Simulation of surface EMG signals at different contraction intensities with the model used in Fig. 1. Simulation of surface EMG signals at different contraction.

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Simulation of surface EMG signals at different contraction intensities with the model used in Fig. 1. Simulation of surface EMG signals at different contraction intensities with the model used in Fig. 1. The distribution of discharge rates of the active MUs was determined as described in Fuglevand et al. (35). The upper limit of MU recruitment was 80% of the excitation level, and discharge rate increased at 0.3 pulses per second (pps)/excitation level. Discharge rate at recruitment was 8 pps for all MUs. Four excitation levels were simulated: 15% (top row) and 35, 55, and 75% (bottom row). The number of MUs activated at the four levels of excitation was 92, 121, 137, and 147. Mean discharge rate is indicated to the left of each row. The coefficient of variation for discharge rate (variability) was assigned values of 0% (left), 10% (middle), and 20% (right). The estimated power spectra for the 20-s simulations are shown (only in the frequency range 0-80 Hz) for both the interference and rectified signals. The arrows indicate the mean discharge rates of the active MUs. Rectification enhanced the low-frequency peaks in the spectra for low coefficients of variations and few active MUs. As the coefficient of variation approached values observed experimentally (65), however, it was difficult to detect the peaks in the rectified EMG spectra because of discharge rate variability. In many cases, peaks were evident in the interference signal but not the rectified signal spectra, because the model of the surface electromyogram as the summation of action potential trains does not hold for the rectified signal. Dario Farina et al. J Appl Physiol 2004;96:1486-1495 ©2004 by American Physiological Society