“…For single sinusoidal wavelengths, D h = λ ( λ / a ) 2 /(8 π 3 ), where λ and a denote the wavelength and amplitude of ground undulations, respectively [ McClung , ]. The linear viscous fluid assumption is a crude one: for dense snow, rheometrical tests exhibit a nonlinear viscoelastic behavior (shear thinning, with a shear thinning index close to 1/3, as in Glen's law used for ice) [ Scapozza and Bartelt , ; Delmas , ]. However, several experiments have tried to estimate bulk shear viscosity: it has usually been found that snow viscosity varies by several orders of magnitude as a function of temperature, density, and liquid water content: η ranges from 10 6 Pa s to 10 12 Pa s [ Haefeli , ; Bucher , ; Salm , ; Haefeli , ; Salm , ; Shapiro et al , ; Teufelsbauer , ]; the typical values for snow at T = 0°C with ρ = 400 kg m −3 are η ∼ 5×10 10 Pa s and ν ∼ 0.2 [ Shinojima , ; Shapiro et al , ].…”