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Fig. K.1.

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Tidal torque between the Earth and the Moon corresponding to the coupled oceanic-solid response in two configurations: a global oceanic shell of thickness H = 4000 m (shown in red), and a hemispherical ocean with the same thickness, symmetric around the equator and bounded by longitudes λ = 0 and λ = π (in blue). Energy dissipation is quantified by the linear Rayleigh drag frequency σR. The logarithm of the torque is plotted as a function of the normalized frequency ω = (Ω − norb)/Ω0, where the Earth’s spin rate varies with the tidal forcing frequency Ω = norb + σ/2 at fixed norb, and Ω0 being the present spin rate of the Earth.

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