Earth's orbital history revised



Ferenc Varadi 1 and Bruce Runnegar 1,2; astrobiology.ucla.edu


1Institute of Geophysics and Planetary Physics

2Department of Earth and Space Sciences

University of California, Los Angeles, CA 90095-1567


WE carried out several long-term simulations of planetary orbits in which the equations of motions were directly integrated using an accurate multi-step scheme. The physical models, with increasing complexity, include corrections to the Newtonian attraction of point masses: General Relativity, analytically averaged models of the lunar orbit and the J2 term of the solar gravity field. The model used by Quinn et al. (1991) turned out to be inadequate upon comparison with the case in which the Moon was resolved as a separate body (R5). We found by empirical means a much better model which is used in R7, R8 and R9.

MORE:

Comparisons

Chaotic transitions


Summary of simulations

Simulation
designation

General
Relativity

Modeling of
Moon

Solar
J2

Step size
(days)

Length
(Ma)

Still
running?

R1

no

barycenter

no

0.25

100

no

R2

yes

barycenter

no

0.3125

212

no

R3

yes

barycenter

no

0.25

89

no

R4

yes

AM

no

0.3125

123

no

R5

yes

resolved

no

0.03125

23

yes

R6

yes

AM+ICA

no

0.3125

6

no

R7

yes

MAM

no

0.3125

180

yes

R8

yes

MAM+MICA

no

0.3125

10

no

R9

yes

MAM

yes

0.3125

150

yes

AM: The avereged Earth-Moon model of Quinn et al. (1991)
MAM: Modifief average Earth-Moon model.
ICA: Initial conditions adjusted for consistency (Quinn et al., 1991)
MICA: Modified adjustment of initial conditions.



References
Laskar, J.: 1990, Icarus 88, 266.
Laskar, J.:1999, Phil. Trans. R. Soc. Lond. A357, 1735.
Quinn, T. Q., Tremaine, S. and Duncan, M.: 1991, Astron. J. 101, 2287.
Shackleton, N. J., Crowhurst, S. J., Weedon, G. P. and Laskar, J.: 1999, Phil. Trans. R. Soc. Lond. A357, 1907.
Zachos, J. C.; Flower, B. P. and Paul, H.: 1997, Nature 388, 567.


Background image: NASA/JPL/Malin Space Science Systems