TJ-II:Magnetics: Difference between revisions

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== Mirnov coils ==
== Mirnov coils ==


[[File:TJ-II_Poloidal_Mirnov.png|300px|thumb|right|The poloidal array of Mirnov coils at TJ-II]]
[[File:Mirnov_coils.png|600px|thumb|right|The poloidal array of Mirnov coils at TJ-II]]


TJ-II is fitted with an ample set of Mirnov coils:
[[TJ-II]] is fitted with an ample set of Mirnov coils:
<ref>[http://www.new.ans.org/pubs/journals/fst/a_1283 R. Jiménez-Gómez et al., Fusion Science and Technology '''51''', 20 (2007)]</ref>
<ref>E. Ascasíbar et al, ''Energy content and magnetic configuration scan in TJ-II plasmas'', [http://www-fusion.ciemat.es/SW2005/conferences/madison99/Papers/Ascsibar.pdf 12<sup>th</sup> Int. Stell. Workshop (1999)]</ref>
* Two straight arrays above the plasma column, each with 12 coils, mounted in a 0.5 mm thick stainless steel tube attached to a port flange. The 12 coils are distributed in 4 groups of 3 coils each, separated by a distance of 30 mm. The three coils in each group measure the three cylindrical components (''R'', ''Z'', and ''&phi;'') of the magnetic field. They are located in [[TJ-II:Sectors|sectors]] B5 and C4, at ''&phi;'' = 142 and 218 degrees.
<ref>R. Jiménez-Gómez et al., ''Analysis of Magnetohydrodynamic Instabilities in TJ-II Plasmas'', [http://www.new.ans.org/pubs/journals/fst/a_1283 Fusion Science and Technology '''51''', 20 (2007)]</ref>
* One poloidal array with 15 coils measuring the poloidal field component. This array is located between [[TJ-II:Sectors|sectors]] D4 and D5, at ''&phi;'' = 315 degrees.
<ref>R. Jiménez-Gómez, A. Könies, E. Ascasíbar, F. Castejón, T. Estrada, L. G. Eliseev, A. V. Melnikov, J.A. Jiménez, D. G. Pretty, D. Jiménez-Rey, M.A. Pedrosa, A. de Bustos and S. Yamamoto, ''Alfvén eigenmodes measured in the TJ-II stellarator'', [[doi:10.1088/0029-5515/51/3/033001|Nucl. Fusion '''51''', 3 (2011) 033001]]</ref>
There are two straight arrays above the plasma column, each with 12 coils, mounted in a 0.5 mm thick stainless steel tube attached to a port flange. The 12 coils are distributed in 4 groups of 3 coils each, separated by a distance of 30 mm. The three coils in each group measure the three cylindrical components (''R'', ''&phi;'', and ''Z'') of the magnetic field.
* One straight array in [[TJ-II:Sectors|sector]] B5, at ''&phi;'' = 232&deg;. The corresponding signals in the [[TJ-II:Shot database|TJ-II database]] are called 'MIB5xy', where 'x' is 'R', 'F' (&phi;), or 'Z', and 'y' is the coil number.
* One straight array in [[TJ-II:Sectors|sector]] C4, at ''&phi;'' = 308&deg;.  
* One poloidal array with 15 coils measuring the poloidal field component. This array is located between [[TJ-II:Sectors|sectors]] D4 and D5, at ''&phi;'' = 45&deg;. The signals in the [[TJ-II:Shot database|TJ-II database]] corresponding to these coils are called 'MID5Px', where 'x' is the coil number. This array has been enhanced by 10 additional coils (5 at each end).
* Two toroidal arrays (installed 2018) <ref>E. Ascasíbar et al., ''Measurements of magnetic field fluctuations in TJ-II plasmas with new in-vessel helical arrays of magnetic coils'', [[doi:10.1063/5.0102037|Rev. Sci. Instrum. '''93''' (2022) 093508]]</ref>


== Rogowski coils ==
== Rogowski coils ==
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Two Rogowski coils have been installed in [[TJ-II:Sectors|sectors]] A5 (148.7&deg;) and B4 (211.3&deg;). Since the coils have to surround the plasma column completely, they are located under the protecting tiles of the groove that runs toroidally all along the [[TJ-II:Vacuum system|vacuum vessel]]. For this purpose, 2 mm deep channels were machined on the vacuum side of the groove, at the above mentioned poloidal cross sections, in order to allow enough space for the coils.
Two Rogowski coils have been installed in [[TJ-II:Sectors|sectors]] A5 (148.7&deg;) and B4 (211.3&deg;). Since the coils have to surround the plasma column completely, they are located under the protecting tiles of the groove that runs toroidally all along the [[TJ-II:Vacuum system|vacuum vessel]]. For this purpose, 2 mm deep channels were machined on the vacuum side of the groove, at the above mentioned poloidal cross sections, in order to allow enough space for the coils.


The signals 'Ip_a5_' and 'Ip_b4_' in the [[TJ-II:Shot database|TJ-II database]] provide the corresponding measurements of the net plasma current.
The signals 'Ip_a5_' and 'Ip_b4_' in the [[TJ-II:Shot database|TJ-II database]] provide the corresponding measurements of the net plasma current (in kA).


== Diamagnetic loops ==
== Diamagnetic loops ==


[[File:TJ-II_Diamagnetic_loop.jpg|200px|thumb|left|TJ-II diamagnetic loop]]
[[File:TJ-II_Diamagnetic_loop.jpg|200px|thumb|left|TJ-II diamagnetic loop of [[TJ-II:Sectors|sector]] B4]]


Two internal diamagnetic loops are installed at [[TJ-II:Sectors|sector]] B4 (135&deg;) and C4 (225&deg;).
Two internal diamagnetic loops are installed in [[TJ-II:Sectors|sector]] A5 (135&deg;) and B4 (225&deg;).
They consist of a main loop which encircles the plasma column
They consist of a main loop which encircles the plasma column
and runs under the protecting tiles in the groove region and a compensating loop which
and runs under the protecting tiles in the groove region and a compensating loop which
measures only the vacuum magnetic flux.
measures only the vacuum magnetic flux.


The signal 'W_b4_corr' in the [[TJ-II:Shot database|TJ-II database]] returns the energy content of the plasma, based on the diamagnetic loop in [[TJ-II:Sectors|sector]] B4, corrected for the net plasma current.
The signals 'W_a5_corr_' and 'W_b4_corr_' in the [[TJ-II:Shot database|TJ-II database]] return the energy content of the plasma (in kJ), based on the diamagnetic loop in [[TJ-II:Sectors|sectors]] A5 and B4, corrected for the net plasma current.


== References ==
== References ==
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