1995
DOI: 10.1029/95ja02691
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Dissipative MHD solutions for resonant Alfvén waves in two‐dimensional poloidal magnetoplasmas

Abstract: The resonant excitation of Alfv6n waves is considered in a resistive warm plasma embedded in a purely poloidal field. The magnetostatic equilibrium is invariant in the y direction. The driven problem is studied in the asymptotic state, so we can assume that all wave fields vary as exp[i(Ay-cot)]. Resistive solutions are derived in the vicinity of the resonance with the aid of an asymptotic expansion procedure. We find that the zeroth-order functions of the flux coordinate have to satisfy differential equations… Show more

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Cited by 13 publications
(10 citation statements)
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“…Here the Alfvén continuum is not affected by gravity, but the slow continuum is affected and it might be better referred to as the slow-gravity continuum. The singular solutions of the continuum Alfvén waves for 2D magnetostatic equilibrium models with a purely poloidal magnetic field were discussed in detail by Thompson & Wright (1993), Wright & Thompson (1994) and Tirry & Goossens (1995).…”
Section: The Continuous Spectrummentioning
confidence: 99%
“…Here the Alfvén continuum is not affected by gravity, but the slow continuum is affected and it might be better referred to as the slow-gravity continuum. The singular solutions of the continuum Alfvén waves for 2D magnetostatic equilibrium models with a purely poloidal magnetic field were discussed in detail by Thompson & Wright (1993), Wright & Thompson (1994) and Tirry & Goossens (1995).…”
Section: The Continuous Spectrummentioning
confidence: 99%
“…In onedimensional equilibrium models, the energy flux into the resonance is proportional to the magnetic pressure perturbation squared (Andries et al, 2000;Andries & Goossens, 2001), a result that was used by Arregui et al (2007b) to analyse the influence of the internal structuring of coronal loops on the damping by comparing the efficiency of the process at internal and external layers. In two-dimensional equilibrium states, the energy flux absorbed at a particular field line is proportional to the overlap integral between P T (r A , z), the profile of P T along the tube at the resonant position, and the resonant Alfvén eigenfunctions (Thompson & Wright, 1993;Tirry & Goossens, 1995). This is why the longitudinal profiles of b z and v ϕ , and their modification due to changes in the longitudinal density distribution are so relevant in determining kink mode damping times.…”
Section: Energy Analysismentioning
confidence: 99%
“…Even under these most favorable of circumstances, the resultant PDEs are generally not solvable in terms of ODEs through the method of separation of variables. The critical layer phenomenon may also persist in these more general circumstances, but it generally requires line-tying of the magnetic Ðeld at a rigid boundary (e.g., Poedts & Goossens 1987, 1988Tirry & Goossens 1995).…”
Section: Exemplary Model Calculationsmentioning
confidence: 99%