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        2007-12-18

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Summary

 

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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

 
SUMMARY

Here at the beginning of the 21st century, scientists and educators still teach and still believe that lighter and heavier bodies — per Galileo fall at precisely the same rate (see falling rate difference for separate trials), but the truth is far more fascinating. A trivial and still overlooked consequence of Newton’s laws is that, because of their asymmetric gravitational interactions, lighter and heavier bodies do not fall at precisely the same rate, with only one exception: lighter and heavier bodies will fall at precisely the same rate — Newton-theoretically — when the 3 masses (including e.g. the Earth) are at the vertices of an equilateral triangle, i.e. when one of the bodies occupies a Trojan point (or Lagrangian point L4 or L5) with respect to the other 2 bodies.

The situation is even simpler for the separate release of the 2 bodies. Since the heavier body causes e.g. the Earth to accelerate toward it more quickly, heavier bodies will always fall faster than lighter bodies in the reference frame of either the Earth or the other body. This is a potentially important consequence of Newton’s theory of gravity that was overlooked — or at least never analyzed and/or commented on — by Einstein, whose relativity postulates that lighter and heavier test particles will accelerate at the same rate. By Newton’s theory, they will only accelerate at the same rate if their acceleration is measured with respect to the absolute Newtonian space-time framework, and even then only at the instant of release (t=0) and not after (t>0). This is not the best fundamental necessity for “relativity”.

Here we will primarily explore the simultaneous release case since this is the most interesting historically and astronomically.

Newton should never have overlooked this mostly non-zero falling rate difference, that it implies the (probable) existence of Trojan points, and that it is essential to the gravitational dynamics of these Trojan points and their associated Trojan asteroids which move in “tadpole” and “horseshoe” orbits around them. If Sir Isaac — or even his lesser contemporaries — had only questioned the scientific dogma of their day, and sacrificed that Sacred Cow as they had Aristotle, he or they could easily have discovered (well, at least predicted) Trojan points over a century before Lagrange.

The millennia old “science wars” that are heating up yet again find a new and crucial twist on an old wrinkle: science failing, but this time on science’s own terms. As we submit more and more to science and its control over our daily lives, we must learn to remember that even “modern” science is not only fundamentally fallible, but that it can fail in its foundations — even in the simplest things — for hundreds of years without notice. It is also good to study the overt anger and summary dismissal by leading scientists when science is seriously questioned, on its own terms; this is a whole different level of the failure of science on its own terms, but one that needs to be “fresh-aired” completely, and remembered forever lest it be repeated.

RECENT HISTORY: The equation(s) showing the falling rate difference as a function of the mass difference (and angle of separation) and linking that to Lagrange’s Trojan points (Lagrangian points L4 and L5) was first published on the Internet in 1995 (by PAIAS). Since then, it has been expanded with commentary, history, analysis, philosophy and more commentary, and even a look at the future of Trojan body astronomy, including raising the question of whether stable ternary star systems are possible.

 

 

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