Fig. 7
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Modelled temperatureTF and apparent emissivity εF versus topographic models: (a) T(ε) (b) ε(Em). In the simulations A = 0.63, p = 0.5, R = 2 mm and the ice phase is amorphous. The thermal conductivity is constant, either kE0 = 0 (Γ = 0 when not specified in the legend) or kE0 = 0.001 W m−1 K−1 (Γ ~ 15 MKS). TF and εF are calculated for five footprints (#1 to #5) regularly distributed along the emission angle Em. The observed (Tobs, εobs) in the 350 footprints of observation CIRS_222DI_DIONE001_PIE are plotted (+). The topographic models are: flat for the flat case assuming average hemispherical emissivity εh (Eq. (13)), flat+ed for the flat case assuming directional emissivity ϵd (Eq. (14)), n=222 for the ellipsoidal n-ell model, q=64, 128 or 512 for the q-topo model at various spatial resolutions of the GTM. The effect of the spatial sensitivity (SS) of FP1 is shown for the GTM with q = 64 and kE0 = 0 (q=64+SS) or for kE0 = 0.001 W m−1 K−1 and p = 0.5 (q=64+SS, Γ = 15).
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