Speaker
Ondřej Grover
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Description
The Reynolds stress and is gradient is a key quantity for the experimental
validation of theories of turbulence suppression by zonal flows and other
sheared flows. A common diagnostic for its measurement is an array of
appropriately positioned Langmuir probes. However, simultaneous Reynolds stress profile measurements with Langmuir and ball-pen
probes show a strong influence of electron temperature fluctuations on the final measured
value. The diagnostic used on COMPASS is a
complex probe head mounted on a horizontal reciprocating manipulator which allows measurements deep in the edge plasma. This enables a direct measurement of $E_r$ as well as the
radial-poloidal component of the Reynolds stress tensor $R_{rp}$.
While the Reynolds stress gradients calculated from either probe type are
found to be comparable in the close vicinity of the LCFS, they are significantly different
even in terms of polarity deeper inside the LCFS. Specifically, the $R_{rp}$ calculated from Langmuir probes is found to be lower than from
ball-pen probes due to high-frequency $T_e$ fluctuations. The radial profile of
the differences in the measured values is examined in detail and a correction
for the Langmuir probe measurement in
terms of local plasma parameters measurable by Langmuir probes is proposed.
Primary author
Ondřej Grover
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Co-authors
Jakub Seidl
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Jiří Adámek
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Josef Havlíček
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Martin Hron
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Matěj Tomeš
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Petr Vondráček
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Radomír Pánek
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
Vladimír Weinzettl
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)
team COMPASS
(Institute of Plasma Physics, The Czech Academy of Sciences, Prague, Czech Republic)