<i>α</i> Effect and Magnetic Diffusivity <i>β</i> in Helical Plasma Under Turbulence Growth
We investigate the transport coefficients <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="htt...
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Format: | Article |
Language: | English |
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MDPI AG
2025-06-01
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Series: | Universe |
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Online Access: | https://www.mdpi.com/2218-1997/11/7/203 |
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Summary: | We investigate the transport coefficients <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> in plasma systems with varying Reynolds numbers while maintaining a unit magnetic Prandtl number (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mo form="prefix">Pr</mo><mi mathvariant="normal">M</mi></msub></semantics></math></inline-formula>). The <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> tensors parameterize the turbulent electromotive force (EMF) in terms of the large-scale magnetic field <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mover><mi mathvariant="bold">B</mi><mo>¯</mo></mover></semantics></math></inline-formula> and current density as follows: <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>⟨</mo><mi mathvariant="bold">u</mi><mo>×</mo><mi mathvariant="bold">b</mi><mo>⟩</mo></mrow><mo>=</mo><mi>α</mi><mover><mi mathvariant="bold">B</mi><mo>¯</mo></mover><mo>−</mo><mi>β</mi><mrow><mo>∇</mo><mo>×</mo><mover><mi mathvariant="bold">B</mi><mo>¯</mo></mover></mrow></mrow></semantics></math></inline-formula>. In astrophysical plasmas, high fluid Reynolds numbers (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>R</mi><mi>e</mi></mrow></semantics></math></inline-formula>) and magnetic Reynolds numbers (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>R</mi><msub><mi>e</mi><mi mathvariant="normal">M</mi></msub></mrow></semantics></math></inline-formula>) drive turbulence, where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>R</mi><mi>e</mi></mrow></semantics></math></inline-formula> governs flow dynamics and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>R</mi><msub><mi>e</mi><mi mathvariant="normal">M</mi></msub></mrow></semantics></math></inline-formula> controls magnetic field evolution. The coefficients <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>α</mi><mi>semi</mi></msub></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>β</mi><mi>semi</mi></msub></semantics></math></inline-formula> are obtained from large-scale magnetic field data as estimates of the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> tensors, while <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>β</mi><mi>theo</mi></msub></semantics></math></inline-formula> is derived from turbulent kinetic energy data. The reconstructed large-scale field <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mover><mi>B</mi><mo>¯</mo></mover></semantics></math></inline-formula> agrees with simulations, confirming consistency among <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula>, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mover><mi>B</mi><mo>¯</mo></mover></semantics></math></inline-formula> in weakly nonlinear regimes. This highlights the need to incorporate magnetic effects under strong nonlinearity. To clarify <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula>, we introduce a field structure model, identifying <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula> as the electrodynamic induction effect and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> as the fluid-like diffusion effect. The agreement between our method and direct simulations suggests that plasma turbulence and magnetic interactions can be analyzed using fundamental physical quantities. Moreover, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>α</mi><mi>semi</mi></msub></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>β</mi><mi>semi</mi></msub></semantics></math></inline-formula>, which successfully reproduce the numerically obtained magnetic field, provide a benchmark for future theoretical studies. |
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ISSN: | 2218-1997 |