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The opacity calculations

A new opacity model relevant to the physical conditions typical of protoplanetary accretion disks is developed. As primal absorbers, we consider dust grains of different compositions, sizes, shapes and structures and various atoms, ions, molecules and electrons.

The wavelength-dependent (monochromatic), Rosseland mean and Planck mean opacities are computed for temperatures between $5$ K and $10\,000$ K and gas density ranges $2\,10^{-18}$ g cm$^{-3}$ and $2\,10^{-7}$ g cm$^{-3}$. The opacity model is described in more details in the paper by Semenov et al. [1]. The main advantage of our model is that works well for a wide range of the gas temperatures as well as gas densities, where diversity of the relevant physical processes causes the many recent models to fail.

To illustrate the results of our investigations, we compare Rosseland and Planck mean opacities calculated by the recent opacity models in Fig. 1.

Additionally, we study how different Rosseland mean values may affect the thermal structure of active accretion disks. We use a full 2D hydrodynamical code designed to simulate the interaction of the protoplanetary disk matter with a protoplanet and apply three various opacity tables to compute the disk midplane temperature (courtesy to G. D'Angelo). It is plotted in Fig. 2, where the corresponding disk models parameters are indicated. One may figure out immediately that the midplane temperature values can differ by up to $50\%$. This tells us about the importance of a proper opacity modelling.

Another aim was to make the opacity tables together with representative figures, tables and data easily accessible to the scientific community. We created a corresponding web-page and put it on the Internet: http://www.astro.uni-jena.de/Users/henning/Opacities/opacities.html.

The results of this work were reported in the NATO advanced workshop ''On the Optics of Cosmic Dust'', Bratislava, 16-19 November 2001 and presented in a poster during ``Stellar Atmosphere Modelling'' workshop, Tübingen, 8-12 April 2002 [2].

Figure 1: The comparison of the recent opacity models.
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\psfig{figure=fig3.ps,height=6.8cm,width=9.06cm,angle=0}\end{center}\end{figure}

Figure 2: The disk midplane temperature obtained with three different opacity models.
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\psfig{figure=fig4.ps,height=6.8cm,width=9.06cm,angle=0}\end{center}\end{figure}


next up previous
Next: The reduction of chemical Up: Astrophysical Modeling - The Previous: Astrophysical Modeling - The
Dimitri Semenov 2002-06-15