$\begin{figure} {{\includegraphics[width=9cm]{4805fig1.EPS} }} \end{figure}$ Figure 1: Radial self-similar velocity distributions as a function of the self-similar variable $\xi$ for a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}$ , $2\times 10^{-3}$ , $3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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In the text

$\begin{figure} {{\includegraphics[width=9cm]{4805fig2.EPS} }} \end{figure}$ Figure 2: Azimuthal self-similar velocity distributions as a function of the self-similar variable $\xi$ , corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}, 2\times 10^{-3}, 3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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In the text

$\begin{figure} {{\includegraphics[width=9cm]{4805fig3.EPS} }} \end{figure}$ Figure 3: Self-similar surface density distributions as a function the of self-similar variable $\xi$ , corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}, 2\times 10^{-3}, 3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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In the text

$\begin{figure} {{\includegraphics[width=9cm]{4805fig4.EPS} }} \end{figure}$ Figure 4: Self-similar mass accretion rate distributions as a function of the self-similar variable $\xi$ , corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}, 2\times 10^{-3}, 3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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In the text

$\begin{figure} {{\includegraphics[width=9cm]{4805fig5.EPS} }} \end{figure}$ Figure 5: Distribution of the Toomre Q value as a function of the self-similar variable $\xi$ , corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}, 2\times 10^{-3}, 3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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In the text

$\begin{figure} {{\includegraphics[width=9cm]{4805fig6.EPS} }} \end{figure}$ Figure 6: The angular momentum coefficient profile, q, as a function the self-similar variable $\xi$ corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ . We see its behavior versus the dimensionless viscosity parameter for b) $\beta$ disks c) $\alpha$ disks at $\gamma =1.1$ .
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In the text

$\begin{figure} {{\includegraphics[width=9cm]{4805fig1.EPS} }} \end{figure}$	Figure 1: Radial self-similar velocity distributions as a function of the self-similar variable $\xi$ for a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}$ , $2\times 10^{-3}$ , $3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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$\begin{figure} {{\includegraphics[width=9cm]{4805fig2.EPS} }} \end{figure}$	Figure 2: Azimuthal self-similar velocity distributions as a function of the self-similar variable $\xi$ , corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}, 2\times 10^{-3}, 3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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$\begin{figure} {{\includegraphics[width=9cm]{4805fig3.EPS} }} \end{figure}$	Figure 3: Self-similar surface density distributions as a function the of self-similar variable $\xi$ , corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}, 2\times 10^{-3}, 3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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$\begin{figure} {{\includegraphics[width=9cm]{4805fig4.EPS} }} \end{figure}$	Figure 4: Self-similar mass accretion rate distributions as a function of the self-similar variable $\xi$ , corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}, 2\times 10^{-3}, 3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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$\begin{figure} {{\includegraphics[width=9cm]{4805fig5.EPS} }} \end{figure}$	Figure 5: Distribution of the Toomre Q value as a function of the self-similar variable $\xi$ , corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ b) $\beta =10^{-3}, 2\times 10^{-3}, 3\times 10^{-3}$ at $\gamma =1.1$ c) $\beta =10^{-3}$ and $\alpha =10^{-1}$ at $\gamma =1.1$ .
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$\begin{figure} {{\includegraphics[width=9cm]{4805fig6.EPS} }} \end{figure}$	Figure 6: The angular momentum coefficient profile, q, as a function the self-similar variable $\xi$ corresponding to a) $\gamma =1.0, 1.1$ at $\beta =10^{-3}$ . We see its behavior versus the dimensionless viscosity parameter for b) $\beta$ disks c) $\alpha$ disks at $\gamma =1.1$ .
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