1970
DOI: 10.1007/bf01230432
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A semi-analytic theory for the motion of a lunar satellite

Abstract: A semi-analytical solution to the problem of the motion of a satellite of the moon is presented. The theory is developed to third order, where first order is 10-2. Perturbative effects which are considered include those due to the attraction of the moon, earth, and sun, the non-sphericity of the moon's gravitational field, the oblateness of the earth, coupling of lower-order terms, solar radiation pressure, and physical libration. Short-period terms and those with the period of the moon's longitude are produce… Show more

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Cited by 31 publications
(14 citation statements)
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“…However, λ 22 contains the time explicitly (Giacaglia et al 1970). Using spherical trigonometry we have sin(φ) = sin(i) sin( f + g).…”
Section: Oblateness Of the Moonmentioning
confidence: 98%
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“…However, λ 22 contains the time explicitly (Giacaglia et al 1970). Using spherical trigonometry we have sin(φ) = sin(i) sin( f + g).…”
Section: Oblateness Of the Moonmentioning
confidence: 98%
“…, we call this term n M H as used by Giacaglia et al (1970). The Hamiltonian is still time-dependent through λ ⊗ .…”
Section: ∂(H )mentioning
confidence: 98%
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“…Because the phenomenon of order reduction often arises in long-period perturbation terms of lunar satellite, so early solutions wcrc always given in semi-analytical form [1][2][3]. However some modifications were made in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…In the main problem, the following approximations are made by Giacaglia et al (1970): i) the Moon's orbit around the Earth lies on the lunar equatorial plane; ii) the orbit of the Moon around the Earth is circular; iii) the longitude of lunar longest meridian λ 22 is equal to the longitude of the Earth λ ⊕ . The classical Keplerian orbital elements are used to define the orbit of a lunar orbiter; i.e.…”
Section: Hamiltonian Formulationmentioning
confidence: 99%