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  • .../math> is the flux surface label and <math>\theta, \phi</math> are <math>2\pi</math>-periodic poloidal and toroidal-like angles. = \frac{d\psi}{d V}\int_0^{2\pi}\int_0^{2\pi}\Phi\; \sqrt{g} d\theta d\phi
    22 KB (3,727 words) - 12:49, 26 January 2023
  • ...reduced resolutions. After installation and out-of-window focusing, He and PI recordings in the plasma are required before the experimental sessions. .... We intend to investigate how impurity injection by LBO immediately after PI affects transport.
    57 KB (8,410 words) - 12:54, 26 January 2024
  • ...chi = \frac{I_{tor}}{2\pi}\mathbf{B}\cdot\nabla\theta + \frac{I_{pol}^d}{2\pi}\mathbf{B}\cdot\nabla\phi + \mathbf{B}\cdot\nabla\tilde\chi~. \mathbf{B}\cdot\nabla\tilde\chi = B^2 - \frac{1}{4\pi^2\sqrt{g}}\left(I_{tor}\Psi_{pol}' + I_{pol}^d\Psi_{tor}' \right)~,
    4 KB (655 words) - 12:29, 11 October 2012
  • \frac{-I'_{tor}\Psi'_{pol} + I'_{pol}\Psi'_{tor}}{4\pi^2\sqrt{g_f}} :<math>(-{I}'_{tor}{\Psi}'_{pol} + {I}'_{pol}{\Psi}'_{tor})= 4\pi^2{p}'\langle(\sqrt{g_f})^{-1}\rangle^{-1} = p'V'~.
    4 KB (683 words) - 11:59, 12 August 2011
  • ...le_P}{B_\theta^2(a)} = \frac{2 \pi \int_0^a{B_\theta^2(\rho) \rho d\rho}}{\pi a^2 B_\theta^2(a)}</math> Using Ampère's Law (<math>2 \pi a B_\theta(a) = \mu_0 I</math>), one obtains <ref name="Freidberg"/>
    3 KB (458 words) - 12:30, 26 January 2023
  • ...of core turbulence is reduced strongly for a short time scale (1 ms) after PI, this being followed by an increase in the evolution of plasma density and ...uations with the same system. Measurement of edge plasma turbulence during PI with Langmuir probes.
    3 KB (457 words) - 14:41, 23 February 2021
  • ...ar [[tokamak]], the [[Toroidal coordinates|poloidal circumference]] is ''2&pi;r''. The connection length is <math>L = 2\pi r/\sin(\alpha)</math>,
    1 KB (229 words) - 12:36, 26 January 2023
  • The rotational transform (or field line pitch) ''&iota;/2&pi;'' is defined as the number of poloidal transits per single toroidal transi :<math>\frac{\iota}{2 \pi} = \frac{d \psi}{d \Phi}</math>
    2 KB (347 words) - 12:31, 26 January 2023
  • |Rotational transform, ''&iota;/2&pi;'': || 0.9 - 2.5 || * [[TJ-II:Pellet injector|Pellet injector]] (PI)
    9 KB (1,177 words) - 12:45, 22 February 2022
  • ...ed on the volume ''V(&psi;)'' enclosed in a flux surface (using ''V'' = 2 &pi;<sup>2</sup>''Rr''<sub>eff</sub><sup>2</sup>) * Based on the surface area ''S(&psi;)'' of a flux surface (using ''S'' = 4 &pi;<sup>2</sup>''Rr''<sub>eff</sub>)
    6 KB (944 words) - 11:25, 6 October 2019
  • PI Checks: We will require some time at 9 am to check out and condition the PI.
    3 KB (462 words) - 11:50, 7 October 2019
  • ...diamagnetic energy content up to 40% higher to in reference shots without PI. Moreover, the energy confinement time, as determined using a diamagnetic l
    3 KB (512 words) - 10:52, 23 September 2021
  • ...IEC (NBI) compared to density evolution without a confinement enhancement (PI in ECRH).
    3 KB (463 words) - 10:46, 23 September 2021
  • ...eliac TJ-II will be used. It is equipped with a cryogenic pellet injector (PI) for fuelling with solid hydrogen. During previous projects it was found th The PI and TESPEL systems on TJ-II share a common injection system and guide lines
    5 KB (693 words) - 09:30, 11 April 2024
  • ...ta ^{3}(\vec R - \vec R_p)\delta(v_{||} - v_{||p})\delta(\mu - \mu_p) /(2 \pi B),
    4 KB (643 words) - 09:20, 28 June 2022
  • :<math>s_{\rm local} = 2 \pi \vec{h} \cdot \vec{\nabla} \times \vec{h}</math>
    2 KB (230 words) - 15:41, 3 April 2018
  • :<math>n_G = \frac{I_p}{\pi a^2}</math>
    1 KB (217 words) - 10:42, 9 July 2020
  • ...oordinate <math>\eta</math> is a poloidal angle and runs from 0 to <math>2\pi</math>.
    6 KB (836 words) - 12:13, 12 December 2023
  • |Rotational transform, ''&iota;/2&pi;'': || 5/6-5/4 ||
    8 KB (1,072 words) - 08:37, 10 April 2023
  • :<math>p(y|x) = \frac{1}{\sqrt{2\pi \Delta y^2}}\exp \left ( -\frac{(y-y_0)^2}{2\Delta y^2}\right )</math>
    8 KB (1,274 words) - 12:41, 26 January 2023
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