2011
DOI: 10.2478/v10018-011-0013-3
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Construction of the New High-Precision Moon Rotation Series at a Long Time Intervals

Abstract: Construction of the New High-Precision Moon Rotation Series at a Long Time Intervals The main purposes of this research are the construction of the new high-precision Moon Rotation Series (MRS2011), dynamically adequate to the DE404/LE404 and the DE406/LE406 ephemeris, over long time intervals. The comparison of the new highprecision Moon Rotation solutions of MRS2011 with the solution of MRS2010 (Pashkevich and Eroshkin, 2010), which is dynamically adequate to the DE200/LE200 ephemeris over 418.9 year… Show more

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Cited by 3 publications
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“…As a result from (8) and (9), following expressions are obtained: (10) Expressions for the perturbing terms of the physical librations of the Moon for the fixed ecliptic of epoch J2000 are defined by the following (Pashkevich and Eroshkin, 2011): (11) where W , U and V are the perturbing terms of the physical librations of the Moon in the longitude, in the inclination and in the node longitude, respectively; \ is the longitude of the descending node of epoch J2000 of the lunar equator; I is a constant angle of the inclination of the lunar equator to the fixed ecliptic J2000 ( I ~ 1 o 32'); T is the inclination of the lunar equator to the fixed ecliptic J2000; M is the proper rotation angle of the Moon between the descending node of epoch J2000 and the principal axis of the minimum moment of inertia; L e is the mean longitude of the Moon and : is the mean longitude of the ascending node of its orbit.…”
Section: Methods Of the Problem Solutionmentioning
confidence: 99%
“…As a result from (8) and (9), following expressions are obtained: (10) Expressions for the perturbing terms of the physical librations of the Moon for the fixed ecliptic of epoch J2000 are defined by the following (Pashkevich and Eroshkin, 2011): (11) where W , U and V are the perturbing terms of the physical librations of the Moon in the longitude, in the inclination and in the node longitude, respectively; \ is the longitude of the descending node of epoch J2000 of the lunar equator; I is a constant angle of the inclination of the lunar equator to the fixed ecliptic J2000 ( I ~ 1 o 32'); T is the inclination of the lunar equator to the fixed ecliptic J2000; M is the proper rotation angle of the Moon between the descending node of epoch J2000 and the principal axis of the minimum moment of inertia; L e is the mean longitude of the Moon and : is the mean longitude of the ascending node of its orbit.…”
Section: Methods Of the Problem Solutionmentioning
confidence: 99%
“…The discrepancies of the comparison between the numerical solutions and semi-analytical series MRS2011B for Newtonian (dynamical) case in the previous investigation (Pashkevich and Eroshkin 2011) are depicted in Figure 1. The discrepancies of the comparison between the numerical solutions and semi-analytical series MRS2014 for Newtonian (dynamical) case in the previous investigation (Pashkevich 2015) are depicted in Figure 3.…”
Section: A the Investigation Of The Rigid Moon Rotation Over 2000 Yementioning
confidence: 99%
“…The problem formularized in the Rodrigues -Hamilton parameters (Pashkevich and Eroshkin 2011), which in this paper are expressed via the perturbing terms of the physical librations of the Moon: cos sin sin sin , 2 2 2 2 sin cos cos cos . 2 2 2 …”
Section: Mathematical Modelmentioning
confidence: 99%