Fig. 3

First- and second-kind solutions of the symmetric tube as functions of the expansion parameter ϵ2. In a) a large range of ϵ2 values is considered. The dotted lines correspond to the asymptotic values of the frequency for ϵ2 → ∞, Ω+, given by Eq. (31). The dot-dashed lines correspond to the asymptotic values of the frequencies for ϵ2 → −∞, Ω−. In b) only the range of realistic ϵ2 values is considered. The half-length of the tube is set to L = 100 Mm, the thread half-length is l = 5 Mm, the radius of curvature is R = 60 Mm, the coronal sound speed csc = 200 km s-1, and the temperature contrast χ = 100.
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