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Excitation of inertial modes in a closed grid turbulence experiment under rotation
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10.1063/1.3540660
/content/aip/journal/pof2/23/1/10.1063/1.3540660
http://aip.metastore.ingenta.com/content/aip/journal/pof2/23/1/10.1063/1.3540660

Figures

Image of FIG. 1.
FIG. 1.

Schematic view of the experimental setup, in the “simple grid” configuration. The tank is filled with 52 cm of water and is rotating at an angular velocity of . A square grid of 40 mm mesh is towed by four shafts from the bottom to the top at constant velocity . PIV measurements in a vertical plane are achieved in the rotating frame, based on a laser sheet illuminating the vertical plane and a camera aiming normally at it.

Image of FIG. 2.
FIG. 2.

Times series of the vertical velocity measured at the center of the flow , for 20 realizations performed at (in various colors). The black thick line shows the ensemble average of these time series.

Image of FIG. 3.
FIG. 3.

Total (dashed), mean (continuous), and turbulent (dashed-dotted) kinetic energies as a function of the number of tank rotations from 40 realizations performed at . Inset: ratio of turbulent to total kinetic energy (4), measured at times of maximum mean energy.

Image of FIG. 4.
FIG. 4.

Temporal energy spectrum of the total (dashed), mean (continuous), and turbulent (dashed-dotted) component of the flow as a function of computed from 40 decay realizations performed at , with (a) linear and (b) logarithmic -axis. Inertial modes can develop for angular frequencies . The modes corresponding to the peak frequencies are given in Table I.

Image of FIG. 5.
FIG. 5.

Spatial structure of the five dominating inertial modes listed in Table I, extracted by band-pass filtering of the ensemble-averaged fields. The ellipses show the velocity orbit, and the arrows illustrate the velocity field at a given arbitrary phase of the oscillation. The color of the ellipses traces the ellipticity (see the text for details). (a) ; (b) ; (c) ; (d) ; (e) . Resolution of the fields has been reduced by a factor 6 for a better visibility.

Image of FIG. 6.
FIG. 6.

Vertical velocity field in the wake of the grid. (a) Simple grid configuration. (b) Modified configuration with the inner walls attached to the grid, represented by the six vertical thick lines. The grid is towed from the bottom, and is at the height in these snapshots. (c) Horizontal profile of the vertical velocity, at a distance below the grid (indicated by the horizontal lines in a and b). Continuous line: simple grid configuration. Dashed line: modified configuration with inner walls. The vertical black lines show the locations of the vertical inner walls.

Image of FIG. 7.
FIG. 7.

Schematic view of the modified grid configuration (the outer water tank is not shown; see Fig. 1). Three inner tanks are mounted on the grid, and turbulence is generated by raising the set . Each inner tank consists in four vertical sidewalls, without top and bottom walls.

Image of FIG. 8.
FIG. 8.

Total (dashed), mean (continuous), and turbulent (dashed-dotted) kinetic energies as a function of reduced time from 40 decay realizations performed at with the modified configuration with inner tanks. Inset: ratio of turbulent to total kinetic energy as a function of reduced time with (points) and without (triangles) inner tanks.

Image of FIG. 9.
FIG. 9.

Temporal energy spectrum of the total (dashed), mean (continuous), and turbulent (dashed-dotted) component of the flow as a function of computed from 40 decay realizations performed at with inner tanks, with (a) linear and (b) logarithmic -axis. The dotted line reproduces spectrum of the mean flow for comparison (Fig. 4), obtained with the simple grid configuration.

Tables

Generic image for table
Table I.

Numerical values of normalized frequencies for different modes of order (where is the vertical wavenumber, characterizes the horizontal structure, and is the symmetry of the mode) compared to the experimental peaks in Fig. 4. The uncertainty of the experimental values is . The numerical values are computed for an aspect ratio identical to the experimental one .

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/content/aip/journal/pof2/23/1/10.1063/1.3540660
2011-01-11
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Excitation of inertial modes in a closed grid turbulence experiment under rotation
http://aip.metastore.ingenta.com/content/aip/journal/pof2/23/1/10.1063/1.3540660
10.1063/1.3540660
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