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TJ-II:Fast camera: Difference between revisions
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[[TJ-II]] disposes of | [[TJ-II]] disposes of various fast camera systems for plasma imaging | ||
<ref name="Alonso">[http://dx.doi.org/10.1088/0741-3335/48/12B/S44 J.A. Alonso et al, ''Impact of different confinement regimes on the two-dimensional structure of edge turbulence'', Plasma Phys. Control. Fusion '''48''' (2006) B465-B473]</ref> | <ref name="Alonso">[http://dx.doi.org/10.1088/0741-3335/48/12B/S44 J.A. Alonso et al, ''Impact of different confinement regimes on the two-dimensional structure of edge turbulence'', Plasma Phys. Control. Fusion '''48''' (2006) B465-B473]</ref> | ||
<ref name="Carralero">[http://dx.doi.org/10.1016/j.jnucmat.2009.01.140 D. Carralero et al, ''Turbulence studies by fast camera imaging experiments in the TJII stellarator'', Journal of Nuclear Materials '''390-391''' (2009) 457-460]</ref> | <ref name="Carralero">[http://dx.doi.org/10.1016/j.jnucmat.2009.01.140 D. Carralero et al, ''Turbulence studies by fast camera imaging experiments in the TJII stellarator'', Journal of Nuclear Materials '''390-391''' (2009) 457-460]</ref> | ||
<ref name="delaCal">[http://onlinelibrary.wiley.com/doi/10.1002/ctpp.201000039/pdf E. de la Cal et al, ''The visible intensified cameras for plasma imaging in the TJ-II stellarator'', Contrib. Plasma Phys. (2010)]</ref>. | <ref name="delaCal">[http://onlinelibrary.wiley.com/doi/10.1002/ctpp.201000039/pdf E. de la Cal et al, ''The visible intensified cameras for plasma imaging in the TJ-II stellarator'', Contrib. Plasma Phys. (2010)]</ref>. | ||
The main system is located in [[TJ-II:Sectors|sector]] B8, [[TJ-II:Ports|port]] B8TANG, viewing | The main system is located in [[TJ-II:Sectors|sector]] B8, [[TJ-II:Ports|port]] B8TANG, viewing the [[TJ-II:Limiter|poloidal limiter]] in sector C3 tangentially. | ||
== Cameras == | == Cameras == | ||
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== Videos == | == Videos == | ||
Below are some examples of movies recorded with the fast camera system of TJ-II. | |||
=== Limiter Recycling === | === Limiter Recycling === | ||
[[File: | [[File:24119.jpg|300px|link=media:24119.gif|Limiter recycling movie]] | ||
Without filter and 75 mm lens. Speed: 54000 fps. Exposure time: 9μs. V: 650 V. | Without filter and 75 mm lens. Speed: 54000 fps. Exposure time: 9μs. V: 650 V. | ||
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=== Helium Puffing === | === Helium Puffing === | ||
[[File: | [[File:24080.jpg|300px|link=media:24080.gif|Helium puffing movie]] | ||
Without filter and 75 mm lens. Speed: 100000 fps. Exposure time: 1μs. V: 700 V. | Without filter and 75 mm lens. Speed: 100000 fps. Exposure time: 1μs. V: 700 V. | ||
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=== Surface Interaction === | === Surface Interaction === | ||
[[File: | [[File:18152.jpg|300px|link=media:18152.gif|Surface interaction movie]] | ||
TJ-II plasma observed from a tangential port at 17.5 kHz sampling rate, with a lithium filter and image intensifier. In the field of view, the two most prominent areas of plasma-wall interaction can be seen: the poloidal limiter (lower) and the hardcore (helical limiter). As the plasma transits form ECH to NBI plasmas, the interaction level diminishes and becomes predominantly centered in the limiter. <ref name="Carralero"></ref> From the lithium emission fluctuations information on the electron density fluctuations can be gained. <ref name="delaCal"></ref> | TJ-II plasma observed from a tangential port at 17.5 kHz sampling rate, with a lithium filter and image intensifier. In the field of view, the two most prominent areas of plasma-wall interaction can be seen: the poloidal limiter (lower) and the hardcore (helical limiter). As the plasma transits form ECH to NBI plasmas, the interaction level diminishes and becomes predominantly centered in the limiter. <ref name="Carralero"></ref> From the lithium emission fluctuations information on the electron density fluctuations can be gained. <ref name="delaCal"></ref> | ||
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=== Dust === | === Dust === | ||
[[File: | [[File:Polvo1b.jpg|300px|link=media:Polvo1b.gif|Dust movie]] | ||
First insertion of the poloidal limiter after a lithiation of the vacuum vessel. Tangential observation, 15 kHz sampling rate. The ejection of lithium flakes from the carbon surface can be seen clearly at the beginning of the discharge. At the end of the video, as the plasma becomes colder, the flakes penetrate deeper into it until they float freely in the post-discharge plasmoid. | First insertion of the poloidal limiter after a lithiation of the vacuum vessel. Tangential observation, 15 kHz sampling rate. The ejection of lithium flakes from the carbon surface can be seen clearly at the beginning of the discharge. At the end of the video, as the plasma becomes colder, the flakes penetrate deeper into it until they float freely in the post-discharge plasmoid. | ||