Keep the time on the moon: a relative approach to the moon hours
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Abstract and 1. Introduction
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The watch is in orbit
2.1 Time Format
2.2 The domestic frame for the moon
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Differences of the average clock between the earth and the moon
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Watch at Lagance points on Earth
4.1 The watch in Lagrang Point L1
4.2. The watch is in Lagrang Point L2
4.3. The watch is in Lagrange Point L4 or L5
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Conclusions
Approach 1: Fermi coordination with the original in the center of the moon
Approach 2: Building the center of the bloc frame freely
Things 3: Earth and moon movement equations
Approach 4: Comparing the results in rotating and non -periodic coordinates systems
Thanks, appreciation and references
Approach 1: Fermi coordination with the original in the center of the moon
We give the transformation equations between Parisian coordinates and natural coordinates, and he throws with the center in the moon as follows:[6]
Here, blogging (m) as in Fifth(M) It represents the quantities that were evaluated in the center of the block. The V (M) is the size of the moon’s speed. The transformation transactions can be derived:
The metropolitan tensioner is converted with the usual formula:
Where the plural agreement applies to repeated indicators. Thus, for the time time consisting of the metropolis in the freedom -falling frame.
Approach 2: Building the center of the bloc frame freely
The transformation transactions are easily obtained from the above -made transformations
The mirror tensioner is transformed with EQ. (72): The Mistress G00 component in the center of the mass,
Summary, numerical fixed in the middle of the mass system
Authors:
(1) Neil Ashbi, National Institute of Standards and Technology, Bulder, Co 80305 ([email protected]);
(2) Bijunath R. Patla, National Institute of Standards and Technology, Bulder, Co 80305 ([email protected]).