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Hamiltonian, synodic

Let us consider a rotating or synodic reference frame centered at the barycenter of P and P2 assume that the units of measure are such that the relative angular velocity of P and P2 is unity. Then, the coordinates of Pi and P2 are, respectively, Pi( 2>0) and P2(—Mi,0). Let (qi,q2) be the coordinates of S in the synodic frame (see Figure 4). In order to derive the synodic Hamiltonian, we consider the generating function... [Pg.211]

It is trivial to check that the synodic Hamiltonian takes the form... [Pg.212]

In a synodic reference frame, the Hamiltonian of the planar, circular, restricted three-body problem is given by... [Pg.218]

In the framework of the circular, restricted three-body problem, let us consider the motion in the 3-dimensional space of the three bodies S, Pi and P2. The primaries move in the c/ic/2 plane around their common center of mass, while in the synodic frame their coordinates become Pi(p2,0,0), P2(—Pu 0) 0)- Assume that the (/lfjg-plane rotates with unit angular velocity about the vertical axis. Then, the Hamiltonian function is given by... [Pg.221]


See other pages where Hamiltonian, synodic is mentioned: [Pg.212]   
See also in sourсe #XX -- [ Pg.212 ]




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