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The purpose of the work presented is three-fold: 1

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TEMPORAL SEPARATION OF TURBULENT TIME SERIES:

MEASUREMENTS AND SIMULATIONS

N P Basse1;2, S Zoletnik3, M Saman4, G Antar5 and P K Michelsen1

1 Association EURATOM - Ris National Laboratory, DK-4000 Roskilde, Denmark

2 H.C. rsted Institute, NBIfAPG, DK-2100 Copenhagen, Denmark

3 CAT-SCIENCE Bt. Detrek}o u. 1/b, H-1022 Budapest, Hungary

4 Department of Physics, University of Wisconsin, Madison, Wi., 53706, USA

5 University of California San Diego, La Jolla, California 92093-0417, USA Density uctuations were measured with the CO2 laser based LOcalised TUrbulence Scattering (LOTUS) diagnostic [1] in the Wendelstein 7-AS (W7-AS) stellarator. The discharge analysed in this paper exhibited three connement states: First L-mode, thereafter dithering H-mode and nally ELM-free H-mode (H). We measured density uctuations for a perpendicular wavenumberk? of 14 cm;1 in two toroidally displaced vertical measurement volumes passing through the plasma center. The purpose of the work presented is three-fold:

1. Verify that the basic procedure [2] can be applied to W7-AS plasmas 2. Use simulations to establish criteria for the applicability of the technique 3. Investigate the dierences in the signals between L- and H-modes

Basically, we detect a complex signalS from each volume and can construct the phase derivative with respect to time

S =X + iY =Aei @t = [X@tY ;Y@tX]=A2; (1) whose sign determines the direction of the poloidal propagation of the uctuations. To illustrate point 3 above, gure 1 shows the amplitude of the measured density

uctuation signal (top) and the corresponding phase derivative (bottom) for three 100

s time windows.

Figure 1: Amplitude (top) and phase derivative (bottom) of the signal from volume 1.

Left: L-mode, center: H-mode and right: Background. Data shown was bandpass ltered [1 kHz, 1 MHz].

References

[1] Saman M et al., Rev. Sci. Instrum. 72 (2001) 2579

[2] Antar G et al., Plasma Phys. Control. Fusion 41 (1999) 733

Referencer

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Steven Borish Department of Human Development California State University, East Bay Hayward, CA

Steven Borish Department of Human Development California State University, East Bay Hayward, CA

Figure 5: Left: Wavenumber spectrum of L-mode density uctuations; power-law ts to the 3 smallest and 5 largest wavenumbers is also shown, right: H-mode wavenumber spectrum

[3] Temporal separation of the density fluctuation signal measured by light scattering, G.Antar et al., Plasma Phys. Fusion 41 (1999) 733 [4] Turbulence reduction and poloidal

[3] Temporal separation of the density fluctuation signal measured by light scattering, G.Antar et al., Plasma Phys. Fusion 41 (1999) 733 [4] Turbulence reduction and poloidal

[3] Temporal separation of the density fluctuation signal measured by light scattering, G.Antar et al., Plasma Phys. Fusion 41 (1999) 733 [4] Turbulence reduction and poloidal

[3] Temporal Separation of the Density Fluctuation Signal Measured by Light Scattering, G.Antar et al., Plasma Phys. Fusion

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