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On the use of reduced grids in conjunction with the Equator-Pole grid system Cover

On the use of reduced grids in conjunction with the Equator-Pole grid system

By:   
Open Access
|Jan 2020

Figures & Tables

Fig. 1.

A small part 0λ45o and θ0 of a reduced grid for n = 160 and K = 3.

Table 1.

Reduced lat-lon grids with n = 360 and K segments on a hemisphere, using method I. Let NK be the total number of discretisation points for given K, pK is the decrease in per cent of N1, that is NK=(1pK/100)N1, and the quantity si is the number of parallels in the segment Sid. The area of the polar regions as per cent of the total area of the sphere is given by qK=100(1sinθK).

Kθ1θ2θ3θK1θKs1s2s3sK1sKσKpKqK145.0561.1892029237.450.843171.12699.523334.046.855.13814111.098814.218431.543.652.057.53513981.084816.216529.140.348.855.360.032129771.071817.913627.538.846.457.861.630128661.064119.412
Table 2.

Let N be the total number of discretisation points and si the number of parallels in the segment Sid. The areas of the polar regions as per cent of the total area of the sphere is given by q10=100(1sinθ10).

Grid system optimised according to method Iθ1θ2θ3θ4θ10s1s2s3s4s10σq10N23.933.340.145.665.9251987158281.04568.74.504·106Grid system with square net rectangles at θ=±π/4 in S4dθ¯1θ¯2θ¯3θ¯4θ¯10s¯1s¯2s¯3s¯4s¯10σ¯q¯10N¯25.034.942.047.768.22641037560271.05087.24.535·106
Table 3.

Normalised errors for solid rotation of the Cosine bell, n = 360, Δt=600 s, T = 12 days, α=π/3, and minimisation over c.

Minimum ofK108·c2psl2(H,12)r¯m(12)r¯e(12)l2(H,12)166.3632.6832e-031.6530e-069.1873e-06r¯m(12)1717635.1712e-033.6007e-076.9466e-05r¯e(12)13.9633.1638e-033.3152e-065.4354e-07l2(H,12)357.6632.8474e-038.6327e-088.8857e-06r¯m(12)3111632.9961e-032.4432e-081.6017e-05r¯e(12)32.08633.4038e-034.4039e-065.3897e-07l2(H,12)1146427.9403e-031.0634e-052.5847e-04r¯m(12)139.5428.3855e-037.6221e-067.3130e-05r¯e(12)10421.2667e-022.2503e-058.9115e-06l2(H,12)3130428.4252e-031.4219e-072.6351e-04r¯m(12)3164428.4670e-034.6614e-083.3125e-04r¯e(12)30.475429.6882e-031.2742e-054.4044e-06
Table 4.

Normalised errors for time dependent flow(Läuter), ¯2(Ψ*,15) minimised over c, n = 360, T = 15 days, α=π/4.

ΔtK108·c2pl2(Ψ*,5)l2(Ψ*,10)l2(Ψ*,15)30010.64762.0990e-94.1368e-96.2114e-930024.5562.1000e-94.1388e-96.2162e-930038.3462.1009e-94.1406e-96.2194e-9300419.462.1017e-94.1425e-96.2246e-9200119.464.1770e-108.2351e-101.2441e-9200233.464.2473e-108.3782e-101.3045e-9200341.564.3385e-108.5626e-101.3103e-9200453.264.4641e-108.8151e-101.3570e-9300129.844.2311e-88.5435e-82.5160e-7300349.849.2164e-81.8420e-74.6289e-7200157.447.7793e-81.5523e-73.9484e-7200398.641.7989e-73.5752e-77.8727e-7
Table 5.

Normalised errors for time dependent flow(Läuter), r¯e(15) minimised over c, n = 360, 2p=6,Δt=300 s, T = 15 days, α=π/4.

K108·c2(Ψ*,5)2(Ψ*,10)2(Ψ*,15)r¯m(15)r¯e(15)10.6862.0990e-94.1368e-96.2114e-94.9431e-121.8120e-1122.582.1000e-94.1388e-96.2175e-91.4348e-122.3018e-1131.132.1008e-94.1418e-91.8382e-89.2212e-122.0840e-1144.312.1011e-94.1610e-99.1909e-83.3190e-112.6892e-11
Fig. 2.

Contour curves for the total height H of the fluid for the mountain problem, no. 5 from Williamson et al. (1992): n = 360, K = 3, 2p = 6, c=105, T = 15 days. Method I.

Table 6.

Zonal flow over an isolated mountain, θc=30o, n = 360, K = 3, Δt=300, T = 15 days, 6 or 4 before r¯m(15) or r¯e(15) denotes the approximation order.

Method106·c6, r¯m(15)6, r¯e(15)106·c4, r¯m(15)4, r¯e(15)I101.0986e-062.3144e-0331.0277e-062.3085e-03I121.0977e-062.3143e-0359.9984e-072.3039e-03I151.0985e-062.3142e-03101.0358e-062.2925e-03II, q = 60.43.4746e-072.3150e-0315.5676e-072.3132e-03II, q = 60.53.4208e-072.3150e-0334.8095e-072.3086e-03II, q = 613.5403e-072.3150e-0354.8333e-072.3039e-03
Table 7.

The mountain problem, θc=30o, n = 360, K = 3, Δt=300, T = 5 years.

Method2p106·crm(T)re(T)I6121.49·1051.12·102II, q = 660.50.87·1051.04·102
Language: English
Page range: 1792736 - 1792736
Published on: Jan 1, 2020
Published by: Stockholm University Press
In partnership with: Paradigm Publishing Services

© 2020 Göran Starius, published by Stockholm University Press
This work is licensed under the Creative Commons Attribution 4.0 License.