$\begin{figure} \par\includegraphics[trim=1cm 0.5cm 1.5cm 1.5cm, clip, width=7cm]{1258fi1} \end{figure}$ Figure 1: Uncertainty on the velocity measurements $\sigma _v$ for a 45 mn time averaging with respect to different instrumental cadences.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[trim=0.5cm 0cm 0.5cm 0.5cm, width=7cm]{1258fi2} \end{figure}$ Figure 2: Top: distributions of balltracked velocities at 3 cadences for test data on 11 November 2007. Bottom: distribution of the balltracked velocities for the 2007 April 10 dataset. Time average is 30 mn and spatial smoothing has an FWHM of 4 Mm.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=8.5cm]{1258fi7} \end{figure}$ Figure 5: Sketch of the Lagrangian representation of a vortex flow. The concentric circles represent the iso-contours of the tangential velocity increasing toward the center of the flow. The segmented arrows represent massless chained corks.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[trim= 1cm 1cm 0cm 0cm, clip, width=8.5cm, keepaspectratio=true]{1258fi9} \end{figure}$ Figure 7: Zoomed-in velocity field of Fig. 4 with a filled contour of the maximum Ca II emission. The red square indicates the patch represented in Fig. 8.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=8.5cm, keepaspectratio=true]{1258fi10} \end{figure}$ Figure 8: Na I stokes V (FG/SOT) from the November dataset at 3 different times centered on the vortex flows. The FOV of ${\sim }20\times 20$ Mm² is designated by the red square in Fig. 7. The yellow arrow points at a unipolar (black) magnetized fluid element. The dashed cross is a graphical fixed reference to help visualize the relative motions.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[trim=1cm 0.5cm 1.5cm 1.5cm, clip, width=7cm]{1258fi1} \end{figure}$	Figure 1: Uncertainty on the velocity measurements $\sigma _v$ for a 45 mn time averaging with respect to different instrumental cadences.
Open with DEXTER

$\begin{figure} \par\includegraphics[trim=0.5cm 0cm 0.5cm 0.5cm, width=7cm]{1258fi2} \end{figure}$	Figure 2: Top: distributions of balltracked velocities at 3 cadences for test data on 11 November 2007. Bottom: distribution of the balltracked velocities for the 2007 April 10 dataset. Time average is 30 mn and spatial smoothing has an FWHM of 4 Mm.
Open with DEXTER

$\begin{figure} \par\mbox{\subfigure[10\textsuperscript{th} Apr. 2007 18:15 UTC]{... ... 1cm 0cm 0.5cm, clip, width=8cm, keepaspectratio=true]{1258fi4} }}\end{figure}$	Figure 3: Velocity vector fields of 2007 April 10. The FOV is ${\sim }86\times 86$ Mm². Red square : 15.5 Mm (diagonal).
Open with DEXTER

$\begin{figure} \par\mbox{\subfigure[07\textsuperscript{th} Nov. 2007 03:37 UTC]{... ... 1cm 0cm 0.5cm, clip, width=8cm, keepaspectratio=true]{1258fi6} }}\end{figure}$	Figure 4: Velocity vector fields of 2007 November 7. The FOV is ${\sim }86\times 86$ Mm². Red square : 21 Mm (diagonal).
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.5cm]{1258fi7} \end{figure}$	Figure 5: Sketch of the Lagrangian representation of a vortex flow. The concentric circles represent the iso-contours of the tangential velocity increasing toward the center of the flow. The segmented arrows represent massless chained corks.
Open with DEXTER

$\begin{figure} \par\includegraphics[trim=3cm 1cm 1cm 1cm, clip, width=8cm, keepaspectratio=true]{1258fi8} \end{figure}$	Figure 6: Eulerian representation of the flow in the red square of Fig. 4. The colored background is the normalized vertical curl.
Open with DEXTER

$\begin{figure} \par\includegraphics[trim= 1cm 1cm 0cm 0cm, clip, width=8.5cm, keepaspectratio=true]{1258fi9} \end{figure}$	Figure 7: Zoomed-in velocity field of Fig. 4 with a filled contour of the maximum Ca II emission. The red square indicates the patch represented in Fig. 8.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.5cm, keepaspectratio=true]{1258fi10} \end{figure}$	Figure 8: Na I stokes V (FG/SOT) from the November dataset at 3 different times centered on the vortex flows. The FOV of ${\sim }20\times 20$ Mm² is designated by the red square in Fig. 7. The yellow arrow points at a unipolar (black) magnetized fluid element. The dashed cross is a graphical fixed reference to help visualize the relative motions.
Open with DEXTER