All Figures

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f1.eps} \end{figure}$ Figure 1: The dependence of density on the spatial coordinate y( $\tau =3$ ), curve 1 - kinetic equation solution, curve 2 - diffusion approximation, curve 3 - telegraph equation solution, curve 4 - solution of transport Eq. (27), dashed curve - unscattered particles, dotted curve - scattered particles.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f2.eps} \end{figure}$ Figure 2: The temporal dependence of density in y=2 position, curve 1 - kinetic equation solution, curve 2 - diffusion approximation, curve 3 - telegraph equation solution, curve 4 - solution of transport Eq. (27), dashed curve - unscattered particles, dotted curve - scattered particles.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f3.eps} \par\end{figure}$ Figure 3: The temporal dependence of anisotropy $\xi$ in y=2 position, curve 1 - kinetic equation solution, curve 2 - diffusion approximation, curve 3 - telegraph equation solution, curve 4 - solution of new transport equation.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f4.eps} \end{figure}$ Figure 4: The temporal dependence of particle density in y=1 position, curve 1 - solution of transport Eq. (27), curve 2 - solution of transport Eq. (37), dashed curve - diffusion approximation.
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f5.eps} \end{figure}$ Figure 5: The temporal profile of solar particle event of July 14, 2000, as recorded by the neutron monitor Sanae and calculated enhancements of CR intensity. Time is in minutes after energetic particle injection near the Sun (the SCR release was supposed to occur at 10.20 UT). The dotted curve corresponds to the diffusion approximation, the dashed curve illustrates the solution (69) under isotropic scattering, and the solid line is associated with (69) in the case of linearly anisotropic scattering ( $\alpha =1/3,\gamma =0$ ).
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In the text

$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f1.eps} \end{figure}$	Figure 1: The dependence of density on the spatial coordinate y( $\tau =3$ ), curve 1 - kinetic equation solution, curve 2 - diffusion approximation, curve 3 - telegraph equation solution, curve 4 - solution of transport Eq. (27), dashed curve - unscattered particles, dotted curve - scattered particles.
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$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f2.eps} \end{figure}$	Figure 2: The temporal dependence of density in y=2 position, curve 1 - kinetic equation solution, curve 2 - diffusion approximation, curve 3 - telegraph equation solution, curve 4 - solution of transport Eq. (27), dashed curve - unscattered particles, dotted curve - scattered particles.
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$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f3.eps} \par\end{figure}$	Figure 3: The temporal dependence of anisotropy $\xi$ in y=2 position, curve 1 - kinetic equation solution, curve 2 - diffusion approximation, curve 3 - telegraph equation solution, curve 4 - solution of new transport equation.
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$\begin{figure} \par\includegraphics[angle=-90,width=8.8cm,clip]{f4.eps} \end{figure}$	Figure 4: The temporal dependence of particle density in y=1 position, curve 1 - solution of transport Eq. (27), curve 2 - solution of transport Eq. (37), dashed curve - diffusion approximation.
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