Resonant Topographic Waves in Barotropic and Baroclinic Flows
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Cites methods from "Resonant Topographic Waves in Barot..."
...Bistable solutions to simple models of planetary flow over topography were obtained by Charney and DeVote [1979], Hart [1979], and Pedlosky [1981]. The relevance of bistability to low-frequency atmospheric variability was often interpreted to stand or fall by the discovery of such bimodality in NH winter data....
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Cites background from "Resonant Topographic Waves in Barot..."
...The lateral boundary conditions at the two rigid walls are (Pedlosky 1981)...
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...…] ]c9 21 u (¹ c9 2 Fc9) 1 (b 1 Fu )0 01 2]t ]x ]x 2 2 25 2J(c9, ¹ c 1 h) 2 J(c, ¹ c9) 1 ¹ c*. (2b)S The lateral boundary conditions at the two rigid walls are (Pedlosky 1981) 2]c ] c 5 0, 5 0 at y 5 0, L , (3)y]x ]t]y where 5 limX→` (1/2X) c dx is the zonally avXc #2X eraged part of the…...
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...Finally, the bottom topography is considered to be wavy and h 5 «h9(x, y) is assumed in the quasigeostrophic regime (Pedlosky 1981)....
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...The bottom topography may be chosen to be of the following form (Pedlosky 1981) h9 5 h9 exp(ikx) sin(my/2) 1 c.c.,0 (10) where is the constant amplitude of the wavy topog-h90 raphy, k 5 2k0 is the zonal wavenumber of the wavenumber two topography, and m 5 22p/Ly....
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...The bottom topography may be chosen to be of the following form (Pedlosky 1981)...
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