We now consider the effects of variation in the relative widths of the hot and cool electron distributions.
The widths are found to be greater for large angles of propagation.
The double layer widths are found to be greater for larger angles of propagation.
At this level, one cannot come to a conclusion as these behaviors must be compared to the resonance widths.
The widths of individual trabeculae are variable, but none is greater than 1.0 mm.
The evolution of the half widths of the 0 and @ profiles is shown in figure 15(a).
Bell-shaped membership functions with centers m i and widths si are used as the adjustable parameters in all the computations.
Although b-wave widths were shor tened to ;100 ms in pigmented mice, they remained wide in the albino animals.
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