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Fig. 6. Experiment 2: numerical solution at several time moments (North pole view)
where
∂t = c 1 cos ϕ θ 2 γ cos ξ tan κ 2 ϕ cos γt cos 2 t − sin ξ sin 2 t ,
∂T
∂λ = c 1 ω cos ϕ cos 2 t cos ξ,
2 T
∂λ 2 = −c 1 ω 2 cos ϕ cos 2 t sin ξ,
∂T
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