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The defibrillation waveform for all patients was programmed to the optimal pulse width settings based on a theoretical 3.5 ms membrane time constant using a commercially available chart of optimal defibrillation pulse width (Phase 1/Phase 2) durations.
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The apparent pulse width of Phase 2 coming around the epicenter is about 30– 40 seconds.
The oblique propagation of solitons in an inhomogeneous plasma has been investigated by Aziz and Stroth [8] in which the effects of electron and ion temperatures along with their concentrations on soliton width and phase velocity were studied.
From Fig. 15, the proposed method outperforms the method in [21] and the correct ratio of the proposed method is greater than 90%% when SNR >2 dB, because the peak width of phase search pseudo-spectrum is narrower.
Stimulation consisted of trains of biphasic, 25 µs width per phase pulses presented at 80 Hz.
Electrically-evoked ABRs were obtained by using biphasic pulses, 50 ms width per phase, presented at 20 Hz.
The results show that the annealing process after electron irradiation modifies the phase-transition temperature and the width of phase-transition hysteresis.
The ultra-fine microstructure with submicron scaled acicular α/α′ phases (60 400 nm in width) and β phase is obtained under the scanning speed of 600 mm min− 1.
The apparent pulse width of the phase (about 20 s) is shorter than that of Phase 2 (about 30 40 s).
The mentioned drawback is not present in the natural model; thus, the diffuse interface width between two phases in a multiple phase setup remains the same.
The coarsening kinetics over these two orders of magnitude change could be described by r2 − r2o = kt, where r is the phase width after time t at 1173 K, ro is initial phase width, and k is a constant.
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