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Disc Structure

Fig. 1 shows the evolution of surface density (left pan el) and the final disc structure (right panel). Averaging is done by using

\begin{displaymath}
<f(\vec{r})> = \sum_{j=1}^N \frac{m_j}{\rho(\vec{r}_j)}
W(\vec{r}-\vec{r}_j, h),
\end{displaymath}

where $W(r,h)$ is the kernel given by

\begin{displaymath}
W(r,h) = \frac{1}{\pi h^3} \left\{
\begin{array}{ll}
1-\f...
...}{h} < 2,\\
&\\
0 & {\rm otherwise}.
\end{array} \right.
\end{displaymath}

Figure 1: (Left) Surface density evolution from $t = $0 to 30 in units of $P_{\rm orb}$. The interval of time between adjacent contours is 5 ($t = $ 0, 5, $\ldots$ from bottom). (Right) Disc structure at $t = 30$. The black, the blue, and the red lines are for the surface density, the radial Mach number, and the angular velocity normalized by the stellar break-up velocity, respectively. The magenta line is for $\alpha_{\rm SS}$ and the green line is for the smoothing length normalized by the disc scale-height.
\includegraphics[height=10cm]{rdist.ps}



Atsuo Okazaki 2002-01-28