<p>The 2-D edge plasma fluid transport code, UEDGE has been used to simulate the edge and scrape-off layer regions of circular limiter plasmas of ADITYA-U. The computational mesh defining the limiter geometry of ADITYA-U has been introduced in the UEDGE code through an in-house developed routine. It has successfully been integrated with the UEDGE code and the measured radial profile of electron density (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(n_e\)</EquationSource> </InlineEquation>) in the edge region is modelled using the simulations. The plasma discharge for the present study has plasma current <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\text {I}_{P}\)</EquationSource> </InlineEquation> <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\sim\)</EquationSource> </InlineEquation> 130 kA, duration <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\sim\)</EquationSource> </InlineEquation> 150 ms, chord-averaged electron density <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\sim\)</EquationSource> </InlineEquation> 1.3 <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\times\)</EquationSource> </InlineEquation> <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(10^{19}\)</EquationSource> </InlineEquation> <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\text {m}^{-3}\)</EquationSource> </InlineEquation>, and central electron temperature <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\sim\)</EquationSource> </InlineEquation> 270 eV has been observed. The maximum toroidal magnetic field is <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\sim\)</EquationSource> </InlineEquation> 1.2 T. It has been found that an inward convective velocity, <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\text {v}_{conv}\)</EquationSource> </InlineEquation> <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\sim\)</EquationSource> </InlineEquation> 1.5 m/s is required in addition to the constant perpendicular diffusion coefficient, <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\text {D}_{\perp }\)</EquationSource> </InlineEquation> <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\sim\)</EquationSource> </InlineEquation> 0.2 <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\text {m}^2\)</EquationSource> </InlineEquation>/s to adequately match the measured <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\text {n}_e\)</EquationSource> </InlineEquation> profile in typical discharges of ADITYA-U. The value of <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\text {D}_{\perp }\)</EquationSource> </InlineEquation> <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\sim\)</EquationSource> </InlineEquation> 0.2 <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(\text {m}^2\)</EquationSource> </InlineEquation>/s is found to lie between the estimated neoclassical diffusivity and Bohm diffusivity.</p>

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Effect of convective transport in edge and scrape-off-layer plasmas of ADITYA-U tokamak

  • Ritu Dey,
  • M. B. Chowdhuri,
  • Joydeep Ghosh,
  • Tanmay M. Macwan,
  • Kaushlender Singh,
  • H. Raj,
  • R. L. Tanna,
  • R. Manchanda,
  • Deepti Sharma,
  • T. D. Rognlien

摘要

The 2-D edge plasma fluid transport code, UEDGE has been used to simulate the edge and scrape-off layer regions of circular limiter plasmas of ADITYA-U. The computational mesh defining the limiter geometry of ADITYA-U has been introduced in the UEDGE code through an in-house developed routine. It has successfully been integrated with the UEDGE code and the measured radial profile of electron density ( \(n_e\) ) in the edge region is modelled using the simulations. The plasma discharge for the present study has plasma current \(\text {I}_{P}\) \(\sim\) 130 kA, duration \(\sim\) 150 ms, chord-averaged electron density \(\sim\) 1.3 \(\times\) \(10^{19}\) \(\text {m}^{-3}\) , and central electron temperature \(\sim\) 270 eV has been observed. The maximum toroidal magnetic field is \(\sim\) 1.2 T. It has been found that an inward convective velocity, \(\text {v}_{conv}\) \(\sim\) 1.5 m/s is required in addition to the constant perpendicular diffusion coefficient, \(\text {D}_{\perp }\) \(\sim\) 0.2 \(\text {m}^2\) /s to adequately match the measured \(\text {n}_e\) profile in typical discharges of ADITYA-U. The value of \(\text {D}_{\perp }\) \(\sim\) 0.2 \(\text {m}^2\) /s is found to lie between the estimated neoclassical diffusivity and Bohm diffusivity.