On the Numerical Integration of Two Body Problem with Variable Mass

Author(s):  
C. Calvo ◽  
M. Palacios
2014 ◽  
Vol 2014 ◽  
pp. 1-11
Author(s):  
José Antonio López Ortí ◽  
Francisco José Marco Castillo ◽  
María José Martínez Usó

This paper aimed to address the study of a new family of anomalies, called natural anomalies, defined as a one-parameter convex linear combination of the true and secondary anomalies, measured from the primary and the secondary focus of the ellipse, and its use in the study of analytical and numerical solutions of perturbed two-body problem. We take two approaches: first, the study of the analytical development of the basic quantities of the two-body problem to be used in the analytical theories of the planetary motion and second, the study of the minimization of the errors in the numerical integration by an appropriate choice of parameters in our family for each value of the eccentricity. The use of an appropriate value of the parameter can improve the length of the developments in the analytical theories and reduce the errors in the case of the numerical integration.


Icarus ◽  
1963 ◽  
Vol 2 ◽  
pp. 440-451 ◽  
Author(s):  
John D. Hadjidemetriou

1983 ◽  
Vol 74 ◽  
pp. 369-375
Author(s):  
T.B. Omarov ◽  
M.J. Minglibaev

SummaryThe new nonstationary model problem is considered. Its solution generalizes by form the known particular Mestschersky-Vinti solution in a two-body problem of variable mass. The equations of the corresponding perturbed motion are deduced. In the case of a two-body problem of variable mass μ. the perturbing force is proportional to second temporal derivative from the value μ-1 . It is possible to describe with a good approximation such qualitative effects in this problem as a trapping and disintegration on a basis of properties of the model problem. Let us consider the example of a trapping.


1979 ◽  
Vol 81 ◽  
pp. 49-52
Author(s):  
T. B. Omarov

Some non-stationary problems of celestial mechanics can be described in an inertial system of right-angled coordinates with gravitational potential of the form: where is a sufficiently arbitrary function of time and is the meaning of in the initial epoch For example, in a two-body problem of variable mass we have:


1974 ◽  
Vol 10 (2) ◽  
pp. 141-149 ◽  
Author(s):  
Pierre Guillaume

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