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 . C lose-up below unit trace shows consistent shape and amplitude of the potential of this unit. 

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 . C lose-up below unit trace shows consistent shape and amplitude of the potential of this unit. 

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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...

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... 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 ( ϳ 25 ␮ m 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, record- ings 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 land- marks and its location was marked on a “map” overlaid on the muscle using a transparency. 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 “recog- nized” this part of the record as the unit potential and marked it in a raster of the trace (Fig. 1 c ). 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 recruit- ment 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. 2 a ). 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. 2 a ). 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 f unctions with a threshold nonlinearity were fit to the frequency data according to the formula: Firing frequency cos (1) where c is a constant offset, a is a constant scaling the cosine f unction, 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. Figure 2 a 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. 2 b , the length of the dashed lines ) should increase until for force directions Ն 90° from ␾ 0, the unit is silent and threshold force is infinite. This relation of threshold force to force direction is f ulfilled 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 ...

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... We show here that most of the motor units from the triceps surae muscles might receive two sources of common inputs. The combination of multiple independent inputs might therefore explain why previous works reported changes in recruitment strategies between motor units from the same muscle while changing the mechanical constraints of the task (Desnedt & Gidaux, 1981;Herrmann & Flanders, 1998;Marshall et al., 2022;ter Haar Romeny et al., 1984). ...
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... For different skeletal muscles, regional changes in the EMG amplitude have been observed for a number of circumstances, such as for different joint positions (Watanabe et al., 2012), contraction durations (Farina et al., 2008;Tucker et al., 2009) and force levels (Holtermann et al., 2005;Rojas-Martínez et al., 2012), as well as during standing (Vieira et al., 2010) or dynamic contractions (Falla and Farina, 2007). The mechanical efficiency of specific regions within the muscle (Herrmann and Flanders, 1998;Holtermann et al., 2005) and neural strategies for delaying and/or minimizing muscle fatigue (Falla and Farina, 2007;van Dieën et al., 1993) are examples of potential mechanisms of uneven distribution of activity within muscles. ...
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Proper muscle activity quantification is highly relevant to monitor and treat spastic cocontraction. As activity may distribute unevenly within muscle volumes, particularly for pennate calf muscles, surface electromyograms (EMGs) detected by traditional bipolar montage may provide biased estimations of muscle activity. We compared cocontraction estimates obtained using bipolar vs grids of electrodes (high-density EMG, HD-EMG). EMGs were collected from medial gastrocnemius, soleus and tibialis anterior during isometric plantar and dorsi-flexion efforts at three levels (30%, 70% and 100% MVC), knee flexed and extended. Cocontraction index (CCI) was estimated separately for each electrode pair in the grid. While soleus and tibialis anterior CCI estimates did not depend on the detection system considered, for gastrocnemius bipolar electrodes provided larger cocontraction estimates than HD-EMG at highest effort levels, at both knee angles (ANOVA; P < .001). Interestingly, HD-EMG detected greater gastrocnemius EMGs distally during plantar flexions, and greater CCI values proximally during dorsiflexions. These results suggest that bipolar electrodes: (i) provide reliable estimates of soleus and tibialis anterior cocontraction; (ii) may under-or overestimate gastrocnemius cocontraction, depending on their distal or proximal position.