Lunar properties from transient and steady magnetic field measurements.

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The electrical conductivity of the lunar interior has been determined from magnetic field step transients measured on the lunar dark side. The simplest model which best fits the data is a spherically symmetric three layer model having a nonconducting outer crust of radial thickness ≈ 0.03R moon; an intermediate layer of thicknessΔR≈0.37R moon, with electrical conductivityσ 1 ≈ 3.5 × 10-4 mhos/m; and an inner core of radiusR 2 ≈ 0.6R m with conductivityσ 2 ≈ 10-2 mhos/m. Temperatures calculated from these conductivities in the three regions for an example of an olivine Moon are as follows: crust, < 440 K; intermediate layer, ≈ 890 K; and core, ≈ 1240 K. The whole-moon relative permeability has been calculated from the measurements to beμ/μ 0 = 1.03 ± 0.13. Remanent magnetic fields at the landing sites are 38 ± 3γ at Apollo 12, 43 ± 6 and 103 ± 5γ at two Apollo 14 sites separated by 1.1 km, and 6 ± 4γ at the Apollo 15 site. Measurements show that the 38γ remanent field at the Apollo 12 site is compressed to 54γ by a solar wind pressure increase of 7 × 10-8 dynes/cm2.

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