$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig1.ps}\end{figure}$ Figure 1: The time-evolution of the magnetic field perturbation, for B₀ = 7 Gauss and for several values of the resistivity $\eta$ (s). Notice that, for $\eta \neq 0$ , the perturbation's amplitude is saturated, acquiring large values for long enough time intervals.
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In the text

$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig2.ps}\end{figure}$ Figure 2: The time-evolution of the electric field perturbation, for B₀ = 7 Gauss and for several values of the resistivity $\eta$ (s). Notice that, in this case, there is no saturation.
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In the text

$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig3.ps}\end{figure}$ Figure 3: The time-evolution of the energy density perturbation for several values of the coordinate wave-length $\lambda$ in terms of $\lambda _{\rm c}$ .
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In the text

$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig4.ps}\end{figure}$ Figure 4: The time-evolution of the magnetic field perturbation for $\eta = 0.0645$ s, B₀ = 7 Gauss and for several values of the coordinate wave-number in terms of $k_{\rm c}$ .
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In the text

$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig5.ps}\end{figure}$ Figure 5: The time-evolution of the energy density perturbation, for $k = k_{\rm c}$ and for several values of the resistivity $\eta$ (s). We observe that the Jeans instability becomes more prominent as the resistivity grows.
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In the text

$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig1.ps}\end{figure}$	Figure 1: The time-evolution of the magnetic field perturbation, for B₀ = 7 Gauss and for several values of the resistivity $\eta$ (s). Notice that, for $\eta \neq 0$ , the perturbation's amplitude is saturated, acquiring large values for long enough time intervals.
Open with DEXTER

$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig2.ps}\end{figure}$	Figure 2: The time-evolution of the electric field perturbation, for B₀ = 7 Gauss and for several values of the resistivity $\eta$ (s). Notice that, in this case, there is no saturation.
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$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig3.ps}\end{figure}$	Figure 3: The time-evolution of the energy density perturbation for several values of the coordinate wave-length $\lambda$ in terms of $\lambda _{\rm c}$ .
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$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig4.ps}\end{figure}$	Figure 4: The time-evolution of the magnetic field perturbation for $\eta = 0.0645$ s, B₀ = 7 Gauss and for several values of the coordinate wave-number in terms of $k_{\rm c}$ .
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$\begin{figure} \par\includegraphics[height=6.3cm,width=8cm,clip]{7109fig5.ps}\end{figure}$	Figure 5: The time-evolution of the energy density perturbation, for $k = k_{\rm c}$ and for several values of the resistivity $\eta$ (s). We observe that the Jeans instability becomes more prominent as the resistivity grows.
Open with DEXTER