Abstract <p>The paper presents a numerical analysis of the possibility of performing local measurements of potential and plasma density fluctuations in the T-15MD tokamak using the Heavy Ion Beam Probe (HIBP) diagnostic. Four types of fluctuations are considered in the frequency range up to 500 kHz: Geodesic Acoustic Mode (GAM), Quasi-Coherent Mode (QCM), Tearing Mode (TM), and Alfvén eigenmode (AE). For each type of fluctuation, spatial measurement areas are defined for regimes with different values of average density <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({{\bar {n}}_{e}}\)</EquationSource> <!--PlasPhys2560392Vinitskiy-m1--> </InlineEquation> and toroidal magnetic field <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\({{B}_{T}}\)</EquationSource> <!--PlasPhys2560392Vinitskiy-m2--> </InlineEquation>. Regimes with flat and peaked density profiles are considered. It is shown that high-Q fluctuations (GAM, AE, TM) can be measured in the peripheral region of the plasma <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\rho &lt; 0.8\)</EquationSource> <!--PlasPhys2560392Vinitskiy-m3--> </InlineEquation> up to density <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({{\bar {n}}_{e}} \leqslant 7 \times {{10}^{{19}}}\;{{{\text{m}}}^{{ - 3}}}\)</EquationSource> <!--PlasPhys2560392Vinitskiy-m4--> </InlineEquation>, while low-Q QCMs can be measured up to <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({{\bar {n}}_{e}} \leqslant 5 \times {{10}^{{19}}}\;{{{\text{m}}}^{{ - 3}}}\)</EquationSource> <!--PlasPhys2560392Vinitskiy-m5--> </InlineEquation>. In the plasma gradient region <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\rho = 0.5{-} 0.9\)</EquationSource> <!--PlasPhys2560392Vinitskiy-m6--> </InlineEquation> the measurement of high-Q fluctuations is possible at a density of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({{\bar {n}}_{e}} \leqslant 5 \times {{10}^{{19}}}\;{{{\text{m}}}^{{ - 3}}}\)</EquationSource> <!--PlasPhys2560392Vinitskiy-m7--> </InlineEquation>, and of the low-Q QCM at a density of <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({{\bar {n}}_{e}} \leqslant 3 \times {{10}^{{19}}}\;{{{\text{m}}}^{{ - 3}}}\)</EquationSource> <!--PlasPhys2560392Vinitskiy-m8--> </InlineEquation>.</p>

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Spatial Areas of Potential and Density Fluctuation Measurements Using HIBP on the T-15MD Tokamak

  • E. A. Vinitskiy,
  • L. G. Eliseev,
  • D. A. Shelukhin,
  • Y. M. Ammosov,
  • A. V. Melnikov

摘要

Abstract

The paper presents a numerical analysis of the possibility of performing local measurements of potential and plasma density fluctuations in the T-15MD tokamak using the Heavy Ion Beam Probe (HIBP) diagnostic. Four types of fluctuations are considered in the frequency range up to 500 kHz: Geodesic Acoustic Mode (GAM), Quasi-Coherent Mode (QCM), Tearing Mode (TM), and Alfvén eigenmode (AE). For each type of fluctuation, spatial measurement areas are defined for regimes with different values of average density \({{\bar {n}}_{e}}\) and toroidal magnetic field \({{B}_{T}}\) . Regimes with flat and peaked density profiles are considered. It is shown that high-Q fluctuations (GAM, AE, TM) can be measured in the peripheral region of the plasma \(\rho < 0.8\) up to density \({{\bar {n}}_{e}} \leqslant 7 \times {{10}^{{19}}}\;{{{\text{m}}}^{{ - 3}}}\) , while low-Q QCMs can be measured up to \({{\bar {n}}_{e}} \leqslant 5 \times {{10}^{{19}}}\;{{{\text{m}}}^{{ - 3}}}\) . In the plasma gradient region \(\rho = 0.5{-} 0.9\) the measurement of high-Q fluctuations is possible at a density of \({{\bar {n}}_{e}} \leqslant 5 \times {{10}^{{19}}}\;{{{\text{m}}}^{{ - 3}}}\) , and of the low-Q QCM at a density of \({{\bar {n}}_{e}} \leqslant 3 \times {{10}^{{19}}}\;{{{\text{m}}}^{{ - 3}}}\) .