Three Classes of Newtonian Three-Body Planar Periodic Orbits (by Milovan Šuvakov [student], Veljko Dmitrašinović [senior nuclear physicist] of Belgrade)They use topological and numerical methods to find three classes with 13 new types of periodic orbits in the 3-body problem.

The two-body problem in Newton's gravity happens to be fully solvable. You may prove that the elliptical orbits with the right parameters and the center-of-mass in one of the foci exactly solves Newton's equations of motion. Kepler's laws – that were guessed before Newton found his theory – exactly describe some of the solutions.

The equation for the ellipse (in space) may be written down explicitly, in terms of elementary functions. However, in the precise parameterization we want, \(x(t),y(t),z(t)\), it's somewhat more subtle. Nevertheless, we count the two-body problems among the analytically solvable ones.

Note that two bodies have 6 components of positions and 6 components of momenta. However, there are 3 conserved components of momentum, 3 conserved components of the angular momentum, 3 conserved components of the Runge-Lenz vector, and one conserved energy. In total, there are 12 parameters determining the initial state and 10 constraints that restrict its evolution. This turns out to be enough although it looks I am missing one constraint for an argument I would be able to give. ;-) If you know how to complete it, let me know.

For the 3-body problem, there are still 10 integrals of motion but the dimension of the phase space jumps to 18 which is way too much. There's no way to write down the general solution. In general, the behavior of the system exhibits some chaotic behavior etc. Henri Poincaré proposed that in such a messy situation, one should focus on the periodic solutions as our fifth column that helps us to penetrate into the chaotic enemy's party.

Well, using his words,

“... what makes these (periodic) solutions so precious to us, is that they are, so to say, the only opening through which we can try to penetrate in a place which, up to now, was supposed to be inaccessible”.Interestingly enough, these periodic solutions only began to be mass-produced in recent 40 years. The two Serbs added quite a collection of drilled holes among these "openings". Here's a figure from their paper that does a good job in showing the complicated topology of some of the solutions:

*See also the 3-body gallery in Serbia. The spheres are "shape spheres" that encode the relative distances between the 3 bodies in a certain way.*

Because of the 3-body problem and the fact that its situation is generic, I never understood the amazement – e.g. by folks like Stephen Wolfram – that simple rules may lead to solutions we can't write down analytically. In fact, it's almost always the case that there's no way to write down an explicit solution to a problem such as a complicated enough differential equation or their set. The situation of the 3-body problem is a rule, not an exception.

On the contrary, I believe that what is precious for a physicist is to find some way to understand some problems despite the fact that their vast majority is not "integrable" – solutions can't be written in an easy form. When physicists do so, they usually depend on the subset they understand more than the bulk – either problems that are fully "integrable" or problems whose properties of a certain kind (e.g. the topological ones) can be determined exactly. All the other problems and solutions are phrased as variations or perturbations of the "more integrable" ones.

You will need to read the paper if you want to know any details. It's clearly written. I would be sort of surprised if these exotic shapes in the figure-eight [shape] family and other families were spotted by observational astronomers but that doesn't mean that there aren't arguments in favor of their existence. When you have 3 bodies, the proximity of their orbit to a periodic one (in time) is a good explanation why no pair among the 3 bodies has collided yet (after millions or billions of years). This "survival explanation" is actually the only one I am able to think about that would explain why the periodic orbits could be "attractors" in the real world. Well, we don't know too many real-world 3-body systems with comparable masses, anyway, so these questions might be a bit academic.

L.v=0 should do the job of the missing constraint.

ReplyDeleteI don't understand what you mean by "v". There are three bodies. Moreover, if you mean things like

ReplyDeleteL . A = 0

for the Runge-Lenz vector A, it is not a constraint, but a redundancy of the constraints, so it actually reduces the number of constraints. I am still confused by the counting.

v is the relative velocity (in the 2 body problem). the constraint "L . v = cte = 0" comes along with the "L x v + r = cte = A"

ReplyDeleteI see, got it, thanks a lot. I was thinking about the 3-body problem at the same moment which is silly.

ReplyDeleteSo now, there are 11 constraints for 12 variables which means that the allowed region in the phase space is 12-11=1-dimensional which exactly corresponds to the freedom to choose 1 parameter t, and create a 1-dimensional orbit.

Lubos, you should optimize the page so that when sharing it or a post on facebook, it shows more than just a link. it should preview images from the article or a general image when there are not.

ReplyDeletelubos

ReplyDeleteHow it connected with Efimov state ?

http://en.wikipedia.org/wiki/Efimov_state

Dear George, apologies for that. Now I spent 30 minutes by fixing it - see og:image in the HTML source. However, it still doesn't work well because Facebook now requires at least 180-pixel thumbnails for the links, otherwise it offers inappropriate ones or no thumbnails at all.

ReplyDeleteI've ever seen a page with code that scales it but it disappeared somewhere.

If the constraint 180 didn't exist, I promise you that Facebook would offer you a thumbnail seen at

http://motls.blogspot.cz/?m=1

as well as the overall TRF logo. Cheers, LM

it only shows the green mathjax button on the right for the posts and the lhcb post on the main page. other times it would not usually have a thumbnail for the main page. if you fix it, it will look nicer on facebook and more people will click on it. it will also get more impressions when an image is included.

ReplyDeleteApologies, it behaves differently when I post it on Facebook. So it's an irregular behavior of a sort and I have no clue how to fix it for you.

ReplyDeleteit shows the relevant image of the spheres only when i click on share the discussion, not when i click on share the page or when i post the link.

ReplyDeleteIsn't it just because the list of images is cached somewhere?

ReplyDeleteTry to erase the "posting the link" comment on FB and post a new URL where .com is replaced by .de or .cz or .ca or .sk or something else, for example, and you may get new images.

I won't do more research on this - this has already been a lot of time relatively to the importance of this issue. If you tell me how the HTML template could be improved, the final answer, I may return to it but otherwise I won't.

ReplyDeleteA "freeway" through the solar system resembling a vast array of virtualClarification: Interplanetary Superhighwaywinding tunnels and conduits around the Sun and planets, as envisioned by an engineer at NASA's Jet Propulsion Laboratory (JPL), Pasadena, Calif., can slash the amount of fuel needed for future space missions.

It's more then just astronomical observation that one may look out to the stars as some elliptical pattern. IN a sense it becomes a very detailed and intrinsic pattern established, as some kind of freeway uesd in our Earth Orbits. Ltool becomes a useful resource for identifying such locations.

Best,

ok it works when .com is replaced.

ReplyDeleteI count like this: a) 6 of the 12 two-body variables are the positions and momenta of the CM, with the initial positions arbitrary and the momenta constant via translation invariance (momentum conservation); b) in the 2-body problem, assuming a central force, rotation invariance (conserved angular momentum vector L) takes care of 2 more variables (motion is in a plane, so theta=pi/2 and theta.dot=0) and determines a constant of the motion (3 constraints) c) For a conservative force, the energy E provides another constant of the motion; and d) for the inverse-square force, the direction of the RL vector A sets the direction of the perihelion (in the plane, so 1 one variable, with the other two components of A being interdependent with L and E. That takes care of 6+3+1+1=11 variables, with one left for the initial angular position of the particle, which was the conclusion you knew was correct all along... I like your physics discussions...

ReplyDelete