Abstract

The dissipation of energy in the mantle of the Earth is held to be the main cause of the damping of the free nutation. The mantle is treated as a “Maxwell body.” Under these assumptions the period and the time constant of the damping are calculated in analogy to a former calculation of Jeffreys, who restricted himself to the case of an ideal elastic body. Comparison with the observed period and damping gives Love parameter z ≈ 0.3 and relaxation time τ ≈ 10 8 sec. It turns out, however, that a layer with τ values of 10 5 sec below a large zone with τ ≈ 10 8 sec would give about the same dissipation: therefore one can't find such a layer from the damping data. Nevertheless, a sufficiently large zone in the mantle with τ ⪆ 10 8 sec seems to be necessary in order to excite free nutation. On the other hand, zones of many hundred kilometers in size with relaxation times of τ ≈ 10 6 sec may hardly exist in the mantle, otherwise the damping should be more effective.

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