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<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 [[TJ-II:Limiter|poloidal limiter]] in sector C3 tangentially. | 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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The dynamic range of the sensor is 8 bits, and the memory size is 8 GB. | The dynamic range of the sensor is 8 bits, and the memory size is 8 GB. | ||
== Image Intensifier for Fast Camera== | == Image Intensifier for Fast Camera== | ||
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[[File:TJ-II_Fast_camera_diagram.jpg|800px|thumb|center|Schematic diagram of the TJ-II fast camera installation]] | [[File:TJ-II_Fast_camera_diagram.jpg|800px|thumb|center|Schematic diagram of the TJ-II fast camera installation]] | ||
== Videos == | == Videos == | ||
Below are some examples of movies recorded with the fast camera system of TJ-II. Click on the images to see the corresponding movie. | Below are some examples of movies recorded with the fast camera system of TJ-II. Click on the images to see the corresponding movie. | ||
=== Double imaging to visualize the fine structure of Blobs=== | === Double imaging to visualize the fine structure of Blobs=== | ||
[[File:Double_Imaging.jpg|300px|link=http://www-fusion.ciemat.es/fileshare/doc_exchange/camaras/video_DOUBLE_IMAGING.mp4]] | [[File:Double_Imaging.jpg|300px|link=http://www-fusion.ciemat.es/fileshare/doc_exchange/camaras/video_DOUBLE_IMAGING.mp4]] | ||
A visible fast camera coupled with an image intensifier was employed to view turbulent coherent plasma structures (Blobs) at the gas plume being puffed through a poloidal limiter. The image intensifier amplifies the light intensity thereby allowing the imaging system to be operated at ultra-short exposure times down to 100 ns. | A visible fast camera coupled with an image intensifier was employed to view turbulent coherent plasma structures (Blobs) at the gas plume being puffed through a poloidal limiter. The image intensifier amplifies the light intensity thereby allowing the imaging system to be operated at ultra-short exposure times down to 100 ns. | ||
To distinguish real physical signal from noise we get two simultaneous images with the same view and compare them. We call this Double Imaging technique and it allowed us to validate the detected blob shape to scales down to a few millimetres, limited by our optical resolution. | To distinguish real physical signal from noise we get two simultaneous images with the same view and compare them. We call this Double Imaging technique and it allowed us to validate the detected blob shape to scales down to a few millimetres, limited by our optical resolution. | ||
=== Double Imaging of two He I lines #25623=== | === Double Imaging of two He I lines #25623=== | ||
[[File:25623wComm_Photo000001.jpg|300px|link=http://www-fusion.ciemat.es/camaras/25623wComm.avi|Limiter recycling movie]] | [[File:25623wComm_Photo000001.jpg|300px|link=http://www-fusion.ciemat.es/camaras/25623wComm.avi|Limiter recycling movie]] | ||
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With He I filters (706 nm and 728 nm) and 75 mm lens. Speed: 16000 fps. Exposure time: 60μs. V: 750 V. | With He I filters (706 nm and 728 nm) and 75 mm lens. Speed: 16000 fps. Exposure time: 60μs. V: 750 V. | ||
ECH and NBI plasma with <n<sub>e</sub>>. Recycling at limiter inserted 25 mm inside the LCFS. Edge Mode Instabilities after density increase with strong crashes and collapse. From the ratio of the filtered lines the <n<sub>e</sub>> and <T<sub>e</sub>> can be obtained [4]. | ECH and NBI plasma with <n<sub>e</sub>>. Recycling at limiter inserted 25 mm inside the LCFS. Edge Mode Instabilities after density increase with strong crashes and collapse. From the ratio of the filtered lines the <n<sub>e</sub>> and <T<sub>e</sub>> can be obtained [4]. | ||
=== Limiter Recycling === | === Limiter Recycling === | ||
[[File:24119.jpg|300px|link=media:24119.gif|Limiter recycling movie]] | [[File:24119.jpg|300px|link=media:24119.gif|Limiter recycling movie]] | ||
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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. | ||
ECH plasma with <n<sub>e</sub>> = 5x10<sup>18</sup> m<sup>-3</sup>. Recycling at limiter positioned on the LCFS. The bright spot is Blackbody radiation from a glowing Langmuir probe on the limiter corner. | ECH plasma with <n<sub>e</sub>> = 5x10<sup>18</sup> m<sup>-3</sup>. Recycling at limiter positioned on the LCFS. The bright spot is Blackbody radiation from a glowing Langmuir probe on the limiter corner. | ||
=== Helium Puffing === | === Helium Puffing === | ||
[[File:24080.jpg|300px|link=media:24080.gif|Helium puffing movie]] | [[File:24080.jpg|300px|link=media:24080.gif|Helium puffing movie]] | ||
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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. | ||
ECH plasma with <n<sub>e</sub>> = 5x10<sup>18</sup> m<sup>-3</sup>. Helium puffing through the limiter 35 mm outside LCFS. | ECH plasma with <n<sub>e</sub>> = 5x10<sup>18</sup> m<sup>-3</sup>. Helium puffing through the limiter 35 mm outside LCFS. | ||
=== Lithium emission (Li I filter) === | === Lithium emission (Li I filter) === | ||
[[File:18152.jpg|300px|link=media:18152.gif|Surface interaction movie]] | [[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> | ||
=== Dust === | === Dust === | ||
[[File:Polvo1b.jpg|300px|link=media:Polvo1b.gif|Dust movie]] | [[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. | ||
== References == | == References == | ||
<references /> | <references /> |
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