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$\begin{figure} \par\includegraphics[width=6.5cm,clip]{6142fig1.eps} \end{figure}$ Figure 1: Lyman continuum for models A₁ and C₁. Full lines represent averaged profiles over the width of the thread, dashed lines are mean profiles over the whole length of the thread. Double-arrowed lines belong to the model C₁.
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In the text

$\begin{figure} \par\includegraphics[width=15.8cm,clip]{6142fig2.eps} \end{figure}$ Figure 2: Contribution function for Lyman continuum at the wavelength 911 Å for models A₁ (the first four plots) and model C₁ (the second four plots). The upper pair of the plots for each model represents the viewing along the field lines (from the left side), the lower pair represents the viewing across the field lines (from the bottom). On the left-hand side iso-contours of the temperature (9000, 10 000, 12 000, 15 000, 20 000, 30 000, and 40 000 K) and on the right-hand side iso-contours of the density (0.25, 0.5, 1.0, 1.5, 2.0, and $2.5\times 10^{-13}$ g cm^-3) are shown. The bold dashed line represents the contour of $\tau(911~\AA)=1$ .
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In the text

$\begin{figure} \par\includegraphics[width=16.4cm,clip]{6142fig3.eps} \end{figure}$ Figure 3: Same as in Fig. 2 but at the wavelength 717 Å.
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In the text

$\begin{figure} \par\includegraphics[width=16cm,clip]{6142fig4.eps} \end{figure}$ Figure 4: Same as in Fig. 2 but at the wavelength 504 Å.
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In the text

$\begin{figure} \par\includegraphics[width=8.4cm,clip]{6142fig5.eps} \end{figure}$ Figure 5: Lyman continuum intensity variation along the thread for model C₁. The plot represents one half of the thread from its center.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{6142fig6.eps} \end{figure}$ Figure 6: Lyman continuum for model C₁. The bold line represents an averaged profile seen along the field lines. Other lines belong to different positions along the length of the thread (seen across the field) from the center of the thread (the lowest lines) to the peak (the highest lines).
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{6142fig7.eps} \end{figure}$ Figure 7: Same plot as in Fig. 6, but the intensity is expressed in Watt m^-2 sr^-1 Å^-1 for a better comparison with Parenti et al. (2005).
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{6142fig8.eps} \end{figure}$ Figure 8: Intensity of the Lyman continuum (corrected) from part A_1 of the prominence discussed by Parenti et al. (2005). The bold line represents an averaged profile of model C₁ seen along the field lines. Other lines belong to different positions of model C₁ along the length of the thread (seen across the field).
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{6142fig9.eps} \end{figure}$ Figure 9: Same as in Fig. 8, but for part A_2 of the prominence.
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In the text

$\begin{figure} \par\includegraphics[width=6.5cm,clip]{6142fig1.eps} \end{figure}$	Figure 1: Lyman continuum for models A₁ and C₁. Full lines represent averaged profiles over the width of the thread, dashed lines are mean profiles over the whole length of the thread. Double-arrowed lines belong to the model C₁.
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$\begin{figure} \par\includegraphics[width=16.4cm,clip]{6142fig3.eps} \end{figure}$	Figure 3: Same as in Fig. 2 but at the wavelength 717 Å.
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$\begin{figure} \par\includegraphics[width=16cm,clip]{6142fig4.eps} \end{figure}$	Figure 4: Same as in Fig. 2 but at the wavelength 504 Å.
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$\begin{figure} \par\includegraphics[width=8.4cm,clip]{6142fig5.eps} \end{figure}$	Figure 5: Lyman continuum intensity variation along the thread for model C₁. The plot represents one half of the thread from its center.
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$\begin{figure} \par\includegraphics[width=8.5cm,clip]{6142fig6.eps} \end{figure}$	Figure 6: Lyman continuum for model C₁. The bold line represents an averaged profile seen along the field lines. Other lines belong to different positions along the length of the thread (seen across the field) from the center of the thread (the lowest lines) to the peak (the highest lines).
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$\begin{figure} \par\includegraphics[width=8.5cm,clip]{6142fig7.eps} \end{figure}$	Figure 7: Same plot as in Fig. 6, but the intensity is expressed in Watt m^-2 sr^-1 Å^-1 for a better comparison with Parenti et al. (2005).
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$\begin{figure} \par\includegraphics[width=8.5cm,clip]{6142fig8.eps} \end{figure}$	Figure 8: Intensity of the Lyman continuum (corrected) from part A_1 of the prominence discussed by Parenti et al. (2005). The bold line represents an averaged profile of model C₁ seen along the field lines. Other lines belong to different positions of model C₁ along the length of the thread (seen across the field).
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$\begin{figure} \par\includegraphics[width=8.5cm,clip]{6142fig9.eps} \end{figure}$	Figure 9: Same as in Fig. 8, but for part A_2 of the prominence.
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