Abstract
A Wentzel-Kramer-Brillouin (WKB) approach, based on the method of
Connor, Hastie, and Taylor (1979), is used to obtain simple estimates of
the critical conditions for the onset of ideal magnetohydrodynamic (MHD)
instabilities in line-tied solar coronal loops. The method is
illustrated for the constant twist, Gold-Hoyle (1960) field, and the
critical conditions are compared with previous and new numerical
results. For the force-free case, the WKB estimate for the critical loop
length reduces to (2 * pi * m) + (pi * square root of 2). For the
sufficiently non-force-free case the critical length can be expressed in
the form (l0 + l1)/m. The results confirm the
findings of De Bruyne and Hood (1992) that for force-free fields the m =
1 mode is the first mode to become unstable but for the sufficiently
strong non-force-free case this reverses with the m approaches infinity
mode being excited first.
Original language | English |
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Pages (from-to) | 99-115 |
Journal | Solar Physics |
Volume | 150 |
DOIs | |
Publication status | Published - 1 Mar 1994 |
Keywords
- Applications Of Mathematics
- Coronal Loops
- Force-Free Magnetic Fields
- Magnetohydrodynamic Stability
- Mathematical Models
- Photosphere
- Plasma Equilibrium
- Solar Magnetic Field
- Solar Prominences
- Wentzel-Kramer-Brillouin Method
- Boundary Conditions
- Differential Equations
- Eigenvalues
- Eigenvectors
- Fourier Analysis
- Fourier Series
- Lagrangian Function
- Magnetic Field Configurations
- Plasma Physics