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$\begin{figure} \par\includegraphics[width=7.5cm,clip]{9128fig1.ps}\end{figure}$ Figure 1: Upper panel: number density (solid line) and temperature (triple-dash dot line) profiles for a hydrostatic loop of length L = 8 $\times$ 10⁹ cm and apex temperature $T_{\rm a}=4.0$ MK, with a uniform volumetric heating rate of $E_{\rm H} = 4.9$ $\times$ 10^-3 erg cm^-3 s^-1 required to maintain equilibrium. Lower panel: standing fundamental mode acoustic wave, with v₀=10⁷ cm s^-1.
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In the text

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128figb.ps}\end{figure}$ Figure 2: The absolute, normalised average velocity, $\left\vert\bar{v} / \bar{v_0}\right\vert$ , during the decay phase of the fundamental mode standing wave, for $T_{\rm a}$ = 0.5 MK, 2 $\times$ $10^9 \le L \le 16$ $\times$ 10⁹ cm and an equilibrium ionisation balance.
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In the text

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig2.ps}\end{figure}$ Figure 3: Exponentially decaying curve fits to the peaks in $\left\vert\bar{v} / \bar{v_0}\right\vert$ , along loops with 2 $\times$ $10^9 \le L \le 16$ $\times$ 10⁹ cm, during the decay phase of the fundamental mode standing wave. The curve fits correspond to the mode decay for an equilibrium (+ symbol, solid line) and a non-equilibrium (* symbol, triple-dash dot line) ionisation balance. The apex temperature, $T_{\rm a}$ , of the initial hydrostatic equilibrium is 0.5 MK.
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In the text

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig3.ps}\end{figure}$ Figure 4: As Fig. 3 for $T_{\rm a}=1.0$ MK.
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In the text

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig4.ps}\end{figure}$ Figure 5: As Fig. 3 for $T_{\rm a}=2.0$ MK.
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In the text

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig5.ps}\end{figure}$ Figure 6: As Fig. 3 for 8 $\times$ $10^9 \le L \le 16$ $\times$ 10⁹ cm and $T_{\rm a}=4.0$ MK.
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In the text

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig6.ps}\end{figure}$ Figure 7: As Fig. 3 for 8 $\times$ $10^9 \le L \le 16$ $\times$ 10⁹ cm and $T_{\rm a}=8.0$ MK.
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In the text

$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128fig7.ps}\end{figure}$ Figure 8: The non-equilibrium ionisation balance (solid line) of He, C, O and Fe for the case L=8 $\times$ 10⁹ cm and $T_{\rm a}=0.5$ MK at $t=\tau$ (966 s in Table 3). The equilibrium ionisaton balance (dotted line) is plotted for comparison.
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In the text

$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128fig8.ps}\end{figure}$ Figure 9: As Fig. 8 for L=8 $\times$ 10⁹ cm and $T_{\rm a}=1.0$ MK at t=968 s.
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In the text

$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128fig9.ps}\end{figure}$ Figure 10: As Fig. 8 for L=8 $\times$ 10⁹ cm and $T_{\rm a}=2.0$ MK at t=866 s.
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In the text

$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128figc.ps}\end{figure}$ Figure 11: As Fig. 8 for L=8 $\times$ 10⁹ cm and $T_{\rm a}=4.0$ MK at t=792 s.
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In the text

$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128figd.ps}\end{figure}$ Figure 12: As Fig. 8 for L=8 $\times$ 10⁹ cm and $T_{\rm a}=8.0$ MK at t=556 s.
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In the text

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128figb.ps}\end{figure}$	Figure 2: The absolute, normalised average velocity, $\left\vert\bar{v} / \bar{v_0}\right\vert$ , during the decay phase of the fundamental mode standing wave, for $T_{\rm a}$ = 0.5 MK, 2 $\times$ $10^9 \le L \le 16$ $\times$ 10⁹ cm and an equilibrium ionisation balance.
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$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig3.ps}\end{figure}$	Figure 4: As Fig. 3 for $T_{\rm a}=1.0$ MK.
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$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig4.ps}\end{figure}$	Figure 5: As Fig. 3 for $T_{\rm a}=2.0$ MK.
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$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig5.ps}\end{figure}$	Figure 6: As Fig. 3 for 8 $\times$ $10^9 \le L \le 16$ $\times$ 10⁹ cm and $T_{\rm a}=4.0$ MK.
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$\begin{figure} \par\includegraphics[width=7.7cm,clip]{9128fig6.ps}\end{figure}$	Figure 7: As Fig. 3 for 8 $\times$ $10^9 \le L \le 16$ $\times$ 10⁹ cm and $T_{\rm a}=8.0$ MK.
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$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128fig7.ps}\end{figure}$	Figure 8: The non-equilibrium ionisation balance (solid line) of He, C, O and Fe for the case L=8 $\times$ 10⁹ cm and $T_{\rm a}=0.5$ MK at $t=\tau$ (966 s in Table 3). The equilibrium ionisaton balance (dotted line) is plotted for comparison.
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$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128fig8.ps}\end{figure}$	Figure 9: As Fig. 8 for L=8 $\times$ 10⁹ cm and $T_{\rm a}=1.0$ MK at t=968 s.
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$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128fig9.ps}\end{figure}$	Figure 10: As Fig. 8 for L=8 $\times$ 10⁹ cm and $T_{\rm a}=2.0$ MK at t=866 s.
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$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128figc.ps}\end{figure}$	Figure 11: As Fig. 8 for L=8 $\times$ 10⁹ cm and $T_{\rm a}=4.0$ MK at t=792 s.
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$\begin{figure} \par\includegraphics[width=7.6cm,clip]{9128figd.ps}\end{figure}$	Figure 12: As Fig. 8 for L=8 $\times$ 10⁹ cm and $T_{\rm a}=8.0$ MK at t=556 s.
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