Vol. 89, Issue 4, 1322-1332, October 2000
A predictive model of fatigue in human skeletal muscles
Jun
Ding1,
Anthony S.
Wexler1,2, and
Stuart A.
Binder-Macleod1,3
1 Interdisciplinary Graduate Program in Biomechanics and
Movement Science, 2 Department of Mechanical Engineering,
and 3 Department of Physical Therapy, University of Delaware,
Newark, Delaware 19716
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ABSTRACT |
Fatigue
is a major limitation to the clinical application of functional
electrical stimulation. The activation pattern used during electrical
stimulation affects force and fatigue. Identifying the activation
pattern that produces the greatest force and least fatigue for each
patient is, therefore, of great importance. Mathematical models that
predict muscle forces and fatigue produced by a wide range of
stimulation patterns would facilitate the search for optimal patterns.
Previously, we developed a mathematical isometric force model that
successfully identified the stimulation patterns that produced the
greatest forces from healthy subjects under nonfatigue and fatigue
conditions. The present study introduces a four-parameter fatigue
model, coupled with the force model that predicts the fatigue induced
by different stimulation patterns on different days during isometric
contractions. This fatigue model accounted for 90% of the variability
in forces produced by different fatigue tests. The predicted forces at
the end of fatigue testing differed from those observed by only 9%.
This model demonstrates the potential for predicting muscle fatigue in
response to a wide range of stimulation patterns.
muscle fatigue; functional electrical stimulation; stimulation
pattern; stimulation frequency
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INTRODUCTION |
FUNCTIONAL ELECTRICAL
STIMULATION (FES) is the use of electrical stimulation to
activate muscles to produce functional movements. FES has been used
primarily to restore movement and function in patients with
neurological disorders (1, 10, 22, 25). However, muscles
are recruited differently when stimulated by FES from when they are
activated by the central nervous system. During FES-induced
contractions, motor units are activated synchronously, whereas during
voluntary contraction, they are activated asynchronously (14,
17). In addition, when stimulated by FES, the motor unit recruitment order differs from that seen during voluntary contractions (5). As a result, muscles fatigue more rapidly during FES
than during contractions activated by the central nervous system. This rapid fatigue is a major limitation to the clinical application of FES
(1, 22, 25).
It has been shown that the mean frequency and the pattern of pulses
markedly affect force production and fatigue (3, 9). One
approach to reducing fatigue is to identify the stimulation pattern
that minimizes fatigue and maximizes force. Traditionally, during FES,
skeletal muscles are activated with constant-frequency trains (CFTs),
where the pulses within each train are separated by regular interpulse
intervals (IPIs; Fig. 1). One stimulation pattern that has been shown to produce more force from a fatigued muscle than any CFT is a variable-frequency train (VFT) that begins with a doublet (i.e., 2 pulses separated by a brief IPI)
(7). Recently, a stimulation pattern containing doublets
throughout the train (DFT) was found to produce greater forces than
CFTs and VFTs from fatigued human muscles (4, 15).
However, the pattern that maximizes the force varies with the
physiological conditions of the muscle, such as level of fatigue
(15) or muscle length (24), and varies from
person to person (15, 21). In addition, although VFTs have
been shown to produce greater forces from fatigued muscles, they also
produce greater fatigue than CFTs (8, 9). Moreover, muscle
fatigue is a complex physiological phenomenon, and the underlying
mechanisms are not well understood (2, 19). Numerous tests
and testing sessions would be needed to identify the stimulation
pattern that produces the most force and least fatigue for each
patient. Mathematical models that can predict muscle forces and fatigue
can speed up this process.

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Fig. 1.
Force responses to stimulation patterns. Data were
collected from 1 typical subject's quadriceps femoris muscle under the
nonfatigue condition. Vertical bars on the x-axis designate
the stimulation pulses with pulse width of 600 µs. CFT25, CFT66, and
CFT100, constant-frequency trains with interpulse intervals (IPIs) of
25, 66, and 100 ms; VFT50 and VFT80, variable-frequency trains with an
initial doublet and subsequent IPIs of 50 and 80 ms; DFT155,
stimulation pattern containing doublets throughout the train with IPI
of 155 ms.
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Several models have been developed to study muscle fatigue, including
nonphysiological analytic models (11, 26, 28) and models
that used physiological information such as myoelectric [electromyogram (EMG)] (12, 26) or metabolic (e.g., NMR)
measurements (20, 27) as fatigue indexes added to muscle
force models. All nonphysiological analytic models have only tested
their ability to fit the forces produced during a fatigue test
(11, 26, 28). Although studies have supported a good
correlation between EMG amplitude and the forces during fatigue
(12, 26), the predictive ability of an EMG-based fatigue
model has never been demonstrated. Mizrahi and colleagues
(26) developed a three-time-constant analytic function to
curve fit the isometric forces produced by 20-Hz continuous stimulation
(180 s). The model produced an accurate fit. They also found a strong
exponential relationship (r = 0.986) between the force
and the peak-to-peak amplitude of the EMG M wave during fatigue. They
were not able, however, to predict forces using EMG data when the
muscle was fatigued by a different fatiguing protocol
(26). One of the limitations in modeling fatigue from an
EMG is the difficulty in obtaining clean, artifact-free EMG data,
because the stimulation currents are orders of magnitude larger than
those produced by muscle action potentials (12). In
addition, factors such as muscle fiber composition and stimulation history of the muscle complicate the force-EMG relationships, making it
less practical to predict forces during fatigue from the EMG signals
alone (26).
Mizrahi and colleagues (20, 27) used FES to develop a
series of musculotendon models of fatigue and recovery of the
quadriceps femoris muscles of paralyzed individuals. The 5-element
musculotendon model needed 17 non-muscle-specific parameters taken from
the literature and 5 muscle-specific parameters calculated from the femur length and circumference of the thigh of each subject. In addition, another seven parameters needed for the fatigue index were
obtained by fitting the fatigue equations to pH data during fatigue and
recovery taken from the literature. This model produced fairly good
fits for isometric forces during 180-s fatigue tests at four different
angles but did not include stimulation pattern or frequency as inputs;
therefore, it is not capable of predicting the force responses to a
variety of activation frequencies.
Previously, we developed a force model that accurately predicted the
force responses to a wide range of stimulation patterns when muscles
were nonfatigued or fatigued (15). We noticed that when
the muscles were fatigued the parameter values of this force model
differed significantly from those when the muscles were nonfatigued
(15). Our initial approach to modeling fatigue is to model
the changes in our force model parameter values during muscle fatigue.
The purpose of this study is to present a physiologically based fatigue
model that predicts changes in forces during repetitive activation of
skeletal muscles. The modifications of our previous force model are
presented first, and the theoretical development of the fatigue model
is described immediately thereafter. Next the predictions of the model
and comparison with the experimental data are evaluated.
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DEVELOPMENT OF THE FATIGUE MODEL |
Previously, we developed a mathematical model that successfully
predicted isometric muscle forces to a wide range of stimulation patterns (15). This force model has two differential
equations
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(1)
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with
and
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(2)
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The symbols used in Eqs. 1 and 2 are defined
in Table 1. Briefly, Eq. 1
represents the dynamics of the rate-limiting step leading to the
formation of a Ca2+-troponin complex (CN,
unitless), in which Ri (unitless) accounts for
the nonlinear summation of the Ca2+ transient in single
muscle fibers when stimulated with two closely spaced pulses
(16). This summation enhancement decays with IPI ti
ti
1 (ms). Thus,
Ri
1 for a pulse that occurs a
long time after the preceding pulse, and Ri
R0 for a pulse that occurs immediately after the
preceding pulse. Equation 2 represents the development of
mechanical force (F, in N), which is driven by force-producing
cross-bridges, modeled by a Michaelis-Menten term:
CN/(1 + CN).
The force model is governed by only five free parameters:
R0, A,
c,
1, and
2 (Table 1). In our previous
study,
c was fixed at 20 ms for nonfatigued and fatigued
muscles and
1 was calculated using experimental forces
(15). The other three parameter values were identified by
fitting the model to the measured forces produced by stimulating the
muscle with a combination of two trains (15). For
nonfatigued muscles, the two trains that best parameterized the model
were two VFTs: one with an initial 5-ms IPI followed by constant IPIs
of 10 ms (VFT10) and the other with an initial 5-ms IPI followed by
constant IPIs of 100 ms (VFT100). For fatigued muscles, the train
combination was a CFT with IPIs of 100 ms (CFT100) and VFT100.
The major shortcoming of this force model is that it needed two
different train combinations to parameterize the model for nonfatigued
and fatigued muscles, making it impossible to model the fatigue process
and to predict muscle forces under different levels of fatigue.
Systematic search for the best train or train combination to
parameterize the model under nonfatigue and fatigue conditions was
conducted in a pilot study (unpublished observations). We found the
combination of a VFT with an initial 5-ms IPI followed by four IPIs of
50 ms (VFT50) and CFT100 (i.e., a V50-C100 combination) to be the best.
The V50-C100 combination improved correlation coefficients
(R2) between the predicted and experimental
forces from 0.92 (old combination) to 0.95 (new combination) for
nonfatigued muscles and from 0.89 to 0.92 for fatigued muscles.
As with any other mathematical representations of muscle force, this
force model was inevitably based on some nonphysiological assumptions
such as the same value of
c (20 ms) for nonfatigued and
fatigued muscles. A prolonged Ca2+ transient with fatigued
muscles has been observed by Westerblad and Allen (30),
which might be due to depressed Ca2+ uptake
(31), reduced rate of Ca2+ release
(18), and elevated resting intracellular Ca2+
concentration, however (13). This observation suggests
that fixing
c at 20 ms in our previous study for
fatigued muscles may not be appropriate physiologically, although doing
so may not have affected the model's predictive ability because of the compensation effect from parameters
1 and
2. Conversely, the prolonged relaxation of the force
(controlled by
1 and
2 in the force
model) could also be modeled by the slower Ca2+ dynamics
with the fatigued muscle. For simplicity, in this study for fatigued
muscles, therefore, we fixed
1 and
2 at
the values obtained in the nonfatigued condition and fit the values of
the other three parameters (A, R0,
and
c) to the experimental forces. Further testing of
the V50-C100 combination showed that it was still the best combination
for parameterizing the force model under nonfatigue and fatigue conditions.
In addition, we found significant changes in the values of
A, R0, and
c as the
muscle made the transition from nonfatigue to fatigue conditions. Our
approach to modeling fatigue was to develop a model that could modify
the values of the force model parameters during fatigue. Studies have
shown that, during sustained isometric contractions, the rate and
amount of fatigue are related to the force-time integral produced by
the muscle in response to the train used to fatigue the muscle
(9). Therefore, we used instantaneous force as the driving
function in the fatigue model.
We assume that there is one time constant (
fat)
characterizing the rate of recovery. The fatigue model equations are
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(3)
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(4)
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(5)
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This fatigue model is governed by four parameters:
A (ms
2),
R0
(ms
1 · N
1),

c (N
1), and
fat (ms). Arest,
R0,rest, and
c,rest are the
values when muscles are not fatigued. F is the isomeric force.
Experimental forces were used in Eqs. 3-5 during
parameter identification, but once the fatigue model was parameterized,
forces predicted by Eqs. 1 and 2 were used to
test the ability of the model to predict fatigue (see
METHODS and Fig. 3).
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METHODS |
Experiments were conducted on human quadriceps femoris muscles
of healthy subjects. The experimental setup was similar to that
described previously (6). Briefly, subjects were seated on
a force dynamometer with their hips flexed to ~75° and their knees
flexed to 90°. Two stimulating electrode pads were placed over the
quadriceps muscle. The force transducer was positioned against the
anterior aspect of the leg, proximal to the lateral malleolus. The
subject's maximum voluntary isometric contraction (MVC) was first
determined using a burst superimposition technique (6).
The stimulus intensity was then set to elicit a force equal to 20% of
the subject's MVC obtained during the first testing session. Isometric
force data from the dynamometer's force transducer were digitized at a
rate of 200 Hz.
Stimulation Protocols
Testing began by first potentiating the muscle with 35, 12-pulse
CFTs with IPIs of 70 ms (CFT70; Fig. 2).
One train was delivered every 5 s. Pilot work showed that this
protocol maximally potentiated the muscle without causing a measurable
decline in forces. Two seconds after the potentiation trains, a
six-pulse VFT50 followed by 2 s of rest and then a six-pulse
CFT100 (i.e., the V50-C100 pair that we previously showed was best for
parameterizing the force model) were delivered to the muscle. These two
trains were used to establish the initial, nonfatigue condition for the
fatigue model. Two seconds after the V50-C100 pair, the fatigue
protocol started. Different testing sessions used different fatigue
protocols. Each train in the fatigue protocols had six pulses, and
there was a 500-ms rest time between trains; so the only differences between stimulation trains were the pulse frequency and the train duration. One fatigue protocol had 75 V50-C100 pairs to fatigue the
muscle (150 trains in total). Each of the other five fatigue protocols
contained 10 cycles of trains; each cycle contained 13 fatigue-producing trains followed by the V50-C100 pair, giving a total
of 150 trains. For each of these five fatigue protocols, the
fatigue-producing trains were constant-frequency trains with IPIs of 25 ms (CFT25), 66 ms (CFT66), or 100 ms (CFT100), VFTs with an initial
5-ms doublet followed by constant IPIs of 80 ms (VFT80), or DFTs with a
5-ms doublet as first, third, and fifth IPIs and second and fourth IPIs
of 155 ms (DFT155). The fatigue-producing trains had frequencies of 10 Hz (CFT100) to 40 Hz (CFT25) to cover the wide range of discharge
frequencies reported during physiological activations of human
quadriceps femoris muscle (29). The VFT80 and DFT155 were
chosen because they had the same mean frequency as the CFT66 (15 Hz)
but produced different force profiles (Fig. 1). The V50-C100 pairs
included during the fatigue protocol were used to monitor changes in
the force model parameters with time.

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Fig. 2.
Schematic representation of the experimental protocols. Each
subject received 6 sessions of testing, and each session started with
the same potentiation protocol and continued with 1 of the 6 fatigue
protocols.
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Subjects
Eight healthy subjects were recruited to test the ability of the
fatigue model to fit and predict forces during repetitive activation by
stimulation trains with a wide range of frequencies and patterns. Each
subject signed an informed consent form approved by University of
Delaware Human Subject Review Board.
Three of the eight subjects were tested to study the variance of the
experimental data. Each of these three subjects was tested with a CFT66
fatigue protocol (see Stimulation Protocols) on three different days. Peak forces were calculated for the force responses to
each stimulation train throughout the testing. Fatigue profiles for
peak forces were obtained by plotting the peak forces of each fatigue-producing train against their train number.
R2 values were used to compare the fatigue
profiles between days (i.e., day 1 vs. day 2, day
2 vs. day 3, and day 1 vs. day
3). The range of R2 values was
0.82-0.99 (mean 0.93). Next, the peak forces of the last 10 fatigue-producing trains were averaged to determine the fatigued forces
for each day. For each subject, differences in the fatigued forces
between days were averaged and then normalized to the averaged fatigued
forces to obtain the percent difference. The experimental data showed
that the percent differences in fatigued force between days ranged from
5.5 to 13.4% (mean 8.9%).
Six of the eight subjects were used to test the fatigue model by
measuring the fatigue produced by six different stimulation patterns.
Each subject was tested with all six patterns, only one pattern was
tested during a session, and sessions were separated by
48 h. The
order of sessions was randomized for each subject. The data were used
to test the fatigue model.
Testing the Fatigue Model
Calculating the force model parameter values using experimental
forces.
The force responses to the V50-C100 pair at the end of the potentiation
protocol and during the fatigue protocols were used to calculate the
sets of force model parameter values throughout the testing (76 sets of
force model parameter values for VFT50-CFT100 fatigue protocol; 11 sets
for the other 5 fatigue protocols). The V50-C100 pair delivered at the
end of the potentiation protocol was used to calculate the initial,
nonfatigued force model parameter values. Parameter
c
was set at 20 ms and
1 was identified directly from the
force record as described previously (15). The remaining three force model parameters (A, R0,
and
2) were identified using the following objective
function
|
(6)
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where G1 was minimized using CFSQP
(23), which employs feasibility set techniques coupled to
sequential quadratic programming to identify the optimum values for the
free variables numerically in an objective function (Fig.
3A).

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Fig. 3.
Schematic representations of the procedure used to parameterize the
force model for the nonfatigue condition (A) and during
fatigue testing (B), to parameterize the fatigue model
(C), and to predict the force responses to each fatigue
protocol (D). See Table 1 for definition of abbreviations.
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To identify the force model parameter values during fatigue, an
objective function similar to Eq. 6 was used, except
1 and
2 were fixed at the nonfatigued
values and A, R0, and
c were allowed to change (Fig. 3B). The force
model was fitted with the force responses to the V50-C100 pairs during
fatigue by use of the following objective function
|
(7)
|
G2 was also minimized by CFSQP
(23). There were 75 sets of
(A,R0,
c) for the
V50-C100 fatigue protocol and 10 for each of the other 5 fatigue protocols.
Parameterizing the fatigue model.
Unlike previous physiology-based fatigue models that used EMG or
metabolic changes as fatigue indexes, our fatigue model monitored the
changes of our force model parameter values during fatigue (Eqs.
3-5). To parameterize the fatigue model, the differences
between the predicted and calculated force model parameter values were first normalized to the calculated force model parameter values. This
normalization was performed to allow unbiased, concurrent evaluation of
all three parameters. The objective function was then minimized
|
(8)
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where q designates the number of the sets of force
model parameter values and ranges from 1 to 76 for the V50-C100
protocol and from 1 to 11 for the other protocols;
tq is 0 for the first set of force model
parameter values and 855 ms after the start of the qth
V50-C100 pair, which is the midpoint between the start of the V50 and
the end of the C100; Pjpred is
the jth parameter value (j = 1, 2, and 3 for
A, R0, and
c, respectively) predicted by Eqs. 3-5 at time
tq, and is a function of
fat, the
corresponding
j, and
F(tq) (the experimental force at time
tq).
Pjcalc is the jth
parameter value at time tq calculated
as described above. This objective function was minimized using CFSQP
(23) (Fig. 3C).
Predicting forces by use of the parameterized fatigue model.
For each subject, the fatigue model was parameterized separately using
the forces from each of the six fatigue protocols, resulting in six
sets of fatigue model parameter values. Next, for each set of fatigue
model parameter values, given the stimulation sequence of the fatigue
protocol and initial nonfatigued force model parameter values, the
forces produced in response to each train of each fatiguing protocol
(including the protocol used to determine that set of fatigue model
parameter values) were predicted using the force and fatigue models to
integrate forward (Fig. 3D).
Data Analysis
For each of the six sets of fatigue model parameter values
obtained (i.e., 1 from each fatigue protocol), we tested the ability of
the fatigue model to predict the force responses to all six fatigue
protocols, including the protocol used to parameterize the model. The
evaluation of the fatigue model was begun by comparing subjectively the
predicted with the calculated force model parameter values and by
comparing the predicted with the experimental force responses to each
stimulation train of the fatigue protocol (Figs. 4 and 5).
Then, the predicted and experimental peak force responses to each train
of the fatigue protocol were plotted (Figs.
6 and 7).
R2 values between the predicted and experimental
forces were then calculated to compare the peak forces produced by each
protocol. Next, the percent differences between the predicted and
experimental peak forces at the end of fatigue test were compared. This
measurement was included because R2 is not
sensitive to an offset between the predicted and experimental fatigue
profiles. Finally, we compared the predicted with the experimental
percent decline in forces produced by each fatigue protocol. Paired
t-tests were used to compare the predicted with the
experimental percent decline in forces. Comparisons were significant if
P
0.05.

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Fig. 4.
Example of predicted forces to VFT50-CFT100 combination
(V50-C100) fatigue protocol when the fatigue model was parameterized by
the V50-C100 fatigue protocol for a typical subject. Force model
parameter values were calculated (individual data points in
A-C), and then fatigue model parameter values were
identified (see values for A,
R0, and
 c in A-C). The
fat for this subject was 46.9 s. After the fatigue
model was parameterized, force model parameter values (solid lines in
A-C) and forces (D) were predicted given
only initial force model parameter values
(Arest = 11.9, R0,rest = 0.12, c,rest = 20) and the stimulation protocol (V50-C100).
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Fig. 5.
Example of predicted forces to DFT155 fatigue protocol
when the fatigue model was parameterized by the V50-C100 fatigue
protocol for a typical subject (same subject as in Fig. 4). Force model
parameter values were calculated (individual data points in
A-C). After the fatigue model was parameterized as
described in Fig. 4, force model parameter values (solid lines in
A-C) and forces (D) were predicted given
only initial force model parameter values
(Arest = 11.0, R0,rest = 0.45, c,rest = 20) and the stimulation protocol (DFT155).
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Fig. 6.
Experimental and predicted peak forces for a typical
subject (same subject as in Fig. 4). The fatigue model was
parameterized using data collected when the muscle was fatigued by the
V50-C100 fatigue protocol (Fig. 4). The peak forces produced in
response to the V50-C100 (A), CFT25 (B), CFT66
(C), CFT100 (D), VFT80 (E), and DFT155
(F) fatigue protocols were plotted. Although V50-C100 trains
were included within each protocol, responses to these trains are not
plotted.
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Fig. 7.
Group (n = 6) R2 values
(means ± SE) between experimental and predicted peak forces in
response to each train for each fatigue protocol when the fatigue
modeled was parameterized with force responses to the CFT25
(A), CFT66 (B), CFT100 (C), V50-C100
(D), VFT80 (E), and DFT155 (F) fatigue
protocols. Arrows, model's prediction for the fatigue protocol that
was used to parameterize the model.
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RESULTS |
When the fatigue model was parameterized with the V50-C100
protocol, it accurately predicted the changes in force model parameter A and
c (Figs. 4 and 5) when the muscles were
fatigued by use of a wide range of fatigue protocols. However, although
the data showed that R0 appeared to change in a
sigmoidal fashion, the model predicted that R0
changed exponentially. The fatigue model, parameterized with the
V50-C100 protocol, generally predicted the force responses quite well,
except for the beginning of the CFT25 and DFT155 protocols (Fig. 6).
When the fatigue model was used to predict the force responses to the
same protocol that was used to parameterize the fatigue model (e.g.,
predict the force responses to CFT25 protocol when the model was
parameterized by the CFT25 protocol), all the R2
values between the predicted and experimental peak forces were >0.9,
except for the CFT100 (R2 = 0.84) and
DFT155 protocols (R2 = 0.78; Fig. 7).
Similarly, all the predicted peak forces at the end of fatigue testing
were within 10% of the experimental peak forces, except for the CFT25
protocol (Fig. 8). The smallest percent
differences were with the CFT100 and V50-C100 protocols (~5%).

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Fig. 8.
Group (n = 6) percent differences (means ± SE) between experimental and predicted peak forces at the end of
fatigue protocol when the fatigue modeled was parameterized with force
responses to the CFT25 (A), CFT66 (B), CFT100
(C), V50-C100 (D), VFT80 (E), and
DFT155 (F) fatigue protocols. Arrows, model's prediction
for the fatigue protocol that was used to parameterize the model.
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When the fatigue model was used to predict force responses to the
protocols other than that used to parameterize the fatigue model (e.g.,
predict force responses to CFT100, CFT66, V50-C100, VFT80, and DFT155
protocols when the model was parameterized by the CFT25 protocol), the
model generally accounted for >80% variance of the experimental
forces for most protocols (Fig. 7). The fatigue model, however, did not
do so well in predicting the force responses to the DFT155 protocols
(R2 = 0.52-0.79). The differences
between the predicted and experimental peak forces at the end of the
fatigue test were more variable than the R2
data, with results that ranged from 6% to 32% (Fig. 8). Overall, when
the model was parameterized with the V50-C100 protocol, the fatigue
model produced the smallest percent differences (9%).
Because the V50-C100 protocol was best at parameterizing the fatigue
model among the six protocols tested, it was used to test the model's
ability to predict the percent decline in peak forces during the
fatigue test. When the V50-C100 protocol was used to parameterize the
fatigue model, the predicted percent declines of the peak forces were
within 7% of the experimental peak forces for all the fatigue
protocols except the DFT155 protocol (46%) and the C100 trains in the
V50-C100 protocol (15%). Significant difference was observed only for
the DFT155 protocol (Fig. 9).

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Fig. 9.
Group (n = 6) percent decline (mean ± SE) in peak forces of fatigue-producing trains between experimental
and predicted data. Predicted data were obtained by the fatigue model
when the model was parameterized using the V50-C100 protocol. Paired
tests were used to compare predicted and experimental percent declines.
*Comparison was significant, P 0.05.
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DISCUSSION |
The fatigue model presented in this study was tested using data
from human quadriceps femoris muscles with protocols consisting of
trains with a wide range of frequencies (10-40 Hz) and activation patterns (CFT, VFT, and DFT). In general, subjective (Figs. 4-6) and objective evaluations (Figs. 7-9) suggested that the fatigue model predicted well the force responses to fatigue protocols with
different stimulation patterns on different days.
Among the six protocols tested, the V50-C100 protocol was the best
protocol to parameterize the fatigue model. We believe this was because
this protocol gave the model the most information about changes in
force. The V50-C100 protocol contained 75 pairs of the V50-C100
combination, giving the fatigue model 76 sets of force model parameter
values to model. In contrast, there are only 11 pairs of the V50-C100
combination in the other protocols.
For the three force model parameters that were allowed to change during
fatigue, the model fitted and predicted the changes in A and
c well (Figs. 4 and 5). However, the change in
R0 was not a simple exponential function of
time, as we assumed in the fatigue model (Eq. 4).
R0 characterizes the magnitude of the nonlinear summation in Ca2+ produced by subsequent stimuli (for
additional details see Ref. 15). The over- or underestimation of
R0 by the model has a greater effect on the
force responses to those stimulation trains containing closely spaced
pulses, such as the CFT25, VFT80, and DFT155. As shown in Figs. 4 and
5, the model overestimated R0 in the beginning of the fatigue protocol, producing an increase in the predicted forces
at the beginning of the fatigue tests for the VFT50 in the VFT50-CFT100
protocol and the DFT155 protocol (Fig. 6). This increase in force
predicted by the model was most pronounced in the DFT155 protocol,
because this pattern contained three doublets. In addition, we also
observed that the fatigue model overestimated the force response to the
first train in the CFT25 protocol and underestimated the forces to the
first trains in the VFT80 and DFT155 protocols (Fig. 6). Because the
fatigue model used the session's nonfatigued force model parameter
values when the initial forces for that session were predicted, the
over- or underestimation seen at the onset of the fatigue protocol was
due to the inaccuracy of predictions in the force model. Modification
of the force model and a more sophisticated modeling of
R0 in the fatigue model, such as adding another
differential equation to allow a second (shorter) time constant to
capture the changes in R0 at the beginning of
fatigue, may be necessary to obtain better predictive ability in
high-frequency trains or those containing doublets.
Previous studies on modeling muscle fatigue have not had stimulation
frequency or pattern as one of the inputs and, therefore, were not
designed to identify stimulation patterns to reduce fatigue during FES
(11, 26, 28). The fatigue model presented in this study
was governed by only four free parameters and was able to predict the
forces of human quadriceps femoris muscles during repetitive activation
with different fatigue protocols on different days, given only the
stimulation protocol and the initial conditions of the muscle. When the
model was parameterized by the best protocol (V50-C100), on average, it
produced an R2 of 0.90 and a percent difference
of 9% between the predicted and experimental peak forces (Figs. 7 and
8). Because the within-subject experimental variance in the fatigue
profiles was 7% (R2 = 0.93) and the
percent difference in experimental forces at the end of the fatigue
testing was 9% (see Subjects), this fatigue model was
considered successful. In addition, the fatigue model also successfully
predicted the effect of stimulation frequency and pattern on fatigue.
Consistent with the experimental data, the model predicted that the
CFT25 protocol would produce the most fatigue among the six protocols
tested (Fig. 9). Also, among the three CFTs (CFT25, CFT66, and CFT100),
the model predicted that the shorter the IPI, the greater the amount of
fatigue; this was the same trend shown by the experimental data.
Finally, for the three protocols that had the same mean frequency
(CFT66, VFT80, and DFT155), the predicted and experimental data showed
that the DFT was the least fatiguing train type.
In conclusion, this study is the first to develop a mathematical model
that predicts isometric forces from human muscles during repetitive
activation by different activation protocols. Unlike previous
approaches to modeling muscle fatigue, we modeled the changes in our
force model parameter values during fatigue, which led to the changes
in the forces. The same approach could be applied to modeling fatigue
during nonisometric muscle contractions once a successful nonisometric
force model is developed. This model, although simple, appears very
promising in predicting isometric forces across days, stimulation
protocols, and levels of fatigue. Muscle fatigue depends on many
factors, including stimulation parameters such as frequency, duty
cycle, and activation patterns (2, 8, 21). We envision
that mathematical models similar to that presented in this study could
help elucidate the mechanisms of fatigue and facilitate the
identification of stimulation patterns that minimize fatigue.
 |
ACKNOWLEDGEMENTS |
We thank Dr. William Rose for helpful comments concerning an
earlier version of the manuscript.
 |
FOOTNOTES |
This study was supported by National Institute of Child Health and
Human Development Grant HD-36797 and the Office of Graduate Studies of
the University of Delaware.
Address for reprint requests and other correspondence: S. A. Binder-Macleod, Dept. of Physical Therapy, 301 McKinly
Laboratory, University of Delaware, Newark, DE 19716 (E-mail:
sbinder{at}udel.edu).
The costs of publication of this
article were defrayed in part by the
payment of page charges. The article
must therefore be hereby marked
"advertisement"
in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
Received 21 April 2000; accepted in final form 22 May 2000.
 |
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