) Vol.11 No.2 162
them, the ultrasound provides an economic noninvasive
imaging technique by transmitting high-frequency
sound waves through a body part. As a handy diagnostic
tool, ultrasound has been widely employed in muscu-
loskeletal biomechanics studies to investigate the in vivo
muscle structure, muscle fiber movement, neuromus-
cular disorders etc.[46 – 49]
. Although superficial muscles
may be easily detected by ultrasound probes, it is diffi-
cult to identify individual small muscles when multiple
muscle groups are involved[50]
. Additionally, due to the
reflection or absorption of sound by superficial tissue
layers, it is still challenging for ultrasound to detect
deeper muscles especially in the pelvic region or around
the trunk. Since ultrasound has difficulty in penetrating
bones, to examine the structure of bones, or a particular
musculoskeletal complex, e. g . certain joints or body
segments, other imaging modalities, such as CT and/or
MRI, are generally used.
3 Biomechanical MSK modelling
3.1 Rigid body modelling of MSK
Rigid body dynamics is typically used to simulate
human/animal motions by considering the body seg-
ments of interest as rigid bodies without any deforma-
tions. Over the past decades, numerous rigid body
models have been developed to simulate human/animalmovements or motions of particular body parts with
varying complexity from simple one-segment model
with 1 DOF to complex model with 10 segments and 23
DOFs[17,51 – 66]
(see Fig. 4). In those models, the con-
necting joints are typically defined as frictionless
ball-and-socket joints, hinge joints or universal joints.
Whilst the mechanical behaviour of muscles was nor-
mally represented using Hill-type models[56,66,67]
, where
the normalized muscle force of the contractile element is
the product of three independent experimentally meas-
ured factors describing the force-length property, the
force-velocity property and the dynamics of neural ac-
tivation[56,57]
. Model simulations can be applied in two
different ways, which are usually referred to as the
forward (direct) dynamics method, and the inverse dy-
namics method. In the forward dynamics method, the
motions of the segments are determined by integrating
the equations of motion based on predefined joint mo-
ment or muscle force/activation data[53,61,65,66,68,69]
. In the
inverse dynamics method, the joint forces and moments
are determined based on the measured joint or segment
motion data[17,28–30,66]
.
Biomechanical analysis based on rigid body models
can be applied to a wide range of problems, such as the
assessment of the effect of tendon transfer surgeries[69 – 71]
,
the investigation of multi-segment interaction[72,73]
, the
musculoskeletal performance during walking and
jumping[65,68,74 – 76]
, the development of neural prosthe-
ses[77]
, the neural control principles of movement[78 – 80]
,
the effect of musculotendon loss or damage on theoverall joint moment capacity
[81], and the effect of load
carriage design on walking performance[82]
. Recently,
several software packages have been developed for rigid
body musculoskeletal model construction, simulation
and analysis, e. g . SIMM[69]
, OpenSim[83]
, AnyBody[84]
,
MSMS[77]
etc., which normally provide graphical user
interface for general users.
Despite the recent great progress and success, there
are still some major unsolved problems in rigid body
musculoskeletal modelling. Firstly, the anatomical jointsare typically simplified as ideal ball-and-socket or hinge
joints to reduce computational load, which are not real-
istic representations of most biological joints. In addi-
tion, there are still a large amount of works needed to
improve the in vivo representation of musculotendon
mechanics and neural dynamics, especially on a sub-
ject-specific basis. Finally, the development of predic-
tive musculoskeletal models, which are capable of pre-
dicting kinematic and kinetic variables during motions
with minimal measurement inputs, still remains as a very
challenging task [61,66,85]
.Fig. 4 A large-scale musculoskeletal model with 23 generalizedDoFs and 54 musculotendon actuators[61].
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3.2 Continuum mechanics modelling of MSK
Over the past decades, methods based on contin-
uum mechanics, e. g . Finite Element (FE) method,
boundary element method etc., have been increasingly
used to investigate the mechanical behaviour of mus-culoskeletal structures by considering constituent com-
ponents as deformable bodies. The FE method is a very
useful numerical tool to handle biological structures
normally with highly non-linear material properties,
irregular geometries and complicated boundary condi-
tions. Recently, the FE method has been widely used in
biomechanical studies of MSK, covering a broad range
of topics, e. g . functions of musculoskeletal complexes,
mechanics of joints and skeletal muscle mechanics etc.
3.2.1 FE modelling of musculoskeletal complexes
The FE method has been particularly useful to in-
vestigate the mechanical behaviour of specific muscu-
loskeletal complexes of the human body, normally
comprising numerous bones, joints and soft tissues, e. g .
the spinal column or the ankle-foot complex. Substantial
FE studies have been conducted on the biomechanics of
cervical vertebrae, thoracic vertebrae and lumbar verte-
brae. Some earliest works involves the modelling of the
cervical spine and the lumbar vertebral motions[86 – 90]
.
Saito et al . constructed a spine model to analyze the
prevention of spinal column deformity with oversimpli-
fied representation of vertebral geometry and the in-
ter-vertebral joints, which may lead to an unrealistic
assessment of load sharing and stress distributions[91]
.
The model may be suitable for the study of gross re-
sponses of the whole column rather than the local
changes at the individual vertebrae level. Kleinberger
presented a sophisticated model including head and
various spinal components for FE analysis[92]
. However,
the model lacked sound representations of the anatomi-cal structure of the spine probably because the major aim
of the study was for crash impact analyses rather than
medical applications. The three-segment lower cervical
spinal unit model constructed by Voo et al . had a rea-
sonable representation of the cervical anatomy based on
CT scans and cryomicrotome anatomical sections[93,94]
,
which could be extended to the construction of the entire
cervical column. Most of the FE studies of spinal col-
umn are based on static analysis[95 – 97]
. Although internal
stresses, strains and other biomechanical responses un-der complex loading conditions could be predicted, they
provide very little information about the in vivo condi-
tion of the whole column during dynamic motions.
Whereas some FE models consisting of a series of
connected vertebrae could predict the dynamic re-
sponses of the spine to external loads
[98,99]
. Zhang et al .constructed a detailed cervical spine model (C0-C7)
[100].
The predicted biomechanical response of human neck
under physiological loadings, near vertex drop impact
and rear-end impact conditions, were analyzed and
compared with published measurement data, demon-
strating potential for future biomedical and traumatic
studies.
The human foot is a very complex structure com-
prising numerous bones, joints and soft tissues, deliver-
ing a variety of biomechanical functions during human
motions. Over the past decades, a large number of studies
based on FE method have been conducted to investigate
the biomechanical functions of the foot complex. Lem-
mon et al . used a 2D FE model to study the effect of
insoles on therapeutic footwear based on quasi-static
simulations[101]
. Patil et al .[102]
conducted a stress distri-
bution study on normal and neuropathic feet during gait
using a 2D model, which was constructed from a lateral
X-ray image. Wu[103]
constructed a 2D FE model to study
the foot bone and muscle stresses resulting from plantar
fasciotomy and major plantar ligament injuries. Chu et
al .[104]
conducted a static parametric analysis using an
asymmetric 3D FE foot model to investigate the an-
kle-foot orthosis effects by considering the foot complex
as a single segment. Jacob et al .[105]
developed a 3D FE
model with the purpose being to investigate the contrib-
uting factors to disintegration of tarsal bones in Hansen’s
disease and diabetes. Gefen et al .[106]
constructed a sub-
ject-specific 3D foot model based on realistic bone ge-
ometry to investigate the biomechanical foot function
during gait. The stress distribution analysis was con-ducted at six representative instants of time during gait.
Gefen[107,108]
also developed a 2D FE model to investi-
gate the foot biomechanics following surgical plantar
fascia release and also to evaluate the plantar stress dis-
tribution of a standing diabetic foot. Cheung et al .[109– 111]
developed a more complicated 3D foot model by using
realistic bone geometry and nonlinear material properties.
The model was used to investigate the effects of plantar
fascia stiffness and Achilles tendon loading, and also to
conduct the parametric design using different structuraland material properties of a foot orthosis. Recently, the
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Journal of Bionic Engineering (2014) Vol.11 No.2 164
foot plantar fascia mechanics, stress concentration in
plantar soft tissues and also the load transfer mechanism
were analyzed using different 3D FE foot models[112 – 116]
.
However, it is noteworthy that almost all these studies are
static or quasi-static in nature. So far, very few foot
biomechanics studies used dynamic FE analysis. Dai et
al .[117]
used a 3D foot model to investigate the effect of
sock wearing on the plantar pressure under different
contact conditions from the foot-flat to the push-off
during the stance phase of gait based on dynamic FE
simulations. However, constant loads were assumed and
extra constraints were used to define the model, which
may lead to unrealistic motion of the foot complex. Very
recently, a fully dynamic foot model without any extra
constraints has been developed to simulate the dynamic
behaviour of the human foot structure during stance
phase of walking, which has demonstrated some advan-
tages over the traditional static or quasi-static FE mod-
els[118]
(see Fig. 5).
3.2.2 FE modelling of musculoskeletal joints
The FE method has also been extensively used to
investigate the joint mechanics, especially the contact
stress and strain responses of different joint components.
Brown and Digioia[119]
used a 2D FE model to analyze
the articular contact at hip joint, by representing the
cartilage using non-linear contact elements. An
axis-symmetric FE model of meniscus was proposed
with non-linear material properties, and the simulation
results suggested high radial strains in the regions where
lesions were most often observed[120]
. Eckstein[121]
used
the FE model to analyze the stress distribution at elbow
joint, and found that incongruity generates advantageous
mechanical stimuli in the joint tissues. The FE method
was also applied to the shoulder mechanism by using
truss, hinge and surface elements to construct the
model[122]
. Sophisticated FE models of the knee joint
were also reported to study the meniscus and the contact
condition between cartilage and meniscus[123 – 125]
. In
addition to cartilages, ligaments are also important
components of a musculoskeletal joint. Usually, 1D
element was employed to represent ligaments in FE
modelling of joints. The 1D representation requires only
few parameters to define the mechanical behaviour. This
approach was proved useful for predicting joint kine-
matics under the application of external loads[126]
. But it
has some shortcomings: (1) non-uniform 3D stresses and
strains cannot be predicted; (2) multiple sets of pa-
rameters and initial tensions routinely produce nearly
identical predictions of joint kinematics[127]
. Ligaments
t = 0 (s) t = 0.03 (s) t = 0.08 (s)
t = 0.27 (s)t = 0.23 (s)t = 0.19 (s)
t = 0.40 (s) t = 0.43 (s)
t = 0.45 (s)t = 0.44 (s)
Fig. 5 The von Mises stress distribution predicted by a dynamic finite element foot model at 10 representative instants oftime over the whole stance phase of human walking [118].
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Ren et al .: Biomechanics of Musculoskeletal System and Its Biomimetic Implications: A Review 165
are subjected to highly non-uniform deformations in vivo
that result from a combination of tension, shear, bending,
and compression[128,129]
, and the regional contribution of
a ligament to joint stability changes with joint orienta-
tion
[130,131]
. Therefore, 3D FE modelling is desirable torepresent these mechanical characteristics
[132–134]. The
FE modelling of musculoskeletal joints offers a useful
tool to predict the spatial and temporal variations in joint
contact stresses and strains, which are difficult or im-
possible to obtain experimentally.
3.2.3 FE modelling of skeletal muscles
As the prime mover of the MSK, skeletal muscles
demonstrate very complicated mechanical properties
coupled with neural excitations and muscle fibre con-
tractions[135,136]
. Currently, most of the mathematical
representations of muscle contraction mechanics are
based on either Hill’s model or Huxley’s theory[137 – 140]
.
Hill’s model depicts the dynamics of a musculotendon
unit using a set of connected discrete mechanical ele-
ments. This could help stimulate some initial schemes
toward a simple FE model of skeletal muscles[141]
.
Some initial works on FE modelling of skeletal
muscles involved the representation of muscle-tendon
complex using a number of simple active 1D line ele-
ments, each of which is composed of motor and vis-
coelastic elements. Since the 1D line elements did not
have volumes and masses, the information about muscle
tissue stresses and inertia effects could not be obtained.
Moreover, the muscle moment arms were assumed to be
equivalent for all fibres within a muscle compartment.
This limits the ability of the model to accurately repre-
sent the actual paths of muscles with complex geometry
and also the stress response of the active part and passive
part individually. A 3D FE muscle model has the poten-
tial to represent the complex muscular structures andimprove our understanding of the musculotendon me-
chanics[58]
. Since a skeletal muscle consists of contrac-
tile muscle fibres arranged within a passive matrix of
connective tissues[142]
, a number of FE models have been
developed to describe the active behaviours of skeletal
muscles. Tsui et al .[143]
constructed a 3D active FE
muscle model by using a user-defined muscle behaviour.
The simulation results of isometric force-length rela-
tionship and force-shortening contraction demonstrated
the potential of the model for studying muscle damageand fatigue. Tang et al .
[140] developed a 3D FE model of
skeletal muscles by integrating a modified Hill’s muscle
model with a muscle fatigue formula, but neglected the
different fibre types inside of the muscle. Based on the
two-state Huxley model, Oomens et al .[144]
constructed a
3D muscle model to estimate the inhomogeneous straindistribution in a skeletal muscle. A good agreement
between the measurement data and the simulation result
showed the proposed model could be employed as a tool
for studies on damage and adaptation of skeletal muscles.
Different from the mechanical properties during active
conditions, the passive muscle behaviour was normally
represented by non-linear hyperelastic or viscoelastic
constitutive relationship in the FE modelling of the
skeletal muscle[140,145,146]
(see Fig. 6).
Due to the highly anisotropic, nonlinear material
property, and also the complex geometry (multiple layers
of soft tissue) and boundary conditions, 3D FE modelling
of stress-strain behaviour of skeletal muscles is normally
complicated and computationally demanding. The tradi-
tional solutions for FE simulations based on standard
Extended
Flexed
Fig. 6 The reconstructed 3D muscle models of gluteus maximus,
gluteus medius, iliacus, psoas by segmentation of MR images[146].
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Journal of Bionic Engineering (2014) Vol.11 No.2 166
non-linear FE formulations are time-consuming even for
one or two muscles[147]
. Blemker et al .[148]
developed a
quasi-static invertible FE algorithm to reduce the com-
putational load, which provided two major improve-
ments over the traditional methods: (1) elements are
allowed to invert by computing robust FE forces with a
invertible framework; (2) the stiffness matrix is positive
semi-definite.
Nowadays, mathematical models representing the
mechanical behaviours for muscle-tendon complexes
used for studying the dynamics of the human MSK are
dominated by various Hill-type models[149 – 151]
. The de-
velopment of bio-realistic and computationally efficient
FE models of the muscular system for assessing the
dynamic functions of biological MSK is still at its very
early stage.
4 Biomimetic studies inspired by MSK bio-
mechanics
4.1 Bioinspired quadrupedal robot - BigDog
BigDog is a dynamically stable quadrupedal robot
developed by Boston Dynamics[152]
, with aim being to
provide load carriage service to accompany soldiers in
harsh rough terrains, which are impossible for conven-
tional vehicles with wheels or treads. The size of the
robot is of a large dog or a small mule, about 1.1 m long
and 1 m tall, and weighs 109 kg. The robot has four legs
that are articulated like a typical quadrupedal animal,
with compliant elements to absorb shock and store en-
ergy during moving. It is capable of performing a variety
of locomotion behaviours, such as walking, running,
climbing, jumping and carrying heavy loads in
rough-terrain conditions[152]
.
Ideas and concepts inspired from quadrupedal
animals have been used in the structure and actuation
design, sensor and motion control of the BigDog robot.The single leg structure, in terms of joint configuration,
standing posture and actuator position, is very similar to
the leg of a typical quadrupedal animal (see Fig. 7).
Going distally from hip joint to metatarsal joint, the leg
actuation of a typical quadrupedal animal becomes less
strong, and contains more compliance. In addition, the
forelimb and hindlimb configuration of the BigDog uses
similar design principle of the four-legged configuration
in horses, dogs and goats[153,154]
. As the compliant
components of animals’ MSK play important role duringdynamic moving, such as running, jumping and gallop-
ing[155]
, spring components are integrated into the leg of
the BigDog to attenuate the ground impact during dy-
namic moving (see Fig. 7). When moving on the ground,
the joint position, joint force, ground contact, ground
load and external obstacles of the robot are monitored by
using onboard sensors to ensure its dynamic balance and
stability. The robot could also behave like quadrupedal
animals to adapt to the local terrain variation by adjust-
ing its body height and attitude, and also foot placements.
Based on those bio-inspired ideas and concepts, the
BigDog exhibits excellent locomotion performance, e. g .
it can climb slopes up to 35 degrees, walk across rubbles,
climb muddy hiking trails, walk in snow and water etc.
So, the BigDog has been considered as one of the most
advanced quadrupedal robots moving on rough ter-
rains[152]
.
4.2 Efficient human-like robot with compliant legs
Over the past decades, many bipedal robots
have been developed to mimic human locomo-
tion[10,12,13,156 – 163]
. Most of those walkers used precise
control to regulate the angle values of each individual joint at each instant of time during locomotion. This
requires actuators with high precision and frequency
response, a precise environment model and also high
energy cost[10,12,13]
. Recently, the concept of passive
dynamic waking, which needs less actuators and active
control than mainstream robots, was proposed as a new
design and control paradigm[159 – 162,164]
. It has been
demonstrated that periodic stable walking can be
achieved with high energy efficiency and little control
by integrating simple actuations into passive dynamicwalkers
[160].
Fig. 7 The bio-inspired back leg of the BigDog robot compared
to the hindlimb of a typical quadrupedal animal[152].
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Ren et al .: Biomechanics of Musculoskeletal System and Its Biomimetic Implications: A Review 167
A recently developed bipedal robot based on the
passive dynamic walking concept, used minimum con-
trol to drive two elastic legs inspired from the structure
of the human leg MSK [164]
. The robot consists of seven
body segments, two servomotors at the hip joints, four passive joints at knee and ankle joints, and totally eight
linear springs (see Fig. 8). The spring components were
used to mimic the passive mechanical function of the
major musculotendon units in human legs. A unique
feature of the robot is that it has six springs spanning
over two joints to mimic the major biarticular muscles in
the leg. The experimental study showed that this
bio-inspired bipedal robot could produce human-like
walking gait by using extremely simple control without
sensory feedback [165]
. This is a good example for de-
velopment of bipedal robots with higher energy effi-
ciency and more natural walking pattern based on ideas
inspired from the biological structure of the MSK.
Hip motor
Springs
Passive joints
Rubber
(a) (b)
(c)
Fig. 8 The human-like bipedal robot with compliant legs[165]. (a)
bipedal robot model, only one leg is shown; (b) schematic of therobot design; (c) the physical robot platform.
5 Challenges and future directions
The last decade has seen great progress and ad-
vance in the human/animal movement studies, which
aim for understanding the biomechanical functions ofthe biological MSK using both experimental and com-
putational approaches. However, due to the great com-
plexity of the biological MSK, there still remain many
unsolved problems and grand challenges in muscu-
loskeletal biomechanics. Skin artefact has been the ma-
jor barrier for 3D motion analysis systems to become a
useful clinical diagnostic tool. X-ray based video sys-
tems (e. g . fluoroscopic systems) may be helpful to re-
duce the skin artefact during motion capture[166 – 168]
, but
the effect of radiation and the limited measuring volume
prevent it from being useful in general cases. Assess-
ment of individual muscle forces in vivo during hu-
man/animal motions has been proven to be a grand
challenge in musculoskeletal biomechanics field[169 – 171]
.
Due to the limitation of the current measuring tech-
niques and ethical reasons, the direct measurement of the
in vivo musculotendon forces is almost impossible. So,
rigid body musculoskeletal modelling technique is
normally used together with optimisation algorithms to
estimate the muscle forces that can reproduce measured
joint motions. However, the determination of the sub-
ject-specific muscle parameters, musculoskeletal ge-
ometry and the rigorous experimental validation of the
calculated results still remain big challenges[172]
. In ad-
dition, development of predictive musculoskeletal
models, which are capable of predicting body kinemat-
ics and kinetics during various movements with mini-
mum measurement inputs[61,66,85]
, will be one of the
major future research directions due to their great po-
tential in clinical diagnosis, rehabilitation engineering
and surgical planning.In musculoskeletal biomechanics studies, compu-
tational FE modelling provides a unique tool to assess
the internal stress/strain conditions of the biological
MSK, which is normally not measurable in vivo. Prop-
erly conducted FE studies could help to investigate the
fundamental biomechanical mechanisms of the MSK, to
improve our understanding of the associated muscu-
loskeletal disorders, and hence to provide sound scien-
tific basis to facilitate clinical diagnosis and surgical
treatments. One of the challenging works in FE model-
ling of MSK is to provide accurate definitions of the in
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Journal of Bionic Engineering (2014) Vol.11 No.2 168
vivo material properties of the soft tissues and hard tis-
sues in MSK. For example, the definition of the consti-
tutive equation of cancellous bones is still a subject of
debate, in particular those relating to post-elastic be-
haviour [173 – 175]
, and the failure criteria[176,177]
. Similarly,
there are also lacks of accurate definitions for the in vivo
material properties for the soft tissues (e. g . cartilages,
ligaments, tendons and muscles etc.).
Another challenging work in FE modelling of MSK
is to provide bio-realistic representations of the anatomy,
structure and function of the human MSK at different
levels/scales (e. g . organ level, tissue level and cell level).
As we know, mechanical loadings at macro level have
effect on behaviours at micro level, conversely me-
chanical properties at micro level influence system re-
sponses at macro level[178]. For example, diabetic foot
ulceration may have a biomechanical etiology[179]
. For
patients with diabetes, some common daily activities,
e. g . walking, may be harmful because diabetes may
affect the biological functions of MSK at various levels.
Dysfunctions at different levels manifest themselves in
terms of loss of sensation[180]
, changes in control of
movement[181]
, and alteration of tissues[182]
and also cell
properties[183]
. It is unclear how do mechanical loads at
macro level (e. g . ground reaction forces) response to
cellular deformations that may cause cell damage oreven ulceration. Mechanical loadings at macro level (e. g .
increased foot contact pressures), redistribution of stress
due to changes in tissue composition (e. g . muscular
atrophy[184]
, cell distribution within tissues, increased
mechanical loading of cells or their decreased damage
resistance may all have contributions to the development
of ulceration. Therefore, a multi-scale modelling
framework is needed to identify the pathways to cell
damage from the mechanical loadings at organ level
through to the deformations at cell level.Multi-scale modelling has been used in basic sci-
ence and engineering areas e. g . mathematics, material
science, chemistry and fluid dynamics etc. for many
years. When applied to MSK biomechanics, the
multi-scale modelling approach is normally based on an
integrated hierarchical structure at multiple body levels,
where the mechanical outputs of macro level models are
transmitted to micro level models with detailed repre-
sentations of MSK at tissue and cell level[185]
. Normally,
rigid body dynamics is used to simulate the mechanical
behaviour of MSK at body level, and continuum me-
chanics is employed to represent the stress-strain inter-
play at organ level, whereas for simulations at tissue and
cell levels specialized algorithms and solvers are nor-
mally needed[178,185]
. Therefore, multi-scale MSK
simulations are computationally intensive, and require
intricate representations and also effective simulation
strategies/approaches to describe the complex interac-
tions among multiple levels.
After multi-scale MSK simulations are conducted
to address specific research problems or particular
clinical questions, the next challenging stage is to in-
terpret and validate the simulation results. It is a very
daunting and time consuming task to interpret the com-
plicated calculation outcomes obtained or to extract
clinically meaningful information from the huge amount
of database generated by the multi-scale simulations.
Moreover, the lack of in vivo subject-specific data (e. g .
muscle forces, mechanical properties of hard and soft
tissues etc.) and the complexity associated with ex-
perimental measurements make the validation of the
simulation results even more challenging[178]
. Although
parameter sensitivity studies coupled with statistical
populations of in vivo and primarily in vitro data may
provide some initial verifications, the limitation of the
current measuring techniques make a thorough sub-
ject-specific in vivo validation impossible. Furthermore,the highly demanding nature of clinical problems need
the future multi-scale MSK models to be easy-to-use,
robust and also with timely solutions.
It is evident that, for multi-scale modelling of hu-
man/animal MSK, from its solution formulation to ex-
perimental validation and clinical application, the in-
herent challenges are hard to be handled based on the
current capacity of experimental and computational
biomechanics. To tackle them effectively, some syner-
getic efforts are necessary not only by coordinating allworks involved in a coherent way, but also by increasing
and encouraging the level of resources sharing and ex-
change in biomechanics community, e. g . data and model
sharing (including those developed by commercial
software packages and self-coded models), format
standardization, and dissemination of solution databases
with model distribution.
Acknowledgements
This work was supported by the International
Cooperation Project of National Natural Science
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Ren et al .: Biomechanics of Musculoskeletal System and Its Biomimetic Implications: A Review 169
Foundation of China (No. 50920105504), the UK En-
gineering and Physical Sciences Research Council Grant
(No. EP/I033602/1), the Project of National Natural
Science Foundation of China (No. 51105167) and the
scientific and technological development planning pro- ject of Jilin Province, China (No. 20130522187JH).
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