$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f1.eps} \end{figure}$ Figure 1: Case of apex (symmetric) heating: periodogram (spectrum) of the velocity and density oscillatory component times series outputted in the following three points: loop apex (solid curve), 1/4 (dash-dotted curve) and 1/6 (dashed curve) of the effective loop length (48 Mm), i.e. at s=0,-12,-16 Mm.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f2.eps} \end{figure}$ Figure 2: Case of apex (symmetric) heating: oscillatory components of time series outputted at $\pm$ 6 Mm and $\pm$ 18 Mm in the time interval of 2500-2800 s. The solid curve shows plasma number density in units of 10¹¹ cm^-3. The dashed curve shows velocity normalized to 400 km s^-1.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f3.eps} \end{figure}$ Figure 3: Case of single footpoint (asymmetric) heating: average temperature, temperature at apex, and number density at the apex as functions of time.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f4.eps} \end{figure}$ Figure 4: Time-distance plots of the velocity and density oscillatory components in the time interval of 2400-2700 s for the case of single footpoint (asymmetric) heating.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f6.eps} \end{figure}$ Figure 6: As in Fig. 2, but for the case of single footpoint (asymmetric) heating. Time interval here is 2400-2700 s.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f1.eps} \end{figure}$	Figure 1: Case of apex (symmetric) heating: periodogram (spectrum) of the velocity and density oscillatory component times series outputted in the following three points: loop apex (solid curve), 1/4 (dash-dotted curve) and 1/6 (dashed curve) of the effective loop length (48 Mm), i.e. at s=0,-12,-16 Mm.
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f2.eps} \end{figure}$	Figure 2: Case of apex (symmetric) heating: oscillatory components of time series outputted at $\pm$ 6 Mm and $\pm$ 18 Mm in the time interval of 2500-2800 s. The solid curve shows plasma number density in units of 10¹¹ cm^-3. The dashed curve shows velocity normalized to 400 km s^-1.
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f3.eps} \end{figure}$	Figure 3: Case of single footpoint (asymmetric) heating: average temperature, temperature at apex, and number density at the apex as functions of time.
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f4.eps} \end{figure}$	Figure 4: Time-distance plots of the velocity and density oscillatory components in the time interval of 2400-2700 s for the case of single footpoint (asymmetric) heating.
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f5.eps} \vspace*{4mm} \end{figure}$	Figure 5: As is Fig. 1 but for the case of single footpoint (asymmetric) heating. Time interval here is 2400-2700 s.
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$\begin{figure} \par\includegraphics[width=8.8cm,clip]{ms0299f6.eps} \end{figure}$	Figure 6: As in Fig. 2, but for the case of single footpoint (asymmetric) heating. Time interval here is 2400-2700 s.
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