File:Cross section 1shift 2elong 3triang 4square.png: Difference between revisions

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(Illustration of the m=1,2,3, and 4 tokamak plasma cross section shape perturbations: m=1 is the Shafranov shift, which displaces the center of a flux surface from the nominal geometric center of the LCFS, m=2 is elongation, which stretches the plasma vertically, m=3 is triangularity, which is increased by pulling the X-points to smaller R, and m=4 is squareness.)
 
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Latest revision as of 22:48, 30 March 2023

Summary

Illustration of the m=1,2,3, and 4 tokamak plasma cross section shape perturbations: m=1 is the Shafranov shift, which displaces the center of a flux surface from the nominal geometric center of the LCFS, m=2 is elongation, which stretches the plasma vertically, m=3 is triangularity, which is increased by pulling the X-points to smaller R, and m=4 is squareness.

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current22:48, 30 March 2023Thumbnail for version as of 22:48, 30 March 2023520 × 220 (52 KB)Eldond (talk | contribs)
22:44, 30 March 2023Thumbnail for version as of 22:44, 30 March 2023520 × 125 (29 KB)Eldond (talk | contribs)Illustration of the m=1,2,3, and 4 tokamak plasma cross section shape perturbations: m=1 is the Shafranov shift, which displaces the center of a flux surface from the nominal geometric center of the LCFS, m=2 is elongation, which stretches the plasma vertically, m=3 is triangularity, which is increased by pulling the X-points to smaller R, and m=4 is squareness.

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