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Fig. 4 Lagrangian Points

 

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Summary
Intro and History
Newton’s Gravity
Trojan Points and Bodies
Tadpole-Horseshoe Orbits
... Oversights
21st Century Astronomy
APPENDIX
Fig. 1 Bodies and Vectors
Fig. 2 Falling Rate Diff.
Fig. 3 Centers of Mass
Fig. 4 Lagrangian Points
Fig. 5 Tadpoles-Horseshoes
Fig. 6a Ternaries?
Fig. 6b Ternaries?
Author

Newton’s... Oversight
Einstein’s... Oversights
Entropy’s... Oversights
Comet Origins
Cosmology... Oversights
Creationism... Oversights

Newton’s Great... Oversight
Galileo’s Falling Bodies and Lagrange’s Trojan Asteroids
With Their Tadpole and Horseshoe Orbits

 

8          FIGURES (cont.)

Figure 4. The Lagrangian Points L1-L5.

WARNING NOTE: if you have spent much time searching the Internet for info on Lagrangian points, you have probably been confused by the lack of consistency in the numbering of the points. About the only consistency that you will find there is that there is agreement that L1-L3 are the collinear points, and L4-L5 are the equilateral triangle points. Sigh... If it helps, the numbering used here is the same as that found in e.g. the Encyclopedia of the Solar System (hyperlink unfortunately no longer seems valid), pp. 815-7; Weissman, McFadden, Johnson, Eds.; Academic Press, 1999. For an example of alternate numbering (with a pedigree), see http://www.astro.queensu.ca/~wiegert/etrojans/etrojans.html (which unfortunately no longer seems valid).

Lagrange’s theory assumes that L1-L5 are occupied only by “infinitesimal” bodies (purely a calculational convenience, since no masses are truly “infinitesimal”). Here the diagram assumes that m << M.

NOTE: technically, the Lagrangian points L4 and L5 do not even exist unless Lagrange’s restriction is met, i.e. that m < ~0.04 M.

The relative positions of L1 and L2 (and even L3, but far less so) with respect to the two non-infinitesimal masses depend on the mass ratio, m/M, but L4 and L5 always form equilateral triangles with m and M.

NOTE: it is implicit in the above diagram that the mass m is much smaller than mass M, i.e. the center of mass of both masses together is very close to the center of mass of M by itself. This is the case with the Sun and Jupiter. However, the more general case needs to be studied, and can be with the aid of computers.

 

 

 

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