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Fig. 1.

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Vertical profiles of the equilibrium properties of a waveguiding magnetic flux tube based on the stratified density and magnetic field intensity models described by Eqs. (15) and (16). (a) Stratified Alfvén speed (CA(z)) inside the flux tube (Eq. (19)) with maximum at around 1.5 solar radii. (b) Stratified tube speed inside the flux tube ( C T ( z ) C A 2 C s 2 C A 2 + C s 2 ) $ \left(C_{_{T}}(z)\equiv\frac{C_{A}^2 C_{s}^2}{C_{A}^2 + C_{s}^2}\right) $. (c) Profile of the normalized equilibrium cross-section of the flux tube (Eq. (17)) relative to the tube cross-section at the base of the corona ( A 0 ( z ) A 0 ( 0 ) ) $ \left(\frac{A_0(z)}{A_0(0)}\right) $, as a function of height which is normalized by the radius of the sun. The Alfvén speed near the corona’s base is 1000 km/s.

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