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The Journal of Neuroscience, October 15, 1998, 18(20):8402-8416
Directional Tuning of Single Motor Units
Uta
Herrmann and
Martha
Flanders
Neuroscience Graduate Program, University of Minnesota,
Minneapolis, Minnesota 55455
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ABSTRACT |
The directional activity of whole muscles has been shown to be
broadly and often multimodally tuned, raising the question of how this
tuning is subserved at the level of single motor units (SMUs).
Previously defined rules of SMU activation would predict that units of
the same muscle (or at least of the same neuromuscular compartment) are
activated homogeneously with activity peaks in the same "best"
direction(s). In the present study, the best directions of SMUs in
human biceps (both heads) and deltoid (anterior, medial, and posterior
portions) were determined by measuring the firing rate and threshold
force of units for recruitment during isometric force ramps in
many different directions. For all muscles studied, neighboring motor
units could have significantly different best directions, suggesting
that each muscle receives multiple directional commands. Furthermore,
17% of the units sampled clearly had a second-best direction,
consistent with a convergence of different directional commands onto
the same motoneuron. The best directions of the units changed gradually
with location in the muscle. Best directions did not cluster into
separate groups, thus, not supporting the existence of clearly
distinguished neuromuscular compartments. Instead, the results reveal a
more gradually distributed activation of the biceps and deltoid
motoneuron pools. A model is proposed in which the central control
mechanism optimizes the fulfillment of the continuously changing
directional force requirements of a movement by gradually recruiting
and derecruiting those units ideally suited for the production of the
required force vector at any given time.
Key words:
motor control; arm movement; reaching; single motor unit; directional tuning; motoneurons
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INTRODUCTION |
The complex task of coordinating the
activation of the appropriate fibers in a given muscle appears, in many
instances, to be fulfilled automatically. Assuming a "common drive"
to all motoneurons (MNs) of each muscle (DeLuca and Erim, 1994 ; Iyer et
al., 1994 ), recruitment order during an augmenting contraction may be
determined by MN size alone (Henneman et al., 1965 ). Because of the
orderly relation between the size of an MN and the mechanical and
biochemical properties of its target muscle fibers (Burke, 1967 ), such
size-ordered recruitment results in a smoothly graded force rise with
minimal fatigue development. Thus, certain aspects of a motor act
appear to be optimized requiring only the most parsimonious neural
circuitry. Unfortunately, however, this elegant functional simplicity
of the size principle/common drive concept is not without drawbacks. When applied to human arm movements it would predict rigidity within a
system whose flexibility is, in fact, amazing. The directional aspects
of everyday reaching movements are manifold, requiring a versatility
that might make it necessary to allow for task-specific, differential
activation of different subunits of the same muscle, resulting in
deviations from a fixed recruitment order.
The results of several studies by Gielen, Denier van der Gon, and
colleagues support the idea of task-dependent recruitment of the
single motor units (SMUs) involved in elbow flexion-extension and
pronation-supination. In the long head of biceps brachii, terHaar Romeny et al. (1984) found units activated differentially in
supination, flexion, or a combination of the two in the lateral, medial, and central part of the muscle, respectively. In a study investigating SMU recruitment patterns in six human elbow muscles, van
Zuylen et al. (1988) found evidence for the existence of subpopulations of SMUs in all but one of the muscles. One example of such
differentiated input to SMUs of the same muscle may consist in a
reciprocal inhibition between only parts of the MN pool of antagonistic
muscles: Jongen et al. (1989) demonstrated that the relative activation
of parts of the same muscle differed depending on whether the muscle
was activated with or without the cocontraction of its antagonist.
One would thus predict that although the activity of whole muscles
involved in a reaching task exhibits broad and often multimodal directional tuning (Buchanan et al., 1986 ; Flanders and Soechting, 1990 ), the SMUs of these muscles would be more narrowly tuned, with
subpopulations of SMUs showing activity peaks for different directions.
This has been confirmed by Theeuwen et al. (1994) for the bimodally
tuned anterior deltoid (AD), a muscle whose two best directions closely
corresponded to the activity peaks of two unimodally tuned
subpopulations of SMUs. However, these investigators did not attempt to
discern differences in the directional tuning of various SMUs within
the same AD subpopulation or within other broadly tuned muscles. Thus,
the issue of directional preferences and subpopulations of SMUs in
proximal arm muscles requires further examination.
The present study examines the directional tuning properties of SMUs in
human biceps brachii (long and short heads) and deltoid (anterior,
medial, and posterior portions). We will present results indicating
that the various SMUs within each portion of each muscle have different
best directions. Directional preferences varied continuously with
location in the muscle rather than clustering into distinct
subpopulations located in the different heads or portions of the
muscles. Furthermore, we found evidence for multiple directional
preferences at a single location. This suggests that the activation of
these muscles is more distributed than might be explained by their
division into known anatomical compartments or discrete subpopulations
of motor units.
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MATERIALS AND METHODS |
Subjects
Data were collected from a total of 203 units in four adult
human subjects with no history of motor impairments. Subject A was a 6 ft 0 in (183 cm), 180 lb (81 kg) male; subject B was a 5 ft 9 in (175 cm), 130 lb (59 kg) female; subject C was a 5 ft 9 in (175 cm), 155 lb
(70 kg) male; and subject D was a 5 ft 10 in (178 cm), 140 lb (64 kg)
female. The protocol was approved by the Human Subjects Committee of
the University of Minnesota, and all subjects gave their informed
consent before participation in the study.
Experimental protocol
General. Subjects stood or sat with the upper arm
vertical, the elbow flexed 90° (so that the forearm was horizontal
and in a parasagittal plane), and the wrist neutral with regard to
pronation-supination. The right wrist was strapped into a brace
connected to a transducer measuring the forces exerted at the wrist
(see Fig. 4a). Forces in various directions were produced by
combinations of elbow flexion-extension and various moments about the
rotational degrees of freedom of the shoulder. The brace rotated freely
about the vertical axis of the transducer (~2 cm proximal to the
wrist flexion-extension axis) so that it was impossible to produce an
isometric moment in this dimension.
Two-dimensional experiments. In the first set of
experiments, subjects produced ramp increases in isometric force in 20 different directions covering the sagittal plane (Fig.
1a, Up-Back plane) and
presented in random order while forces were recorded with a 2 df
force sensor (Measurement Systems, Inc., Fairfield, CT). A cursor
moving on an oscilloscope screen displayed the forces exerted at the
wrist together with the 20 numbered targets representing force
increases of equal magnitude in 20 different directions. The screen was
aligned with the subject's sagittal plane and placed so that the
subjects could comfortably view the cursor movements during the trials.
Before each trial the target number was announced. The subject then
moved the cursor into the center target zone by exerting enough force
to support the weight of the arm. When subjects indicated that they
were ready, the trial was initiated with a frequency-ramped computer
tone. The tone served as a cue for the subject to slowly and accurately
acquire the target and hold the cursor in a steady state at the target
for 2 sec. Data were acquired for 3.5 sec. For each unit, the magnitude
of the target force was set somewhere between 8 and 20 N depending on the strength of the subject and/or the recruitment threshold of the
unit to be studied.

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Figure 1.
a, Distribution of targets. First
set of experiments: subjects produced isometric forces in 20 different
directions covering the sagittal
(Up-Back) plane. Second set: subjects
produced forces in 54 different directions covering the sagittal
(Up-Back), horizontal
(Back-Out), and frontal
(Up-Out) planes. b,
Subject B, sagittal plane: 120 force traces (6 per direction) from four
different experiments. Force traces stay close to the sagittal plane,
especially those in the up and forward directions. c,
Typical force trace (I), unit record
(II), and unit raster
(III). Threshold force is marked in force trace
with a gray line. Close-up below unit trace shows
consistent shape and amplitude of the potential of this unit.
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Experiments were conducted in sets of ~100 trials. None of the units
recorded from was active over a range of >14 of the 20 directions.
Each of the 20 directions was tested at least once for unit activity.
After this, directions for which the unit had remained silent (except
for the directions immediately bordering the activation range of the
unit) were excluded from the experimental protocol. The remaining
directions were tested five times each. To avoid fatigue, subjects were
told to take breaks whenever they wished within a set, and intertrial
intervals were kept between 3 and 10 sec.
Three-dimensional experiments. In a second series of
experiments the set-up was expanded to include recordings during force ramps in the frontal and horizontal planes as well as the sagittal plane (Fig. 1a). Thus, subjects produced forces in 20 different directions in each of the three planes while forces and
moments were recorded with a 6 df force-torque sensor
(JR3 Inc., Woodland, CA). (Although the task
required only the 3 linear df, recordings from the rotational degrees
of freedom were used to cancel sensor cross-talk.) Two more
oscilloscopes were added to the set-up to provide the subject visual
feedback information concerning the forces in the frontal and
horizontal planes. The screens were aligned with the frontal and
horizontal planes and placed so they could be viewed comfortably by
subjects during the experiments. Trials followed the same procedure as
outlined above.
Experiments were conducted in sets of ~120 trials divided into six
blocks (two for each plane) of up to 20 different directions in each
plane. Directions with no unit activity were gradually excluded from
the protocol as described above. The remaining directions were tested
two or three times each.
Using only a 2 df force transducer in the first set of experiments made
it impossible for us to monitor whether subjects produced any forces
out of the sagittal plane. However, we did test for this possibility at
the start of the second experimental set in which a 6 df sensor was
used. Figure 1b depicts 120 force traces to targets in the
sagittal plane (six per direction) by subject B from four different
experimental sessions. The figure shows little deviation from the
sagittal plane, especially for the upward and forward directions [the
directions for which biceps (BI) units are best activated].
Analogous to previous results, some directions show more intertrial
variability than others (Buneo et al., 1995 ). It appears, however, that
when instructed to do so, subjects are able to produce forces that are
reasonably close to the sagittal plane.
Dynamic forces. At the end of two of the experiments in the
second series, after the directional tuning data for various deltoid units had been acquired for slow ramp forces, subject D was asked to
exert dynamic isometric pulses covering the range of directions in
which the units were active. The subject acquired the target in the
given direction rapidly and accurately before relaxing. Recordings
during a total of 140 pulses were obtained (80 in the first experiment,
60 in the second experiment).
Data acquisition and processing
In the first set of experiments [the two-dimensional (2D)
experiments], recordings were taken primarily from posterior deltoid (PD) and from BI. The border between posterior and medial deltoid and
between medial and anterior deltoid cannot be discerned reliably on the
skin surface. We initially sampled units from the posterior half of the
whole deltoid muscle, thus including part of medial deltoid. In subject
A we extended our sample to include units from almost the entire width
of deltoid, thus including several units in anterior deltoid. In the
second set of experiments [the three-dimensional (3D) experiments],
we extended the sampling for all subjects across the entire deltoid
muscle, including all of the posterior, medial, and anterior deltoid.
We did not return to biceps to examine the 3D tuning, nor did we modify
the apparatus to examine the recruitment of BI in
pronation-supination.
Surface EMG was recorded with small bipolar electrodes placed on the
belly of the muscle. The two electrodes were placed on a line running
with the length of the muscle, ~2 cm from each other. Surface EMG
signals were amplified and bandpass filtered (10-5000 Hz). Both force
and surface EMG data were digitized at 10 kHz. EMG levels at steady
state were computed by averaging across a 200 msec segment of rectified
EMG (Pellegrini and Flanders, 1996 ).
Single unit EMG was recorded with bipolar, Teflon-coated, fine-wire
electrodes (~25 µm bare diameter) inserted into the muscle with a
27 gauge hypodermic needle. The needle and wires were sterilized before
the experiment, and the skin was rubbed clean with alcohol before
insertion of the electrodes. Unit recordings were amplified, bandpass
filtered (100-5000 Hz or 100-10,000 Hz), viewed on an oscilloscope,
digitized (10 or 20 kHz), stored on magnetic disk, and backed up on
magneto-optical disk. Over the course of an experimental series,
recordings were made from 15-48 units per subject and muscle, such
that the different recording locations covered the whole width of each
muscle. The place of needle insertion was defined relative to
anatomical landmarks and its location was marked on a "map"
overlaid on the muscle using a transparency.
Data analysis
Unit identification. The activity of each unit was
identified off-line and marked in the unit recording using a
custom-written template-matching program. This program computed the
Pearson correlation coefficient (r) between a template of
the unit (selected from a trial with little noise) and the unit
recording at every point of the trace. The value of r
approached 1.0 for the parts of the trace that closely corresponded to
the template in shape and amplitude, whereas in our experience the
maximum value of r between template and background noise was
between 0.3 and 0.6. Each time the value exceeded a cut-off criterion
(which depending on the background noise level was between 0.7 and
0.9), the program "recognized" this part of the record as the unit
potential and marked it in a raster of the trace (Fig. 1c).
Trials in which a unit started firing during the force ramp but quit
completely at a later point were excluded from the analysis.
Relation between firing rate and recruitment threshold: the
model. In the first series of experiments, whenever possible, threshold force for recruitment and firing rate at steady state were
determined for each unit in each direction (it was not possible to
measure firing frequency when the recruitment of additional units
obscured the unit waveform). Firing frequency was graphed against
direction in polar coordinates (Fig.
2a). In such a polar plot, the
direction of force at the wrist is given by the direction of the line
connecting the origin to a data point (or to a point on the circle in
Fig. 2a). The distance of the data point from the origin
represents the firing frequency of the unit in this direction.
Analogous to the analysis used by Flanders and Soechting (1990) for
surface EMG activity, cosine functions with a threshold nonlinearity
were fit to the frequency data according to the formula:
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(1)
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where c is a constant offset, a is a
constant scaling the cosine function, F is force
magnitude, 0 is the best direction of the unit defined
as the center of the cosine peak, and is the current force
direction.

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Figure 2.
Hypothetical, perfectly cosine-tuned unit with its
best direction (arrows) straight up. a,
Cosine-tuned firing frequency. In the right triangle, firing rate
f is equal to the cosine of the angle .
b, Inversely cosine-tuned threshold force. In the right
triangle the threshold force t is equal to 1/cos .
c, Relation between threshold force and firing
frequency. Threshold force is minimal for directions in which firing
frequency is maximal and vice versa. d, The fact that
threshold data in 2D can be fit by a line is consistent with a model in
which 3D threshold data fall on a plane, and the best direction of the
unit is given by the direction of shortest (i.e., perpendicular)
distance between the plane and the origin (straight up
arrow).
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Figure 2a depicts hypothetical unit activity that is
perfectly cosine tuned with its best direction 0 being
straight up. For forces in this direction, the unit fires at maximum
frequency; as the force direction deviates from this best direction,
firing frequency (the length of the dashed lines) decreases until the unit is silent at angles 90° away from 0.
Compared to the steady-state firing frequency, the level of threshold
force should show the opposite relation to force direction: for its
best direction 0, the unit should be recruited
most readily, i.e., the force level at recruitment should be a minimum
(Fig. 2, compare a,b). As force direction
deviates from 0, the magnitude of threshold force (Fig.
2b, the length of the dashed lines) should increase until for force directions 90° from 0, the
unit is silent and threshold force is infinite. This relation of
threshold force to force direction is fulfilled if threshold force data fall on a straight line when plotted in x, y
force coordinates. That this is, in fact, the case has been
demonstrated by Theeuwen et al. (1994) using SMU threshold data from
seven human shoulder and elbow muscles. In our model, threshold force
(during the ramp) and firing frequency (at steady state) are thus
inversely related. In the right triangles in Figure 2, a and
b, firing frequency (f) is equal to
the cosine of the angle between the best and the current force
direction of the unit, whereas threshold force (t) is equal
to 1.0 divided by the cosine of the same angle .
Based on the findings of Monster and Chan (1977) , which show that SMUs
are recruited at a characteristic frequency and increase their firing
rate as force rises, we suggest the model outlined in Figure
2c. According to this model, a unit starts firing at its
characteristic recruitment frequency [here 7 impulses per second
(ips)] when a threshold level of MN activation is reached. The
horizontal parallel lines represent lines of constant activation level
and, thus, of constant firing frequency. During a force ramp,
activation level rises along the dashed lines with a slope depending on
force direction. For forces in the best direction of the unit, the
slope is maximal, and the force magnitude necessary to reach threshold
activation is a minimum, whereas for other directions, the slope is
lower and threshold force is higher. Beyond recruitment, activation
level (and thus firing frequency) still rises with the same slope, and
the final firing frequency reached for a given direction is given by a
cosine function.
The fact that threshold data in 2D can be fit by a line is consistent
with a model in which 3D threshold data fall on a plane (Fig.
2d) and the best direction of the unit is given by the
direction of the shortest (i.e., perpendicular) distance between the
plane and the origin (Fig. 2d, straight-up
arrow). Analogous to the circular fit to the polar
coordinates of firing frequency in the 2D model, firing frequency in 3D
would follow a sphere.
Relation between firing rate and recruitment threshold: fit to
the data. We plotted 2D threshold data as the x and
y components of the force at which a unit first was active
during the ramp. We then found the best direction of each unit by
fitting a regression line to the data. Only units whose threshold data
could be well fit (p < 0.05) by a straight line
were included in our final analysis.
In some cases the data were better fit by two lines with different
slopes, indicating that the unit would be more appropriately described
as having two best directions. To determine which of the data points
belonged to each line, the data were grouped according to parameters
found by a nonlinear least square estimation method in a standard
statistical software package (Systat, Evanston, IL). The program fit
the following model to the data:
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(2)
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where [X > Break] returns 1.0 if
X > Break is true and 0.0 if it is false.
Thus, Y was related to the X values below the break point with a slope of b1. Above the break
point, Y was then related to X with a slope of
(b1 + b2).
Whereas this method worked well for BI data, for most bidirectional
deltoid units threshold data for forces in the sagittal plane seemed to
fall onto two parallel lines (see Fig. 9, unit 9.3). This created a discontinuous or multivalued
function that could not be split according to the equation above.
Therefore, these data sets were instead split by a 45° line with
negative slope through the origin, which essentially divided the
data points into those for upward-forward directions and those
for downward-backward directions.
The "likelihood-ratio test" for regression parameters was used to
determine whether the fit of the model was significantly (p < 0.05) improved by adding a second line
(Johnson and Wichern, 1982 ). If a two-line model could be fit to the
threshold data of a unit, the frequency data were split up according to
the same break point found in the threshold data, and the two groups
were fit with separate cosine functions. Whether using a two-peak model was justified was again determined with the likelihood-ratio test.
Using the confidence limits on the regression coefficients, we tested
(in 45 units) whether the best directions found with the cosine fit to
the frequency data corresponded to those found with the linear
regression analysis on the threshold data. Because we did not find a
significant difference between these two measures of best direction in
any of the units, we limited most of our analysis to the linear
regression statistics of the threshold data. Employing the regression
line fit to the threshold data made it possible to use standard linear
regression statistics (t test on slopes) to test if the best
directions of two units of the same muscle differed significantly
(i.e., at the p < 0.05 level). Thus, most of the
statistical testing was based on the linear parameters of 2D or 3D
forces.
For the data obtained in the 3D experiments, threshold data were split
into three groups according to the plane of the target force (Fig.
1a), and each group was fit separately with 2D regression lines. In addition, data from trials in all three planes were combined
in 3D and fit by a plane using multiple linear regression analysis
(Fig. 2d). The best direction of a unit was then given by
the line that was normal to the plane and passed through the origin of
the 3D plot.
For units whose 2D plots indicated that they might have two preferred
directions, the entire set of 3D threshold data were split into two
groups. Data from trials with force ramps in the frontal and horizontal
planes were split according to the break points found in each plane
with the least-square estimation method described above. Data from
trials in the sagittal plane were split by the line of intersection
between the sagittal plane and the plane passing through the origin and
the two break points found in the frontal and horizontal planes. The
two groups of data were then fit with one plane each. Whether the
two-plane model significantly improved the fit was determined with the
likelihood-ratio test.
Cluster analysis. Cluster analyses (Systat, nonhierarchical
K-means splitting method) were performed on the distribution of best
directions of the biceps unit sample to divide the data into groups of
units with similar best directions. After the data were broken into
groups, group membership was examined to determine whether units with
similar best directions were located in similar portions of the
muscle.
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RESULTS |
The goal of the present study was to characterize how the
directional activities of SMUs in one muscle combine to account for the
observed directional pattern of whole muscle activation. Using surface
EMG data, in Figure 3 we show the
directional activity of some of the muscles examined in this study, BI
(both heads) and PD, during isometric forces in the sagittal plane. BI
was broadly tuned across the up-backward and up-forward directions. PD on the other hand, exhibited activity peaks in opposite directions, down-backward and up-forward, such that its activity was best fit by
a double cosine function. By characterizing and comparing the
directional activity of many SMUs in BI and deltoid we will show that
the broad and/or bimodal tuning observed for these muscles arises
because units within the same muscle have a range of significantly different preferred directions.

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Figure 3.
Directional activity tuning plots for whole
muscles as measured with surface EMG. BI activity is broadly tuned and
can be fit by a single cosine function. Data from PD can be best fit by
two cosine functions with nearly opposite peaks (two
circles with two arrows). Partially because of
the sampling bias inherent in multiunit surface EMG, it is not clear
exactly how these tuning curves correspond to the tuning of the
individual motor units. All data are from subject B.
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Threshold lines and recruitment reversal
Using data from a BI motor unit, Figure
4 illustrates how threshold force at
recruitment and firing rate at steady state vary systematically with
the direction of force at the wrist. Directions of forces in the
sagittal plane were denoted by positive and negative numbers (for
forward and backward directions, as indicated in Fig. 4b)
and will be referred to by these numbers in the following sections. All
unit traces (three per force direction) were aligned with force onset
(Fig. 4b,c, arrowheads); all were
recorded during the same experiment. One unit could be easily
distinguished from others by the large amplitude of its waveform. This
unit started firing at a minimum force level for directions 0 and +1.
As force direction moved forward from +1 to +3 and backward from 0 to
2, the force levels at recruitment became progressively higher,
whereas firing rate at steady state generally decreased. Figure
4d shows that the threshold force data plotted in
y/x coordinates could be well fit by a line whose
perpendicular (arrow) pointed in a direction closely
corresponding to the direction in which threshold force was at a
minimum (Fig. 4b, direction +1). The majority of BI and
deltoid units examined in the 2D experiments exhibited this type of
recruitment pattern, such that the threshold force data of 91% of the
units could be fit by straight lines (p < 0.05).

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Figure 4.
Threshold force at recruitment and firing rate at
steady state vary systematically with the direction of force at the
wrist. a, Posture of the arm (side view) during the
experiments. b, All unit recordings are aligned with
force rise onset (marked by arrowhead below traces) and
were recorded from one BI electrode during the same experiment. Three
trials are shown for each direction; the presentation order was
randomized during the experiment. As force direction changes from +1 to
+3, and from 0 to 2, the force levels at recruitment become
progressively higher, whereas firing rate at steady state decreases.
c, Typical force trajectory with onset of force rise
marked by the arrowhead. The vertical scale
bar represents 20 N. d, Threshold force data
plotted in y/x coordinates are fit by a
line whose perpendicular (arrow) points in the best
direction of the unit.
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Significant differences in best direction were sometimes found between
units recorded on the same electrode, in which case recruitment
reversal could be observed across trials with different force
directions. Figure 5a shows
that the best directions for unit 5.1 (i.e., Fig. 5, unit 1) and unit
5.2 differed by 13°. The best directions were +31.9° (±5.7°) for
unit 5.1, and +18.7° (±6.5°) for unit 5.2. Therefore, as shown in
Figure 5b, the order of recruitment for these units changed
with force direction, such that for the force ramp in direction 3 (closer to the best direction of unit 1), unit 1 was recruited before
unit 2, whereas for the force ramp in direction 1 (closer to the best
direction of unit 2), unit 2 was recruited first. Considering the
series of 2D experiments (BI and deltoid), significant differences in
best direction (t test on slopes, p < 0.05)
were found in six pairs of units recorded on the same electrode and in
nine pairs of units recorded on different electrodes but in the same
experiment. These pairs of significantly different units found in BI
are marked in Table 1. We can thus rule
out the possibility that differences in best direction between units
found in the 2D experiments are caused by day-to-day variability in the
levels of force outside the sagittal plane, because these differences
are also observed between unit recordings obtained under identical
force conditions.

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Figure 5.
Recruitment reversal with force direction. Units 1 and 2 found on the same electrode had different preferred directions
(arrows) as shown in a and were recruited
in a different order depending on the force direction.
b, For a force ramp in an up-forward direction, unit 1 was recruited before unit 2. For the force ramp in an up-backward
direction, unit 2 was recruited before unit 1.
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Table 1.
List of all biceps units, their best directions (degrees)
as found from the threshold line and frequency cosine fit (where
available), and their minimum threshold force magnitudes as found from
the threshold line
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Best directions of biceps motor units
Directional tuning of BI units
As mentioned in Materials and Methods, firing frequency and
threshold data were never found to predict a significantly different best direction for a given unit. The best directions obtained from the
threshold line fit were then compared among different SMUs in BI and
were found to differ significantly. Figure
6 shows three examples of units with
obvious differences between their directional tuning curves. For unit
6.1, both firing rate and threshold data yielded a best direction that
was up and slightly backward. However, unit 6.2 (found in BI of the
same subject) exhibited activity whose best direction (up-forward)
differed from that of unit 6.1 by 28° (t test,
p < 0.001). Significant differences in best direction
between units of BI were found in all subjects, and for unimodally
tuned units, best directions covered a range of 32, 39, and 40° in
subjects A, B, and C, respectively (Table 1).

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Figure 6.
Threshold lines and frequency data for units in
biceps. Best directions as found from the threshold line or the cosine
fit are marked by arrows. Units 1 and 2 had
significantly different preferred directions. Unit 3 showed more than
one preferred direction. Action potential waveforms for unit 3 are
shown for trials in the two lobes of activation. All data are from
subject B. Bimodally tuned activity was seen in 29% of the biceps
units pooled across all subjects.
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The directional tuning of the units 6.1 and 6.2 described above
conformed to the predictions of the model suggested in Figure 2:
threshold force and firing frequency varied as a simple function of
force direction such that data were best fit by a single line and a
single cosine peak. The slope of this line (and the angular location of
the cosine peak), however, was significantly different for different
units. It would appear from these findings that the broad (and possibly
bimodal) tuning of the BI is accounted for by the combined activity of
unimodally tuned SMUs with different best directions. Consider,
however, the recruitment pattern of unit 6.3. The direction of lowest
threshold force was up-forward. As force direction changed toward
up-backward directions, threshold force initially increased, reached a
(local) maximum for upward directions, but then decreased again and
reached a second local minimum. Firing frequency varied in the reverse
manner, reaching peaks for up-forward directions and up-backward
directions, with a trough for forces directed upward. Threshold force
data for this unit clearly could not be well fit by a single line, and a two-line model significantly improved the fit. A two-peak cosine function improved the fit to the frequency data significantly. It thus
appears that this unit has two preferred directions: up-forward and
up-backward. Such bimodally tuned BI units were found in all subjects
(n = 16, 29%). The range of values representing the
angular difference between first- and second-best directions was
45-98, 30-70, and 72-79° in subjects A, B, and C,
respectively.
Correlation between directional tuning and recording location
Units were sampled from both the long and the short head of BI.
These two parts of the muscle share a common tendon at the elbow but
have different attachments at the shoulder joint and might, therefore,
be expected to be activated differently for different force directions.
This might be reflected in the best directions of their SMUs. Because
we inserted most electrodes near the belly of biceps, the two heads
could not be definitely distinguished for the midrange of electrode
placements. We, therefore, report recording location (as marked for all
subjects on the muscle map in Fig.
7c) on a continuum from medial
(toward the short head) to lateral (toward the long head).

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Figure 7.
Relation between the best direction of a unit and
its location in BI. a, Best directions as found from the
threshold line fit plotted against location in the muscle for each
individual subject. The two preferred directions of a bidirectional
unit are marked with a star for the best direction and
an open circle for the second-best direction. Regressing
only the best direction (for unimodally and bimodally tuned units) on
location in the muscle yielded a significant correlation in subject B
only. b, Pooling data from all subjects by normalizing
recording location yielded a significant correlation between best
direction and location (p < 0.005). This
relation suggests that units located laterally and medially are best
activated for upward and up-forward forces, respectively. (For
simplicity, only the best direction is shown for each unit in the first
plot. In the second plot, the second-best directions are included.)
c, Map of biceps with recording sites in all subjects.
Sites of electrode insertion for a particular subject are marked with a
corresponding letter.
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In Figure 7a the best direction as found from the threshold
line fit is plotted against the location of the recording electrode for
a given unit for each subject. The two preferred directions of a
bidirectional unit are marked with a star for the best direction and an
open circle for the second-best direction. Regressing only the best
direction (for unimodally and bimodally tuned units) on location in the
muscle yielded a significant correlation in subject B only. In the plot
one can see a slight tendency for lateral (long head) units to be
activated best for up and slightly backward directions, whereas medial
(short head) units are activated for up and slightly forward
directions. This slight trend can be seen in the two other subjects
also but failed the tests for significance.
Normalizing location in the muscle and pooling data from all subjects
yielded a significant correlation (p < 0.01)
between best direction and location. For simplicity, the first plot in Figure 7b only includes best directions. In the second plot,
the second-best direction of bidirectional units (open
circles) is also included. In the first plot, one can see
that, with a few exceptions, the first-best directions generally
appeared to fall close to the line. In contrast, the second plot shows
that the second-best directions were usually found at the extremes of
the range. We conclude from the pooled data that there was a gradual location-dependent shift in first-best direction, and a wide range of
first- and second-best directions (77° for best directions and 154°
for first- and second-best directions).
Cluster analysis
If the BI MN pool receives only a limited number of different
directional commands, the best directions of BI SMUs should cluster
into a limited number of distinct groups. To test this hypothesis we
performed a cluster analysis on the estimates of the best directions of
the units. When data from all subjects were pooled, the distribution
could be divided into three groups corresponding to up-backward,
upward, and up-forward directions. Figure
8a shows the histogram (with
bar width of 18°, which was the angular separation between
directions) of the best directions of the units for the pooled data.
Superimposed in gray on the histogram is the more continuous
distribution (bin widths of 1°) of best directions. Separations
between groups are marked by the dashed lines. Visual examination of
the histogram suggests, however, that the distribution can be
characterized as having long tails rather than distinct peaks as would
be expected from a distribution with several clusters. In the second
plot of Figure 8a we, therefore, examined whether members of
the three groups are restricted to certain locations in the muscle.
Members of each group are marked with the number of the respective
group. This plot shows that, in general, members of each group can be
found anywhere in the muscle. There is a slight tendency for units in
groups 2 and 3 to be found toward the long and short head,
respectively. However, the separations are not as clear-cut as would be
expected from a compartmentalized muscle.

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Figure 8.
Distribution of best directions of units in BI.
Bars of histograms denote bins of 18°, the angular
separation between experimental targets. Superimposed on one histogram
is the "continuous" (bin width of 1°) distributions of best
directions. a, Distribution of best directions as found
from the threshold line. Data are pooled from all subjects and include
only the best direction. Three clusters were found as marked in the
histogram by horizontal, dashed lines.
The second plot shows the distribution of units of each group in the
muscle. Members of a group were not constrained to a specific area in
BI. b, Distribution of best directions (pooled data) as
found from the direction of minimum threshold force. Note the wider
range of best directions when compared with that of
a.
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The lack of consistent and convincing clustering might have arisen from
an aspect of our analysis that might have introduced a central tendency
into the distribution. Although the recruitment pattern of some units
suggested the existence of a second preferred direction, a two-line
model did not significantly improve the fit to the data (see, for
example, unit 6.1). Thus, the unit would have been classified as
unimodally tuned, and one threshold line would have been fit to all
data points. The true best directions for such units might actually be
at more extreme points in the range of best directions and might
actually cluster into different groups. An estimate of best direction
from the threshold data that would be resistant to this distortion
toward a central value is the direction (i.e., one of the 20 directions
used in the experiment) in which average threshold force is a minimum.
Therefore, we repeated the cluster analysis with this more discrete
estimate of the best directions of the units. A histogram of the pooled
data is shown in Figure 8b. As expected, the range of best
directions obtained with this method (144°) was substantially larger
than the range obtained from the perpendicular directions to the
regression lines. (The range was 108, 72, and 144° for subjects A, B,
and C, respectively.) However, when splitting the distribution into 2, 3, or 4 groups by the means of cluster analysis, members of each group
could be found anywhere in the muscle, thus, not providing evidence for
a compartmentalized organization.
We also examined the combined distribution of first- and second-best
directions (obtained from the threshold lines) and again found little
evidence for compartmentalization. Thus, we conclude that the
distribution of preferred directions is continuous over its wide range.
Instead of clustering into distinct compartments, diverse directional
inputs appear to be widely distributed across the width of the
muscle.
Variations in threshold magnitude
It is possible that SMUs in BI are regionalized and/or
differentially activated according to histochemical fiber type as shown for cat hindlimb muscle (Chanaud et al., 1991b ). In this case (because
histochemical fiber type is correlated with MN soma size and,
therefore, with recruitment threshold; Burke, 1967 ) the force magnitude
at recruitment would depend on the location of the unit in BI and/or on
its best direction. We thus tested whether threshold magnitude varied
systematically with the preferred direction of a unit or its location
in BI. Of the six tests performed, the only significant correlation was
obtained between threshold magnitude and location in subject A
(p < 0.05), indicating that in this subject
high- and low-threshold units tended to be found toward the short head
and long head of BI, respectively. When data from all subjects were
pooled by normalizing unit location, no significant relation was found
between threshold magnitude and either best direction or location.
Thus, the results do not support the hypothesis of compartmentalized
fiber types in BI.
Best directions of deltoid motor units: 2D experiments
Considering only the sagittal plane, dramatic differences in
preferred directions were found across the various units in deltoid. Unit 9.1 (Fig. 9) was best activated for
down-backward forces. Unit 9.2, in contrast, was recruited best for
up-forward force directions and, thus, had a best direction in the
sagittal plane that differed by ~180° from that of unit 9.1.

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Figure 9.
Threshold lines for units in deltoid. Best
directions as found from the threshold line are marked by
arrows. Units 1 and 2 had nearly opposite preferred
directions. Units 3-5 showed more than one preferred direction. Action
potential waveforms for units 3-5 are shown for trials in the
different quadrants of activation.
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As in BI, we also found bimodally tuned units in deltoid. Their
threshold plots for the sagittal plane were perhaps more striking than
those of bidirectional units in BI, as the two areas of activation were
generally opposite one another. An example is shown with unit 9.3, a
bimodally tuned unit activated for forces both in the up-forward and
down-backward directions. Recruitment thresholds were well fit by two
nearly parallel lines indicating that the two best directions of this
unit were nearly opposite each other. The matching shapes of the unit
potentials shown for the two activation areas confirm that we were
indeed recording from the same unit. Units with this activation pattern
were found in all three subjects.
To exclude the possibility that units like unit 9.1 and 9.2 might have
a second-best direction with a higher threshold force level than the
level used in the experiment, we asked subjects at the end of the
experiment to produce force ramps to a maximal force level in the
up-forward (for unit 9.1) and down-backward directions (for unit
9.2). Because no activity of these units could be found during these
maximal force ramps, the units were classified as unimodally tuned.
Rare units like unit 9.4 (found only in subject A) had two preferred
directions, both within the range of the down-backward directions.
Equally rare units like 9.5 (found only in subject D) were activated
for up-forward and down-backward forces, much like unit 9.3, but had
an additional area of activation in the down-forward directions. No
line fits for this unit are shown in the figure because the assignment
of the data points in the additional activation area would have been
arbitrary: a third line could have been fit to all points in the lower
right quadrant, or they could have been assigned partly to the line
fits for the up-forward and back-down directions.
Because of the dramatic differences between best directions of units in
deltoid we classified our sample into three main groups: units with
best directions in the up-forward quadrant (e.g., unit 9.2, 22%,
n = 16), units with best directions in the
down-backward quadrant (e.g., unit 9.1, 56%, n = 41),
and those bidirectional units with best directions in both of these two
opposing quadrants (e.g., unit 9.3, 16%, n = 12).
Units with two best directions within one quadrant (such as unit 9.4)
and those that might have three best directions (unit 9.5) together
constituted only 6% (n = 4) of the units examined.
The ranges of best directions within the two groups of unimodally tuned
units were 57, 35, and 21° for the down-backward quadrant and 17, 27, and 21° for the up-forward quadrant for subjects A, B, and D,
respectively. In the description of the 3D experiments below, we will
explore whether units with similar best directions in the sagittal
plane are necessarily similar when their activity tuning in 3D is
considered.
Best directions of deltoid units in 3D
Although deltoid definitely contributes to shoulder
flexion- extension, the primary mechanical action of most of its
fibers is in abduction of the upper arm, i.e., in force directions
outside the sagittal plane (Buneo et al., 1997 ). Describing the
directional tuning of deltoid units only for forces within the sagittal
plane therefore provides an incomplete understanding of unit
activation. A threshold line in the sagittal plane lacks important
information about the orientation of the 3D threshold plane (Fig.
2d): for example, rotation of the threshold plane about any
axis lying within the sagittal plane would not change the orientation
of the threshold line in the sagittal plane. Therefore, units with threshold lines of similar orientation in the sagittal plane might, in
fact, have very different preferred directions when their recruitment pattern in 3D is considered. Similarly, the two threshold planes of
bidirectional units, such as unit 9.3, might be parallel yielding two
best directions 180° apart, or they might have a line of intersection such that the two best directions differ by <180°. Thus, to complete the description of directional SMU activity in deltoid, we recorded from units during forces in directions uniformly covering all three
planes (sagittal, horizontal, and frontal).
Unidirectional deltoid units
We found that the data from different deltoid units could be fit
by planes with widely divergent orientations. Each of the three columns
in Figure 10 represents threshold data
for one deltoid unit. The top three rows depict the threshold lines for
each of the three planes. These were derived only from trials with
force ramps within the respective plane. The bottom row shows the 3D plane fit to data from all trials. In 57 of the 59 units examined in
this set of experiments the plane fit to the threshold data was
significant (p < 0.05). In 45 of these units
the plane fit was significant at the p < 0.01 level.
The values of the correlation coefficient r for the
x, y, and z coordinates of the
threshold force levels ranged from 0.40 to 0.95. These results
illustrate that in consonance with the line fit to the 2D data,
threshold data in 3D can be fit by a plane.

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Figure 10.
Threshold lines and planes for deltoid units 1 (most posterior) to 3 (most anterior). The top three
rows show the threshold lines in each plane derived from trials
with force ramps within the respective plane. For the plots in the
bottom row, data from all trials were combined in 3D and
fit by a plane. The origin of the plot is located at the center of the
cube and is marked by the small sphere in the plot for
unit 2. The equations for the plane fits are as follows: unit 1, z = 2196.3 + 7.4x 2.8y; unit 2, z = 7628.3 3.4x 1.9y; unit 3, z = 1245.6 0.4x 0.3y, where x, y, and
z have positive values for outward, forward, and upward,
respectively. As location of the units changes from posterior to
anterior, the best direction appears to "jump" from down-backward
to up-forward in the sagittal plane; in the horizontal and frontal
planes, however, it appears to gradually rotate counterclockwise from
out-back to out-forward and from out-down to out-up. All data are
from subject A.
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In Figure 10, the threshold line for unit 10.1 in the sagittal plane
was oriented much like that for unit 9.1, with a best direction in the
down-backward direction. In the horizontal and frontal planes, the
threshold line yielded a best direction of out-backward and
out-downward, respectively. The orientation of the threshold plane in
the bottom row illustrates that the 3D best direction of unit 10.1 was
in the out-back-downward direction.
Unit 10.2 was found in a recording location 6.5 cm anterior to that of
unit 10.1 (i.e., in the medial deltoid). Its best direction in the
sagittal plane was in the up-forward direction, comparable to that of
unit 9.2. Considering only the sagittal plane, one might thus conclude
that the best directions for units 10.1 and 10.2 differed by 180°.
The threshold lines for the horizontal and frontal planes, however,
show that the best directions for unit 10.2 in these planes differed
from those of unit 10.1 by only 60 and 15°, respectively. With
respect to the lines for unit 10.1, the threshold lines for unit 10.2 were slightly rotated counterclockwise, such that the best direction
was out-forward for the horizontal plane and straight outward for the
frontal plane. Accordingly, the plane fit to the 3D data yielded a best direction for unit 10.2 that was oriented out-forward and slightly up.
Of the three units in Figure 10, unit 10.3 was found in the most
anterior recording location. Considering only the sagittal plane, this
unit appeared to have approximately the same best direction as unit
10.2; however, the threshold lines for the other two planes were
rotated counterclockwise with respect to those of unit 10.2 (by 30 and
35° for the horizontal and frontal planes, respectively). The best
directions for these planes are thus forward-out (with a greater
forward component than that of unit 10.2) in the horizontal plane and
out-up in the frontal plane. The orientation of the threshold plane in
3D confirms that the best direction of this unit is
up-out-forward.
It follows from these results that the very large (or very small)
differences found between the best directions of deltoid units for
forces in the sagittal plane are deceptive. Units with apparently
opposite best directions in the sagittal plane (such as units 10.1 and
10.2) might in fact have threshold planes that differ only relatively
little in their orientations. Thus, in 3D space the difference between
the best directions of units 10.1 and 10.2 was only 53°. On the other
hand, units with approximately the same best direction in the sagittal
plane might show significant differences between their best directions
in 3D. Thus, the difference between the 3D orientation of the planes of
units 10.2 and 10.3 was 48°, although their threshold lines in the
sagittal plane differed by only 6°.
Bidirectional deltoid units
Analogous to the bimodal units described above for biceps (e.g.,
unit 6.3) we also found evidence for multiple directional inputs on
deltoid SMUs (19%, n = 14 in the 2D experiment (Fig. 9), 7%, n = 5 in the 3D experiments). The 3D
recruitment data for a bidirectional deltoid unit are shown in Figure
11. From the sagittal plane data, which
are best fit by two approximately parallel threshold lines, one cannot
discern whether the threshold planes in 3D would be parallel, yielding
two best directions opposite to each other or whether the two planes
would have a line of intersection. However, two parallel threshold
planes would intersect all three experimental planes with two parallel
lines, and the two-line fits to the horizontal and frontal plane data
clearly show that this is not the case. The two lines in these plots
are not parallel but instead intersect at an angle of 90° in the
horizontal and 125° in the frontal plane. Accordingly, the two
threshold planes fit to the 3D data have a line of intersection. The
best directions for this unit are up-out-forward and
down-out-backward and differ by 93° in 3D. None of the threshold
data of bidirectional units found in the second set of experiments were
fit by two parallel planes, meaning that all bidirectional units
exhibited intersecting threshold planes. The differences between the
two best directions of such units ranged from 58 to 96° in 3D space
with an average value of 77°.

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Figure 11.
Threshold lines (top) and planes
(bottom) for a deltoid unit with two preferred
directions. The origin of the plot is located in the center of the
polygon. From only the sagittal plane data, it might be assumed that
the two threshold planes are parallel and the two best directions
180° apart. Data in the other two planes show, however, that the two
threshold planes have a line of intersection.
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The relation between location and best direction
In Figure 12, each deltoid SMU is
represented by a unit vector radiating (from the origin) in the best
direction of the unit. The color of the vector codes for the
anterior-posterior location of the unit in the muscle. In general, as
unit location changed from posterior (blue end of spectrum) to anterior
(red end), best direction gradually changed from down-backward to
up- forward. A similar pattern was found in all three subjects (Fig.
12a). Regressing recording location on the x,
y, z coordinate of the tip of the unit vector
yielded significant correlations for subject A
(p < 0.001, r = 0.79) and
subject B (p < 0.05, r = 0.71)
but a nonsignificant correlation for subject D
(p = 0.066, r = 0.66). Because
all subjects exhibited a qualitatively similar relation between best
direction and location, we then pooled the data (Fig. 12b).
Pooling data from all subjects by normalizing the unit location (across
the width of each subject's deltoid, see Fig.
13b) yielded a highly significant relation between the 3D best direction and location (p < 0.001, r = 0.64). When
regressing the 2D best directions for the horizontal and frontal planes
on unit location, highly significant correlations
(p < 0.001) were obtained for all three subjects in both planes, with r2-values
ranging from 0.6 to 0.8 (plots not shown). Units located in the
posterior part of the muscle were best activated for out-backward (horizontal plane) and out-downward (frontal plane) forces. As unit
location changed to the more anterior part of the muscle, best
directions gradually changed to the out-forward and out-upward directions, with no suggestion of discontinuity at posterior-medial or
medial-anterior compartmental boundaries.

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Figure 12.
a, 3D best direction of each unit
versus their locations in deltoid, for each subject. The best direction
is given by the direction of the unit vector from the origin. The color
of the vector codes for location. As location changes from posterior to
anterior (and color changes from the blue to the
red end of the spectrum), best direction changes from
down-out-backward to up-out-forward. b, Pooled 3D
best directions of all units versus their normalized locations in
deltoid, for all subjects. Best directions are coded for location as in
a.
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Figure 13.
Dynamic pulses in the frontal plane; relative
timing of two deltoid units with different best directions.
a, Threshold lines of units
M/AD (medial/anterior deltoid) and
MD (medial deltoid) in the frontal plane.
b, Locations of these units. Note that the more anterior
unit has a best direction with a greater upward component than that of
the more medial unit. c, MD rectified multiunit records
for one trial and unit rasters for three trials in each direction (note
that the unit potential could not always be recognized because of
firing of other units). As the direction of the pulse changed from up
to up-out, the bursts were earlier with respect to force onset
(gray line). d, Simultaneously
recorded EMG from M/AD exhibits the opposite temporal relation to force
onset.
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Extension to dynamic forces
The range of threshold magnitudes in our sample of BI and deltoid
units extended from 0.2 to 28 N, and ~50% of the units had threshold
forces of >12 N. Thus, a substantial number of units in both muscles
were recruited at relatively high force levels and could be assumed to
contract quickly enough to be involved in the generation of fast-rising
forces or movements. Moreover, as will be explained below, we found
that units with threshold magnitudes as low as 2 N were involved in the
generation of fast pulses of isometric force.
Figure 13 illustrates the results from an experiment in which subject D
produced isometric pulses to different targets in the frontal plane.
(This figure is also representative of the results of the second
dynamic experiment.) Simultaneous recordings from two different
electrodes are shown. The threshold lines and preferred directions (in
the frontal plane) of two units found on the two different electrodes
are shown in Figure 13a. The best direction of unit MD
(found in the center of deltoid, Fig. 13b) was almost straight outward with only a slight upward component. On the other hand, unit M/AD (found in a recording location ~3 cm anterior to unit
MD) had an up-forward best direction.
Consider now the relative timing of the multiunit bursts on the two
recording electrodes during dynamic pulses (with a 250 msec time to
peak) in the three different directions (Fig.
13c,d). As the direction of the pulse changed
from upward (top lines) to up-out (bottom
lines), the bursts in the two recordings reversed their
order. For the upward direction (closer to best direction of unit
M/AD), the burst in the recording at the more anterior site was
earlier. For the outward direction (closer to best direction of unit
MD), the burst in the recording at the more posterior site was earlier.
Because we have ascertained that units M/AD and MD are involved in
those bursts (as marked in the three-trial unit rasters), it appears
that the recruitment order of these individual units also changed
depending on the direction of the dynamic force.
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DISCUSSION |
We found that threshold data for 93% of our biceps and deltoid
motor units could be fit with lines in 2D and/or planes in 3D,
consistent with a model in which activation levels are tuned as a
cosine function of force direction (Fig. 2) and in consonance with the
well established idea that the descending inputs to spinal motoneuronal-interneuronal pools may have cosine-tuned activity (Georgopoulos et al., 1982 , 1988 ; Fortier et al., 1993 ). Using the
orientation of the line or plane as a measure of the best direction of
a unit, we showed that SMUs of the same muscle were not activated
homogeneously but instead different units had different best
directions. The best directions of units changed continuously with
their locations in the muscle and did not cluster into distinct groups.
For deltoid, the gradual change in best directions may echo the gradual
change in the mechanical actions of the muscle fibers (Buneo et al.,
1996). As discussed below, the gradual change of best directions in
biceps might be understood by considering that during the time course
of a movement, biceps units may act in synergy with various deltoid
units. Thus, the directional specificity of the recruitment order may
act in conjunction with the phenomenon of size-ordered recruitment, to
enable smooth and fatigue-resistant muscle contractions. But before
developing these ideas, we will consider several technical issues that
influence the interpretation of our data.
Technical issues
Using only a 2 df force transducer in the first set of experiments
raised the concern that any significant differences between 2D best
directions of different BI units might be caused by day-to-day variability in the levels of force outside the sagittal plane. This
possibility was ruled out by the fact that unit recordings obtained
under identical force conditions (on the same electrode and/or in the
same recording session) yielded significantly different best directions
(Fig. 5, Table 1). Moreover, we were often able to identify two
different preferred directions for the same unit (Fig. 6, Table 1).
This provides evidence for a wide range of different directional inputs
to the BI MN pool.
Another caveat arose from cases in which the angular separation between
the two putative best directions of a unit was not large enough, and a
possibly bimodal unit was classified as unimodal. This would have
introduced a bias toward a central value in the distribution of best
directions. Despite this possible bias we found a wide range of
different best directions (77° for BI units, Fig. 8a).
When using a method that would be insensitive to this distortion toward
a central value, the range of best directions of BI units increased to
144° (Fig. 8b). These findings support our main conclusion
regarding the distributed activation of the MN pool.
A final issue concerns the validity of the results for anything other
than isometric contractions. Our experimental paradigm seemed to favor
the recruitment of low-threshold units primarily relevant in the
production of static forces rather than movements. There is some
indication that the CNS might employ different strategies in the
control of the small SMUs principally subserving posture and the large
units involved in movement (Ghez, 1979 ; Flanders and Herrmann, 1992 ).
However, it has recently been reported that the same units are
activated (albeit differently) for isometric forces and movements, thus
supporting the idea that units in our sample are also involved in the
generation of movements (van Bolhuis et al., 1997 ). Similarly, in the
present study the same units active during slow ramps also fired during
phasic EMG bursts (Fig. 13). Moreover, because subjects supported the
weight of their arm at the beginning of each trial and because our
analysis relied on the recruitment threshold of a unit, we excluded
units that were active for postural support. Thus, at least for forces
with an upward component (the preferred directions for BI and anterior deltoid units) our sample does not contain those units most likely to
be involved in posture (Table 1). Furthermore, the wide range of
threshold levels and the substantial number of units recruited only at
relatively high forces would suggest that our conclusions also apply to
those units involved in movement generation.
Neural substrate for bidirectional units
Although the majority of units in our sample exhibited tuning
curves that were consistent with the unimodal cosine tuning reported
for supraspinal inputs (Georgopoulos et al., 1988 ), 17% of the units
examined were bimodally tuned. When considering the bidirectional units
in BI and those found in deltoid in the 3D experiments, the angular
differences between best and second-best directions ranged from 30 to
98°. The majority (75%) of these bimodally tuned units had best
directions that were <90° apart. If the two activation lobes of
bidirectional units were to subserve the activation of the muscle as an
agonist and as an antagonist (working in conjunction with another
muscle with the opposite mechanical action, see Flanders and Soechting,
1990 ), the two best directions might be expected to be opposite each
other, i.e., 180° apart. Such an organization might help to stiffen
the joint along the axis of the pulling direction of the muscle. The
much smaller angular separation found here, on the other hand, might suggest that the second activation lobe of a bidirectional unit subserves an activation of part of the parent muscle in synergy with
various other muscles or motor units in the system. The force vectors
produced by such units might be necessary to balance the ones generated
by other synergistic muscles during the production of a desired force
(Flanders, 1993 ). Thus, the bidirectional units found here might
constitute subpopulations that are activated in synergy with other
units in the system. This idea is consistent with findings by Jongen et
al. (1989) who report intramuscular differences in activation during
cocontraction of other muscles.
If these bimodal SMUs receive input from only unimodally tuned neurons,
the question arises as to how unimodal inputs can produce bimodal
outputs. Summing two cosine functions always results in a third
unimodal cosine function. Even when the two input functions have a
threshold nonlinearity (see Materials and Methods section of this study
and Flanders and Soechting, 1990 ) their addition results in a unimodal
output function, unless the angular separation between the two input
peaks is wide and/or the threshold is high. Thus, to reproduce the
tuning pattern of bimodal units whose two best directions differ by
<90° (the norm in our study), some kind of nonlinear interaction has
to occur between the two unimodal inputs.
Using NEURON simulation software (Hines and Carnevale, 1997 ) we
attempted to create the observed MN output solely from a specific pattern of convergence of unimodally tuned inputs at the dendritic arbor of the MN (Herrmann, 1998 ). Several combinations of inputs with
different relative locations, weights, and preferred directions were
simulated, but none of them resulted in the pattern of bimodal output
observed experimentally. Thus, it seems that a solution at the level of
the motoneurons would have to be a very specific one and that unimodal
inputs do not tend to produce a bimodal output as a result of simple
convergence patterns. An alternative model might contain a reciprocal
inhibition between two unimodally tuned inputs. It is also possible
that the bidirectional tuning of SMUs arises from bimodally tuned
inputs.
Compartmentalization versus distributed innervation
It has been suggested that a muscle is organized into smaller
submodules such that the elements controlled by the CNS are neuromuscular compartments rather than whole muscles (Windhorst et al.,
1989 ; English et al., 1993 ). Such partitioned control might be
functionally advantageous because individual muscles are nonuniform in
their mechanical actions (Chanaud et al., 1991a ; Carrasco and English,
1997 ) and/or their fiber type distribution (Chanaud et al., 1991b ). The
existence of neuromuscular compartments suggests the fractionation of
the MN pool of a muscle into smaller, differently activated
subpopulations. Presumably each subpopulation would then receive
homogenous activation such that recruitment order within each
compartment is determined by MN size (Windhorst et al., 1989 ). For cat
hindlimb muscle, the fibers innervated by MNs of the same subpopulation
have been found to be largely restricted to a distinct muscular
territory (English and Letbetter, 1982 ).
According to these arguments we would have expected BI and deltoid
units to fall into a limited number of groups, each group containing
units with the same best direction and localized in a restricted muscle
area. Instead we found a continuous distribution of best directions
with no convincing evidence for clustering. When grouping BI units with
similar best directions together, their anatomical territories
overlapped widely and spanned the whole width of the muscle (Fig. 8).
Thus, the MN pool of these muscles appears not to be compartmentalized
but to instead receive a more continuously distributed innervation.
Georgopoulos et al. (1988) have shown that the 3D best directions of
motor cortical cells uniformly cover the 3D space and do not appear to
cluster into distinct groups. Thus, the neural substrate to create a
continuous, finely graded distribution of the best directions of SMUs
is available at the supraspinal level.
A similar lack of compartmentalization has been found in a bitendoned
finger extensor (Schieber et al., 1997 ). Although one might logically
expect to find two distinct compartments in this muscle (one for each
tendon), most units contribute to force on both tendons, with
selectivity for either tendon ranging on a continuum. Analogously, BI
has two distinct anatomical subdivisions with different attachments and
moment arms at the shoulder (Wood et al., 1989 ), but the organization
of its MN pool reveals more of a continuum. In deltoid, on the other
hand, it seems apparent that the pulling directions of the SMUs change
continually with location along the broad attachment of the muscle
(Buneo et al., 1997 ), thus motivating the continuously changing
directional innervation of different parts of the muscle. Accordingly,
the best directions of deltoid SMUs varied continuously across a wide
area of space (Fig. 12).
The correlation between best direction and recording location might
also be related to the topography of the spinal MN pool as suggested by
Kernell (1989) . A rostrocaudal topography has been described for MN
pools of the two parts of deltoid muscle in the rat (Choi and Hoover,
1996 ). The considerable overlap found between these two pools may be
consistent with our finding of continuous rather than compartmentalized
preferred directions and multiple directional preferences for some
units.
Implications for movement generation
Similar features of muscle activation are found in movements and
dynamic isometric forces (Ghez and Gordon, 1987 ; Flanders et al., 1996 ;
Pellegrini and Flanders, 1996 ). This suggests that similar control
strategies are involved in these two tasks. In Figure 13 we show that
the timing of the activity of a unit moved from an early to a
progressively later point in the force pulse as the direction of the
pulse moved away from the best direction of the unit. Given the
parallels between the neural control of force pulses and movements, one
can speculate that the relative timing of recruitment during a movement
could potentially be predicted from the best directions of the units
under static conditions and the directions of dynamic forces during
movement.
As arm muscles change their mechanical actions with arm posture, the
directional tuning of whole muscles generally changes in parallel with
the new pulling directions of the muscles (Flanders and Soechting,
1990 ). Although it remains to be determined whether the best directions
of the motor units change with posture (or if whole muscle tuning
changes via recruitment of different units), this suggests that the
central control mechanism takes limb configuration into account when
issuing motor commands. Muscles with different mechanical actions are
activated at different times during a reaching movement (Flanders et
al., 1996 ). Thus, a factor determining the timing of the activation of
a muscle might be the degree of correspondence between its pulling
direction and the direction of force currently required. If differences
in mechanical action exist across units within a muscle, the population
of units optimally fit to produce a required force vector will change
with limb position and force direction during a movement.
Based on this logic, we hypothesize that at different points in the
movement, the various units are recruited according to their mechanical
actions. The neuromuscular system could thereby gradually make use of
the wide number of units available instead of activating a few discrete
populations. This spatiotemporal recruitment rule would necessarily
involve violations of the size principle (Henneman et al., 1965 ; see
also DeLuca and Erim, 1994 ). However, reminiscent of the advantages of
size-ordered recruitment, this strategy would minimize fatigue and
increase efficiency because mainly those units ideally suited for the
production of a required force vector would be active at any given
time. Furthermore, because cosine-tuned units are active over a wide
range of directions, the change in unit activation during a movement
need not consist in the abrupt recruitment and derecruitment of
distinct subpopulations but can instead proceed smoothly by gradual
recruitment and derecruitment and differential modulation of the firing
rates of different units. This smooth change in relative unit activity
would agree with the postulate that in the execution of a motor act,
the control mechanism strives to minimize abrupt changes in the motor
commands (Dornay et al., 1996 ).
 |
FOOTNOTES |
Received April 2, 1998; revised July 27, 1998; accepted July 29, 1998.
This work was supported by National Institute of Neurological Disorders
and Stroke Grant R01 NS27484, and it partially fulfilled PhD
requirements. We thank Dr. John F. Soechting for helpful
discussions.
Correspondence should be addressed to Dr. Martha Flanders, Physiology
Department, 6-255 Millard Hall, University of Minnesota, Minneapolis,
MN 55455.
 |
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