Andrej Olenšek1, Zlatko Matjačić. 1. University Rehabilitation Institute, Republic of Slovenia, Ljubljana, Slovenia. andrej.olensek@mail.ir-rs.si
Abstract
BACKGROUND: In clinical gait assessment, the correct interpretation of gait kinematics and kinetics has a decisive impact on the success of the therapeutic programme. Due to the vast amount of information from which primary anomalies should be identified and separated from secondary compensatory changes, as well as the biomechanical complexity and redundancy of the human locomotion system, this task is considerably challenging and requires the attention of an experienced interdisciplinary team of experts. The ongoing research in the field of biomechanics suggests that mathematical modeling may facilitate this task. This paper explores the possibility of generating a family of toe walking gait patterns by systematically changing selected parameters of a feedback-controlled model. METHODS: From the selected clinical case of toe walking we identified typical toe walking characteristics and encoded them as a set of gait-oriented control objectives to be achieved in a feedback-controlled walking model. They were defined as fourth order polynomials and imposed via feedback control at the within-step control level. At the between-step control level, stance leg lengthening velocity at the end of the single support phase was adaptively adjusted after each step so as to facilitate gait velocity control. Each time the gait velocity settled at the desired value, selected intra-step gait characteristics were modified by adjusting the polynomials so as to mimic the effect of a typical therapeutical intervention - inhibitory casting. RESULTS: By systematically adjusting the set of control parameters we were able to generate a family of gait kinematic and kinetic patterns that exhibit similar principal toe walking characteristics, as they were recorded by means of an instrumented gait analysis system in the selected clinical case of toe walking. We further acknowledge that they to some extent follow similar improvement tendencies as those which one can identify in gait kinematics and kinetics in the selected clinical case after inhibitory casting. CONCLUSIONS: The proposed walking model that is based on a two-level control strategy has the ability to generate different gait kinematics and kinetics when the set of control parameters that define walking premises change. Such a framework does not have only educational value, but may also prove to have practical implications in pathological gait diagnostics and treatment.
BACKGROUND: In clinical gait assessment, the correct interpretation of gait kinematics and kinetics has a decisive impact on the success of the therapeutic programme. Due to the vast amount of information from which primary anomalies should be identified and separated from secondary compensatory changes, as well as the biomechanical complexity and redundancy of the human locomotion system, this task is considerably challenging and requires the attention of an experienced interdisciplinary team of experts. The ongoing research in the field of biomechanics suggests that mathematical modeling may facilitate this task. This paper explores the possibility of generating a family of toe walking gait patterns by systematically changing selected parameters of a feedback-controlled model. METHODS: From the selected clinical case of toe walking we identified typical toe walking characteristics and encoded them as a set of gait-oriented control objectives to be achieved in a feedback-controlled walking model. They were defined as fourth order polynomials and imposed via feedback control at the within-step control level. At the between-step control level, stance leg lengthening velocity at the end of the single support phase was adaptively adjusted after each step so as to facilitate gait velocity control. Each time the gait velocity settled at the desired value, selected intra-step gait characteristics were modified by adjusting the polynomials so as to mimic the effect of a typical therapeutical intervention - inhibitory casting. RESULTS: By systematically adjusting the set of control parameters we were able to generate a family of gait kinematic and kinetic patterns that exhibit similar principal toe walking characteristics, as they were recorded by means of an instrumented gait analysis system in the selected clinical case of toe walking. We further acknowledge that they to some extent follow similar improvement tendencies as those which one can identify in gait kinematics and kinetics in the selected clinical case after inhibitory casting. CONCLUSIONS: The proposed walking model that is based on a two-level control strategy has the ability to generate different gait kinematics and kinetics when the set of control parameters that define walking premises change. Such a framework does not have only educational value, but may also prove to have practical implications in pathological gait diagnostics and treatment.
By providing detailed insight into the physiology of human walking, extensive clinical
application of instrumented gait analysis has considerably deepened our understanding of
human locomotion mechanisms and has significantly improved the accuracy and reliability
of pathological gait assessment [1-4]. On the other hand, being faced with a vast amount of information that
required proper interpretation, clinicians, therapists and biomechanists were compelled
to combine efforts to properly process and interpret the available walking information
in order to reach the decision about the most promising therapeutical intervention. This
task is even more challenging if we consider that gait pattern is often changed due to a
combined effect of more than one impaired muscle functionalities and/or bone deformities
rather than due to an isolated gait anomaly [3,4]. Despite continuous efforts, to date no general or standardized methodical
approach has been adopted that would enable straightforward data interpretation and
pathological gait diagnostics, let alone provide a reliable forecast about the most
likely outcome of individual therapeutical intervention.However, the ongoing research in the field of biomechanics suggests that a vast amount
of unused potential may be available in biomechanical modeling and simulation.
Mathematical modeling of the human gait departs from the actual biomechanical system and
describes the properties of the human musculo-skeletal system with corresponding
mathematical models. Such decomposition grants the user unlimited access to all of the
model parameters. In terms of human movement analysis and pathological gait diagnostics
and treatment, the user would strive to identify a particular anomaly by determining the
model parameters that induce the underlying pathology. In the subsequent decision making
process the user would ideally want to estimate the most likely outcome after selected
therapeutical intervention by adjusting these parameters in such a way as to encode the
physiological changes due to particular intervention. The efficiency of such an approach
inevitably depends on the ability authentically to model the human locomotion apparatus
and physiological processes and also on how the motion itself is being generated. There
are two mainstreams being followed when generating motion, and they have proven to have
great potential for practical applicability in human gait interpretation and analyses:
optimization-based modeling [5-19] and control-based modeling [20-27].Optimization-based models generate joint motions and joint forces by optimizing human
related performance criteria subject to physical constraints [5-16,19]. The key issue of such an approach is the selection of appropriate objective
criteria and corresponding constraints [6]. If prerecorded motion data are available, the objective criteria reflect the
actual physiology of human motion. They offer realistic and arbitrarily detailed
modeling of the human locomotion system, which has already proven invaluable in
interpretations of normal as well as pathological human gait [14,16-18]. However, in motion prediction it is doubtful whether if new optimization
criteria can be adequately formulated, since they should relate to the motion which is
actually the subject of prediction. Also, when formulating an optimization problem one
must bear in mind the required computation time. In order to reach an optimal solution
on a large scale musculo-skeletal model, the amount of required computational effort is
enormous. To some extent computational demands may be mitigated by applying
control-based models.Control-based models utilize various control algorithms to calculate joint actuations
that drive the biped to follow predefined trajectories [20-24,28,29]. They are often embedded in the optimization-based walking models. First,
feedback control is used to obtain joint actuations that impose the desired kinematics
obtained by means of motion capture system, and afterwards static optimization
techniques compute the muscle excitation [24-26]. Since this approach can produce high detailed motion on the level of muscle
forces, it seems to be tailored for the interpretation of patient-specific pathological
gait and muscle tendon force prediction. On the other hand, the necessity for a priori
walking demands does interfere with the possibility of motion prediction. Since a priori
walking demands are a prerequisite in the control-based approach, the possibility of
generating new movements that would reflect structural or control changes is
considerably limited. It has been suggested, though, that an adaptive feedback control
may be a promising approach. In [27] we proposed a two-level adaptive feedback control strategy that can generate
toe walking kinematics and kinetics in a simple planar biped walking model that to some
extent corresponds to principal walking characteristics as observed in clinical cases of
toe walking. The method is based on defining a set of general walking premises rather
than prescribing the actual joint angles, which forms a framework where joint angles do
not depend solely on angle references but are free to develop within a set of desired
walking premises.In this paper we explore the possibility of developing a family of toe walking gait
kinematic and kinetic patterns with distinguished toe walking characteristics by first
parametrizing the desired walking premises and later introducing these parameters as
gradually changing control objectives to the feedback-controlled toe walking model. We
envision, that in interpretations of human gait pattern, the imposition of such changes
may encode constrained walking premises due to an underlying primary anomaly, while in
prediction of the therapy outcome they may encode expected walking premises due to
selected therapeutical intervention, whereas the evaluation of resulting gait kinematics
and kinetics at the end would identify the overall success of the selected therapeutical
intervention.
Methods
The following sections present a biped walking model and corresponding two-level control
strategy in a condensed form. A detailed overview is available in [27].
Biped walking model
The model considered is a planar biped walking model with eight body segments. Thigh,
shank and foot segments are connected at hip, knee and ankle joints respectively, and
carry the pelvis and torso segments (Figure 1). We consider a
step to be a movement of the biped walking model between the contact of one leg and
the successive contact of the opposite leg. Each step is divided into phases of
double support and single support. Compared to the double support phase, when both
legs are in contact with the ground, in the single support phase only the stance leg
remains in contact with the ground and the opposite leg advances towards the point of
next contact. Two consecutive steps constitute a complete gait cycle. By following a
Lagrange formulation of the constrained system, the equations of motion in single
support and double support can be formed as:
Figure 1
Schematic representation of the biped walking model.
and written in the state space form as:Schematic representation of the biped walking model.Transition between single support and double support is referred to as the contact
phase and is associated with the swing leg touching the ground. Likewise, transition
between double support and single support is referred to as the take-off phase and is
associated with the trailing leg lifting off the ground. Both transition phases are
assumed to be instantaneous. The following set of algebraic equations describes both
transition phases:In (1) and (3) q is a set of configuration coordinates with superscript
+ denoting the set of configuration variables just after the
transition, and superscript − denoting the set of configuration
variables just before the transition; u denotes the set of joint moments,
M is the inertia matrix, C is the matrix of centripetal and
Coriolis terms, G is the gravity vector, Γ accounts for
constraints and λ is a set of negative ground reaction forces.The control strategy applied in this toe walking model is a two level control
strategy that on a lower, within-step control level in support phases imposes
trajectory tracking via feedback control, and on the higher, between-step control
level adaptively adjusts forward propulsion by changing virtual stance leg
lengthening velocity at the end of the single support after each step so as to
achieve stable gait at the desired gait velocity. In single and double support,
general walking characteristics are encoded as a set of holonomic constraints and as
outputs imposed on the toe walking model via feedback control. Observations of human
walking in the single support phase suggest that humans move roughly symmetrically,
the swing leg is lifted off the ground to assure sufficient foot clearance when
advancing towards the point of new contact, vertical hip movement is minimized to
prevent excessive energy consumption, whereas the pelvis as well as torso segments
display slight oscillatory movement about the selected position close to the
vertical. While this set of demands is sufficient for generating stable walking of
the model, two additional demands are needed to calculate the two remaining joint
moments. Since the aim of the model is to investigate changes in toe walking
kinematics and kinetics subject to variations in control parameter values, these
additional demands have been chosen to control the extent of ankle plantar flexion,
which in toe walking is the main pathological characteristic. For this reason we
introduced the virtual stance/swing leg (L
and L respectively), being the distance
between the tip of stance/swing foot and the hip joint. The virtual stance/swing leg
is further divided into the ankle component of the virtual stance/swing leg
(L and
L, respectively) and the knee
component of the virtual stance/swing leg
(L and
L, respectively) (Figure 1). By selecting ankle components of both virtual legs as the
remaining control objectives, general walking observations in single support can be
incorporated in the following output vector:When zeroing out the yvia feedback control,
w ensures exponential reduction of the
asymmetry immediately after lifting the swing leg off the ground. Furthermore,
controlling the foot clearance on one hand prescribes sufficient foot clearance to
prevent the swing leg from hitting the ground while advancing, but also defines when
the swing leg should touch the ground, thus ending the single support phase. Namely,
assuming that the symmetry is being imposed via feedback control at the end of single
support directly implies that the swing leg should touch the ground and terminate the
single support phase exactly whenIn (5) q denotes the desired
virtual stance leg angle at the end of the single support phase and is related to
desired gait velocity v, desired cadence
cad and desired step length
L asNominal length of the virtual leg L
and k1 determine how high the swing leg is lifted while
advancing, whereas w and
w assure smooth exponential transition. The
remaining
L(q),
q(q),
q(q),
L(q)
and
L(q)
define the desired virtual stance leg length, desired pelvic movement, desired torso
movement and desired lengths of ankle components of stance and swing leg
respectively. They are all defined as fourth order polynomials. As shown in Figure
2, five parameters suffice to completely define the fourth
order polynomial. The initial position and initial velocity for any of the five
polynomials are determined according to the state of the model in the preceding
take-off phase to assure position and velocity continuity, whereas the remaining
three parameters may be user-defined to impose the desired gait characteristics. Five
corresponding parameters for each of the selected reference trajectories are
presented in Table 1.
Figure 2
Polynomial representation of the control objective. Five parameters are
needed for unique definition of the forth order polynomial.
Table 1
List of parameters defining fourth order polynomial representation in five
selected reference trajectories
pss(t)
Lst,v,d(qst,v)
qP(qst,v)
qT(qst,v)
Lst,ankle,d(qst,v)
Lsw,ankle,d(qst,v)
Pss,start
Lst,v,start
qP,start
qT,start
Lst,ankle,start
Lsw,ankle,start
position continuity
Pss,mid
Lst,v,mid
qP,mid
qT,mid
Lst,ankle,mid
Lsw,ankle,mid
user defined
Pss,end
Lst,v,end
qP,end
qT,end
Lst,ankle,end
Lsw,ankle,end
user defined
P˙ss,start
L˙st,v,start
q˙P,start
q˙T,start
L˙st,ankle,start
L˙sw,ankle,start
velocity continuity
P˙ss,end
L˙st,v,end
q˙P,end
q˙T,end
L˙st,ankle,end
L˙sw,ankle,end
user defined
Polynomial representation of the control objective. Five parameters are
needed for unique definition of the forth order polynomial.List of parameters defining fourth order polynomial representation in five
selected reference trajectoriesDue to the fact that both legs are in contact with the ground in double support, the
available space of motions in double support is decreased by one degree of freedom as
compared to single support. Therefore only six linearly independent output functions
can be selected to describe the motion of the toe walking model in double support.
Enforcing symmetry in the double support phase would interfere with forward
progression and prevent proper weight transfer. Instead, the model must take into
account small asymmetrical movement until lifting the trailing leg off the ground.
Similarly, since both legs remain in contact with the ground throughout the double
support, foot clearance is suspended from the set of output functions. Since the
duration of double support is considerably smaller than the duration of single
support, the expected range of motion in double support is considerably smaller. For
this reason we selected the reference trajectories in double support as slow
exponential functions (via w,
w, w,
w and w), which
yields the following output vector in double support:After defining the output vectors in single and double support, the control objective
is to drive the outputs y and
y to zero. By following the standard Lie
derivative notation the following feedback is applied in single support:Likewise, the following set of inputs will impose the desired movement in double
support:In (8) and (9),
LLh denotes
the decoupling matrix, K and
K are positive definite gain matrices whereas the
superscript + indicates Moore-Penrose inverse.Before starting the next single support phase, the higher between-step control level
adaptively adjusts the virtual stance leg lengthening/shortening velocity at the end
of single support according to gait velocity in the preceding step
. If the model walks slower than desired
, then the model should accelerate, whereas if the model
walks faster than desired , then the model should slow down. Preliminary
simulation experiments [27] demonstrated that this is possible by increasing/decreasing push-off
through subtle adjustments of . This is encoded in the following between-step control
algorithm:wherek and kdenote
positive gains. Complete mechanism of the two-level feedback control strategy is
illustrated in Figure 3.
Figure 3
Schematic diagram of the two level control strategy.
Schematic diagram of the two level control strategy.We used Matlab and Matlab Simulink for development of the biped walking model and
control strategy as well as for performing the simulation experiment.
Generating different gait kinematics and kinetics
It has been experimentally verified in [27] that adaptively adjusting after each step so as to enable gait velocity control
significantly improves biped model robustness and stability. In our opinion this is
the essential condition that would assure stability even if the values of selected
control parameters were modified by the user with the intention of generating desired
gait pattern characteristics. According to Table 1 fourteen
control parameters remain available to define specific toe walking characteristics.
Let(11)be the set of selected control parameters and letdenote gait kinematics and kinetics in double support and succeeding single support
(i.e. in one step) after settling at the preselected gait velocity. Assuming that the
toe walking model settles at the desired preselected gait velocity and that
y and yzero out
after being imposed onto the model via feedback control, then each
π may be considered as a stable state of the
toe walking model that is uniquely identified with the set of control parameters
ζ. By changing the set of control parametersthe model will develop new stable gait kinematics and kinetics
π→π
in a finite number of steps l only if
δζ is
sufficiently small to prevent model destabilization. Since
ζ uniquely defines the corresponding
π, in general there exists more than one
sequence of
δζi = j…r,
that will eventually result in developing the same toe walking gait kinematics and
kinetics. Likewise, by selecting such a sequence of
δζi = j…r
that
ζ =ζ, the
toe walking model will return to the same stable state, hence
π =π.
The concept of changing gait kinematics and kinetics by adjusting the set of control
parameters is illustrated in Figure 4.
Figure 4
Transitions between stable states πi. After settling at
desired gait velocity, changing the set of control objectives
ζwill result in settling at new stable state with modified gait
kinematics and kinetics.
Transitions between stable states πi. After settling at
desired gait velocity, changing the set of control objectives
ζwill result in settling at new stable state with modified gait
kinematics and kinetics.
Clinical case of toe walking
The aim of this study was to investigate through simulation experiment whether a
sequence ofζ can be selected in such a way that
the resulting family of simulated toe walking gait patterns would qualitatively
follow kinematic and kinetic changes due to typical intervention in clinical
practice. Considering that the small number of DOFs confines the feasible range of
movements to a significantly smaller space than typically available in humans, we
find incorporation of only principal toe walking characteristics in our toe walking
model rather than exact reconstruction of selected gait kinematics and kinetics to be
a rational compromise. For this reason we followed a typical clinical case of toe
walking gait pattern as recorded in an eleven-year-old male subject before and after
serial inhibitory casting (Figure 5). The subject was diagnosed
with cerebral palsy, spastic diparesis, with excessive equinus gait. Before serial
inhibitory casting he was three times treated with botulinum toxin due to excessive
plantar flexor spasticity and once underwent serial inhibitory casting.
Figure 5
Clinical example of toe walking.
Clinical example of toe walking.We used a standardized methodology for recording the subject’s gait kinematics
and kinetics. 3D movements of IR reflective markers that were placed over palpable
anatomical landmarks were recorded with the Vicon Mx motion capture system and were
used in subsequent joint angle calculations. Simultaneously, we used two AMTI force
plates that were positioned in the middle of the walkway to record ground reaction
forces for subsequent joint moments calculations. A representative gait pattern was
obtained by averaging gait kinematics and kinetics for both legs in at least three
valid strides. A stride was considered to be valid if the same leg landed within the
boundaries of one of the two force plates.The recorded toe walking gait pattern allows us to observe the principal
characteristics of toe walking. Compared to normal walking, the toe walking gait
displays immediate movement towards ankle dorsal flexion after contact, it is further
typical for the ankle joint in support phase to exhibit considerably increased
plantar flexion; particularly increased are also knee flexion in the support phase
and at the end of the swing phase as well as hip flexion throughout the gait cycle.
Consequently, the ankle plantar flexion moment graph displays characteristic increase
in early and midstance phase and decrease during push-off, in the knee moment graph
we noticed considerably pronounced extension moment throughout the stance phase,
whereas in the hip we recorded considerably increased extension moment in the early
stance phase and increased flexion moment in the terminal stance phase. Although the
child persisted in the toe walking gait pattern after inhibitory casting, the
improvement is clearly evident. After inhibitory casting we noticed a significant
shift of the ankle joint trajectory towards normal walking and noteworthy evolution
of somewhat more extended posture in the knee as well as in the hip. This
additionally led towards larger, almost normal ankle plantar flexion moment during
push off, knee extension moment decreased but remained well above the normal level,
whereas both hip extension and flexion moment bursts in early stance and terminal
stance phases decreased, respectively.
Simulation experiment
Clinical observations of toe walking dictated the selection of such a sequence of
ζthat encoded the following simulation
objectives: when compared to normal walking ζ1 had to induce
i) pronounced plantar flexion, ii) increased knee and hip flexion, iii) pronounced
ankle plantar flexion moment in the early stance phase and somewhat decreased ankle
plantar flexion moment during push-off, and iv) pronounced knee extension moment in
the stance phase. After settling at the desired gait velocity,
ζ1 (and successive ζ)
were modified according to (13) in such a way as to gradually encode the primary
effects of inhibitory casting - releasing the tension in the plantar flexor muscle
group - which considerably reduces kinematic constraint predominantly in the ankle
joint. In terms of ζ, such intervention was
encoded predominantly by gradually decreasing
L,
L,
L and
L as well as by
gradually increasing and . We expected that such progressive manipulation with
the set of control parameters ζ (13) should
gradually result in qualitatively similar kinematic and kinetic improvements as
recorded in the selected clinical case (Figure 5): v) ankle
plantar flexion should decrease, vi) knee and hip joints should allow more
outstretched posture, vii) ankle plantar flexion moment during push-off should shift
towards the normal pattern, and viii) knee extension moment should decrease.To assure model stability any change in ζwas
performed manually after the model became stable at desired gait velocity and with a
sufficiently subtle rate of change in
δζ. We used
the standard deviation of gait velocity in the last N steps
σ(v) as a
measure of gait stability. Gait kinematics and kinetics in the k-th step was
considered stable ifwhere ε denotes a sufficiently small level of permissible deviation
from the desired gait velocity. Given the slow rate of change in
δζ the
simulation experiment spanned over more than five hundred successive gait cycles. We
selected gait kinematics and kinetics in five gait cycles that best demonstrate the
development of the desired gait characteristics. Their corresponding
ζ are listed in Table 2.
Table 2
Values of ζi in selected gait cycles
ζ
π1
π2
π3
π4
π5
Lst,v,mid
cm
79.6
79.6
80.0
80.0
80.3
Lst,v,end
cm
82.0
82.0
83.6
81.1
81.9
qP,mid
rad
-0.05
-0.05
-0.05
-0.05
-0.05
qP,end
rad
-0.05
-0.05
-0.05
-0.05
-0.05
q˙P,end
rad/s
-0.15
-0.15
-0.15
-0.15
-0.15
qT,mid
rad
0
0
0
0
0
qT,end
rad
0
0
0
0
0
q˙T,end
rad/s
-0.15
-0.15
-0.15
-0.15
-0.15
Lst,ankle,mid
cm
8.6
7.2
5.6
5.6
5.6
Lst,ankle,end
cm
9.4
8.6
6.2
6.2
6.9
L˙st,ankle,end
cm/s
10
10
20
20
20
Lsw,ankle,mid
cm
8.4
8.4
8.1
8.1
8.1
Lsw,ankle,end
cm
7.6
7.6
6.2
6.8
6.8
L˙sw,ankle,end
cm/s
0
0
10
10
10
Values of ζi in selected gait cycles
Data processing
It is common in biomechanics to present the gait pattern of an individual as a
combination of gait kinematics and kinetics for one leg and for the whole gait cycle
(i.e. between two consecutive contacts of the same leg). For this reason we gathered
the simulation results for one side in two consecutive steps and assumed that a
single support phase of one leg corresponds to a swing phase of the opposite leg.
Additionally, kinetic data were filtered by using a fourth order Butterworth filter
with cutoff frequency f = 5Hz.
Results
Figure 6 shows simulation results in five selected gait cycles.
When qualitatively inspecting kinematics and kinetics, we notice that all simulation
cases developed the principal characteristics of toe walking. Moreover, by progressively
changing the set of control parameters ζ as listed in
Table 2, we were able to generate a sequence of toe walking gait
kinematics and kinetics that gradually developed similar improvement tendencies
(indicated by arrows) as recorded in the clinical case of toe walking after inhibitory
casting (Figure 5). Typically pronounced ankle plantar flexion in
the stance phase gradually decreased and shifted toward the normal range of ankle
movement while retaining the toe walking pattern. In the knee joint approximately 60
degrees of initial knee flexion was reduced to less than 40 degrees after gradually
changing the set of control parameters. A similar result is present in the hip joint -
generally increased hip flexion throughout the stance and hip extension in terminal
stance gradually shifted towards normal hip kinematics.
Figure 6
Developing kinematic diversity in gait simulations by changing the set of
control parameters ζ. The sequence of black and white rectangles below
the three graphs in the lower panel indicate consecutive phases of double support
phase (0–5% of GC), left leg single support phase (5–50% of GC),
double support phase (50–55% of GC) and left leg swing phase (55–100%
of GC). Two transitions from black to white (5% of GC and 55% of GC) indicate
right leg and left leg take-off respectively, whereas transition from white to
black (50% of GC and 100% of GC) indicates the right leg and left leg contact
phase respectively. Additionally, the interval 0–10% of GC is referred to as
early stance phase, the interval 10–40% is referred to as midstance, the
push off indicates the interval 40–50% of GC and the interval 50–55%
denotes terminal stance phase.
Developing kinematic diversity in gait simulations by changing the set of
control parameters ζ. The sequence of black and white rectangles below
the three graphs in the lower panel indicate consecutive phases of double support
phase (0–5% of GC), left leg single support phase (5–50% of GC),
double support phase (50–55% of GC) and left leg swing phase (55–100%
of GC). Two transitions from black to white (5% of GC and 55% of GC) indicate
right leg and left leg take-off respectively, whereas transition from white to
black (50% of GC and 100% of GC) indicates the right leg and left leg contact
phase respectively. Additionally, the interval 0–10% of GC is referred to as
early stance phase, the interval 10–40% is referred to as midstance, the
push off indicates the interval 40–50% of GC and the interval 50–55%
denotes terminal stance phase.The ankle moment graph shows in all gait cycles a characteristic double teeth ankle
plantar flexion moment that is generally present also in clinical cases of toe walking.
After gradually changing the set of control parameters
ζ the first peak in early and mid stance remained
unchanged, whereas the second peak during push-off gradually increased from a typically
modest ankle plantar flexion moment to almost normal range. In the knee joint, the
initially pronounced knee extension moment diminished almost by half after changing the
set of control parameters ζ whereas in the hip joint the effect of varying
the set of control parameters ζ had a negligible effect - all simulation
cases show large extension and flexion moment bursts in the early stance and early swing
phase, respectively, that to some extent coincide with the increased extension moment in
the early stance and increased flexion moment in the early swing phase.In terms of selected ζ (Table 2) we notice that
these changing trends in gait kinematics and kinetics correspond predominantly to
gradual shortenings in the ankle components of virtual stance and swing leg. Decreasing
L,
L,
L and
L up to 35 % not only
changed the ankle kinematics and kinetics; due to the relatively constant length of the
virtual stance leg (L and
L) they also imposed a more
outstretched posture in the knee joint. Such improvements are typically present after
undergoing inhibitory casting in CP children.
Discussion
In the development of our toe walking model, our aim was to form a framework in which
the joint movements would not need to be directly defined but could be inherently
encoded in a set of general walking premises that are imposed through parameterized
reference functions. The rationale behind imposition of the desired walking demands
instead of following prerecorded joint angle trajectories is that in the latter approach
each gait pattern requires its own set of joint angle references, and any deviation from
the existing joint movements significantly aggravates model stability. On the other
hand, in our simulation experiment we have shown that by encoding joint motions via a
set of walking demands, the joint angles are free to develop so as to comply with these
demands, and that changing only one walking demand in general imposes entirely new gait
kinematics and kinetics on all joints without jeopardizing model stability. This closely
relates to the typical situation in pathological gait treatment. Namely, in clinical
gait analysis and treatment the primary effect of a certain anomaly or treatment is
often known only locally, whereas the secondary compensatory changes which arise in
response to a primary anomaly do change the gait kinematics and kinetics globally. For
example, plantar flexor muscle contracture primarily increases ankle plantar flexion and
reduces push-off. On the other hand, the human neural system may compensate for the lack
of push-off by tilting the torso forward, increasing hip moment by recruiting hip
muscles or placing an additional load on the knee joint, depending on the state of the
muscles involved. It is a challenging task that requires a lot of experience to
distinguish between primary anomalies and secondary compensations, as any deviation in
gait kinematics and kinetics from the normal gait occurs due to the combined effect of
primary as well as compensatory anomalies. It is also a crucial step in pathological
gait treatment, as only primary anomalies should be treated, whereas secondary changes
will disappear when they are no longer needed.We envision the following situation in which generating new gait kinematics and kinetics
by gradually changing the walking premises in a simulation model could complement the
conventional approach to pathological gait treatment. When initially being acquainted
with the patient’s gait kinematics and kinetics the therapist would reconstruct
the patient’s gait kinematics and kinetics by systematically tuning walking
premises in the simulation model until the gait kinematics and kinetics of the patient
and the model were matched: in each iteration the therapist would gradually and by
growing δζ change the set of
normal walking premises as defined by the set of normal control parameters
ζ in such a way that the resulting
ζ would impose gait kinematics and kinetics
that would correspond sufficiently well to the gait kinematics and kinetics of the
patient. To simplify, let us assume that to achieve this it would suffice to gradually
adjust the value of only the k-th parameter in each iteration. The validity of such an assumption
proceeds from the ability to modify gait kinematics and kinetics in all joints by
adjusting the value of only one control parameter that in turn adjusts the corresponding
walking premise. Once kinematics and kinetics of the patient and the simulation model
were matched, a team of clinicians, therapists and engineers would interpret the
discrepancies between and in terms of the most likely primary reason. Therefore,
instead of establishing causal relationships between all deviations in gait kinematics
and kinetics, the interpretation of gait kinematics and kinetics by means of simulation
models would focus on determining the primary anomaly that is responsible for a
particular discrepancy between and . This would immediately grade some primary causes which
they would usually consider as very unlikely and would significantly narrow the range of
available therapeutical interventions, which would significantly facilitate the decision
about the most promising treatment. Since the primary effects of most common
interventions are well delineated and can be easily encoded as modification
δζ, the therapist would in
subsequent treatment planning gradually change the existing walking premises
ζ = ζ
+ δζ. Hence, the model would
predict new gait kinematics and kinetics which would reflect the effects due to the
selected therapeutical intervention.Due to the absence of ζand structural simplicity
of our toe walking model which aggravates reconstruction of the actual gait pattern, we
were able only partly to illustrate this procedure in our simulation experiment. By
following simulation objectives i-viii as defined in section Simulation experiment, we
initially established such a set of control parameters
ζ=ζ(π1)
(Table 2) which induced toe walking gait kinematics and kinetics
π1with similar toe walking characteristics as present in the
selected clinical case of toe walking before the intervention (Figure 5) - simulation objectives i-iv. Even though
ζ was not available,
ζ (more precisely high
L,
L,
L and
L) clearly indicates
pronounced plantar flexion. Experience from clinical practice shows that inhibitory
casting primarily decreases ankle plantar flexion and increases dynamics of the
movement. To investigate the effect of such intervention in this particular clinical
case of toe walking we encoded inhibitory casting by gradually reducing
L,
LL
and L as well as increasing
and according to
ζ(π2)…ζ(π5)
in Table 2. Despite toe walking gait characteristics still being
present, gait kinematics and kinetics
π2…π5 (Figure 6) in general moved towards the normal range of movement and complied with
the simulation objectives v-viii. Since the new gait pattern may be considered as less
demanding, we may assume inhibitory casting to be an intervention with a potentially
positive outcome. To evaluate the simulation results, they were compared to the actual
clinical case of toe walking where the patient underwent inhibitory casting (Figure
5). By focusing on generally desired improvements (simulation
objectives v-viii), rather than reproducing the clinical outcome, we notice that
selected simulation gait cycles follow similar improvement tendencies (in Figure 6 they are marked with arrows) to those which one can identify in
gait kinematics and kinetics after inhibitory casting in the selected clinical case
(Figure 5).The limitations of the proposed approach predominantly proceed from the simplified
structure of the simulation model. The small number of degrees of freedom that confines
the motion to only the sagittal plane significantly reduces the feasible range of
movement of the model and cannot adequately account for compensations that often occur
in transversal or coronal planes of motion. The main argument why focusing on sagittal
plane only may be a reasonable compromise is that compensations are considerably better
understood in transversal and coronal planes than in the sagittal plane, which is the
plane of forward propulsion and progression. Nevertheless, expanding the feasible range
of motion to the transversal (and coronal) plane of motion would improve the
applicability of such a model, especially since human gait is synchronized and
interrelated motion in all three planes of motion and should be treated as such. This is
a precondition for successful and accurate reconstruction of patient specific gait
kinematics and kinetics. At the current stage of toe walking model development, the
reconstruction of human locomotion is feasible only to the extent that is supported by
the modest structural complexity of the model. That is why reproduction of the
patient’s gait kinematics and kinetics was beyond the scope of this research and
is the subject of future work. Instead, we focused on construction of the principal
characteristics of toe walking and qualitatively similar improvement tendencies to those
which one can observe in the selected clinical case of toe walking. On the other hand,
the desire to accurately reconstruct a particular gait pattern presumes negligible
adjustments of the proposed control strategy. Namely, to extrapolate the feasible range
of movement to all planes of motion, one would only need to extend the existing set of
walking premises with additional walking premises and introduce them as new control
parameters to the two-level control strategy without interfering with the overall
control scheme (Figure 3). Such a model would then be suitable for
more challenging clinical cases where the gait is changed due to the combined effect of
more than one incorrect muscle functionalities.Following the example of [24-26], the method as presented in this paper could also combine feedback control
and static optimization techniques to calculate muscle forces. Thus the gait analysis
could be extended to a muscle recruitment level instead of joint moments. We further
suggest yet another optimization level which, in the process of gait diagnostics, would
determine the set of control parameters in such a way as to minimize the deviations
between the simulated gait pattern and the gait pattern of a particular patient,
prerecorded by means of instrumented gait analysis. This would not only speed up the
diagnostic process but would also optimize walking demands with respect to each
individual. We also believe this would diminish the undesirable effects of the contact
phase and switching control strategy. The rigid contact model assumes velocity
discontinuities when switching from single to double support, whereas the switching
control strategy imposes two large hip moment bursts at the beginning of the single
support and the beginning of the swing phase (the opposite leg is in single support),
respectively. While they are consistent with clinical observations of toe walking
(Figure 5) it is very likely that the majority of surplus arises
due to rapid correction of asymmetry from the end of double support. This directly
affects the knee moment as well. To meet control demands, the knee actuator must
simultaneously provide sufficient knee flexion moment to compensate for excessive hip
extension moment, which would otherwise force the knee joint to extend.
Conclusions
Simulation experiments have shown that the proposed framework is capable of generating
primary toe walking characteristics as recorded in a selected clinical case of toe
walking. Also, when adjusting the set of control parameters so as to encode the primary
effect of inhibitory casting, which is a typical therapeutical intervention of toe
walking, the resulting gait kinematics and kinetics follow similar improvement
tendencies to those which one can identify in gait kinematics and kinetics after
inhibitory casting in the selected clinical case. This suggests the potentially
practical implication of the proposed framework in clinical gait assessment and therapy
planning in the future.
Competing interests
The authors declare that they have no competing interests.
Author’s contributions
Both authors significantly contributed to the conception, theoretical analysis,
simulation experiments, data interpretation and writing of the manuscript. Both authors
revised and approved the final manuscript.
Authors: Allison S Arnold; Darryl G Thelen; Michael H Schwartz; Frank C Anderson; Scott L Delp Journal: J Biomech Date: 2007-06-18 Impact factor: 2.712
Authors: Benjamin J Fregly; Jeffrey A Reinbolt; Kelly L Rooney; Kim H Mitchell; Terese L Chmielewski Journal: IEEE Trans Biomed Eng Date: 2007-09 Impact factor: 4.538