Figure 26 shows the amplitude of the potential difference as a function of ω.
The behavior of the Equilibrium Temperature as a function of Ω was also investigated.
In Figure 5, we plot |T| as a function of (ω c /ω).
In Figure 5 this error as a function of ω is shown.
φ ( ω, u ) is a continuous even function of u, which is non-decreasing for u > 0, such that φ ( ω, 0 ) = 0, φ ( ω, u ) > 0 for u ≠ 0 and φ ( ω, u ) → ∞ as u → ∞ ; φ ( ω, u ) is a measurable function of ω for each u ∈ R ; φ ( ω, u ) is a convex function of u for each ω ∈ Ω.
For instance, with l2b.glob the RARMISE increased as a function of ε for σ θ anc, but decreased for ω.
In Figure 5, we can see the growth rate ω+ as a function of the k for different values of μ.
The parameters are Ω ce = 0.04, ω p = 0.011, ω b = 0.01. Figure 15 shows the plot of the growth rate as a function of frequency for all of the modes.
The parameters are ω p = 0.04, ω b = 0, γ = 1.0, and Ω ce = 0.0, 0.08, 0.08 and 0.12. Figure 3a d illustrates the phase velocity as a function of frequency for different values of cyclotron frequency.
The parameters are ω b = 0, γ = 1.0, Ω ce = 0.06 and ω p = 0.0, 0.04, 0.06, 0.06 and 0.08. Figure 5a d illustrates the phase velocity as a function of frequency for different values of the plasma density.
