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Figure 30 shows the comparison between the maximum frequency of the four modes as a function of the ω b.
Figure 29 shows the comparison between the maximum growth rate of the four modes as a function of ω b.
The parameters are γ = 1.03122, Ω ce = 0.04 and ω b = 0.04. Figure 24a shows the comparison between the maximum growth rates of the four modes as a function of the plasma frequency.
Open image in new window Fig. 29 Comparison between the normalized maximum growth rate ( ( Im k ^ ) Max ) of the four modes as a function of the beam plasma frequency, ω b.
Open image in new window Fig. 24 Comparison between the a normalized maximum growth rate ( ( Im k ^ ) Max ), b frequency of maximum growth rate (fMax) of the four modes as a function of the plasma frequency, ω p. The parameters are γ = 1.03122, Ω ce = 0.04 and ω b = 0.04. Figure 24b shows the comparison between the maximum frequencies of the four modes as a function of the plasma frequency.
The comparison between the maximum growth rate of the four modes as a function of ω b shows that the behaviors of the (X bp − X p ) and (X bp − O p ) modes as a function of ω b are the same as well as the behavior of the (O bp − O p ) and (O bp − X p ) modes. 10.
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c Peak wavelengths of the two resonance modes as a function of structure angle.
As a consequence, two different device operation modes, as a function of voltage bias, are possible.
Figure 7 Eigenvalues of the normal modes as a function of for.
In Figure 8, the consumed energy per superframe by the device and relay nodes of the three modes as function of PER are compared.
The results of these investigations enable the identification of three modes of failure as a function of the interaction between the shear-head and surrounding concrete.
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