124
edits
TJ-II:Impurity density and potential asymmetries: Difference between revisions
Jump to navigation
Jump to search
TJ-II:Impurity density and potential asymmetries (view source)
Revision as of 16:25, 24 January 2017
, 24 January 2017→Description of the activity, including motivation/objectives and experience of the proponent (typically one-two pages)
Jose.regana (talk | contribs) |
Jose.regana (talk | contribs) |
||
| Line 26: | Line 26: | ||
These, in turn, should result in an anisotropic radiation over each flux surface and consequently | These, in turn, should result in an anisotropic radiation over each flux surface and consequently | ||
a radially asymmetric radiation pattern should follow. | a radially asymmetric radiation pattern should follow. | ||
In the present experiment the analysis of the radial profiles and time evolution of the plasma emissivity using the TJ-II bolometry | |||
system <ref> M. A. Ochando ''et al.'' ''Up-down and in-out asymmetry monitoring based on broadband radiation detectors'' Fusion Sci. and Technol. '''50''' 313 (2006) </ref> after the inyection | |||
of some selected impurities by gas puffing is proposed. The experiment aims at studying the above-mentioned link between the radially assymetric | |||
emissivity and the measured and predicted <math>\Phi_1</math>. The measurement and evolution of <math>\Phi_1</math> will be tracked | |||
during the discharges using the duplicated Langmuir probe system plasma floating potential measurements. | |||
Numerical calculations of <math>\Phi_1</math> will be carried out with the neoclassical version of the code EUTERPE | |||
at different radial locations. | |||
The application of fluid tools is also foreseen for the comparison between simulations and with the experimental results. | |||
== Description of required resources == | == Description of required resources == | ||