Statement Expressing the Chinese People's Firm Support for by Mao Tse-Tung

By Mao Tse-Tung

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20. Notice 56 Fig. 19. Stromgren family g of direct and simple-periodic f the plane Hill problem. Source : The orbits of the figure have bility is lost when V< . - Fig. 20. Stromgren ι 2 - stability 0 but this sta­ y 1 ι 1 family of retrograde orbits of the plane Hill problem. of Ηέηοη, Μ. [104]. 692 «C orbits 1 1 19^Γ^ 79. 704 periodic Hdnon, M. [104]. These orbits are given by the Brown series ; they have both the "inplane" and the "out-of-plane" first order stability for any value of Π 57 The periodic "pseudo-circular" orbits of the plane three-body problem have been computed in the references 133 and 134 for the case of three equal masses.

17. A "pseudo-circular retrograde orbit" in the axes of the center of mass J of the small binary. Ref 68-137 with successive surveys 131, 132). For three given masses the families of periodic orbits are one-non-trivialparameter families that meet each other that can at the be constructed step by step by continuity "bifurcations" where exchanges of stability and take place. In Reference 104 are given many numerical and graphical informations about the simplest periodic orbits of the plane Hill problem (equations (139), (140) with ζ = 0) at orbit g and especially the three below Figs.

Fig. 20. Stromgren ι 2 - stability 0 but this sta­ y 1 ι 1 family of retrograde orbits of the plane Hill problem. of Ηέηοη, Μ. [104]. 692 «C orbits 1 1 19^Γ^ 79. 704 periodic Hdnon, M. [104]. These orbits are given by the Brown series ; they have both the "inplane" and the "out-of-plane" first order stability for any value of Π 57 The periodic "pseudo-circular" orbits of the plane three-body problem have been computed in the references 133 and 134 for the case of three equal masses. 1 and Ref.

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