Many-Body Dynamics: Conserved Hamiltonian?

  • Thread starter Thread starter Gear300
  • Start date Start date
  • Tags Tags
    Systems
AI Thread Summary
In systems with more than two interacting particles, individual conserved Hamiltonians cannot be defined due to the non-symmetrical net forces acting on each particle. While a reduced mass approach in a two-body problem allows for the formulation of Hamiltonians for the center of mass and relative distance, these do not correspond to individual particles. The discussion highlights that using a non-inertial frame complicates conservation laws, as forces become non-symmetric and conservation principles less straightforward. Although it's possible to derive conservation statements in non-inertial frames, they lack the elegance found in inertial frames. Overall, the complexities of particle interactions and frame selection significantly affect the conservation laws applicable to the system.
Gear300
Messages
1,209
Reaction score
9
For a system of more than 2 particles each interacting with each other under a potential (conservative force), does the dynamics of anyone particle exhibit a conserved (energy) quantity --- in other words, is it possible to write down a conserved Hamiltonian for each particle? The reason I ask is that the net force on anyone particle is not necessarily symmetrical.
 
Last edited:
Physics news on Phys.org
You cannot write down individual conserved Hamiltonians for interacting particles even if there are only two particles, so I must not be understanding your question.
 
No, you seem to have understood it.

Though, doesn't it depend on the frame of reference? For instance, in the 2-body problem, if you were to take the frame of reference such that one particle lies at the origin and use a reduced mass description, couldn't you come up with a conserved Hamiltonian?
 
You can't take an inertial frame of reference where one particle lies at the origin. Since the other particle will exert a force on it, a frame of reference tacked onto one particle will be non-inertial, and then questions like "what is a conservation law" get really confusing. If you use a reduced mass description in a two body problem, you have one Hamiltonian for the center of mass, and one Hamiltonian for the relative distance between the particles. These are both conservative, but neither of of them belongs to one particle or the other.
 
kanato said:
You can't take an inertial frame of reference where one particle lies at the origin. Since the other particle will exert a force on it, a frame of reference tacked onto one particle will be non-inertial, and then questions like "what is a conservation law" get really confusing. If you use a reduced mass description in a two body problem, you have one Hamiltonian for the center of mass, and one Hamiltonian for the relative distance between the particles. These are both conservative, but neither of of them belongs to one particle or the other.

If the acceleration of one particle was taken relative to another and it was found that the effective or apparent force in this frame behaved such that a scalar potential existed, then could you not still be able to make a statement on a conservation law despite being in a non-inertial frame?
 
You would, but it would not be as pretty as in an inertial frame. For example, in an inertial frame you have a symmetric momentum conservation law. However, in an accelerating frame you would have a nonsymmetric momentum conservation law. Especially when the acceleration of the frame is time-dependent, things will likely become very messy.
 
Thread 'Question about pressure of a liquid'
I am looking at pressure in liquids and I am testing my idea. The vertical tube is 100m, the contraption is filled with water. The vertical tube is very thin(maybe 1mm^2 cross section). The area of the base is ~100m^2. Will he top half be launched in the air if suddenly it cracked?- assuming its light enough. I want to test my idea that if I had a thin long ruber tube that I lifted up, then the pressure at "red lines" will be high and that the $force = pressure * area$ would be massive...
I feel it should be solvable we just need to find a perfect pattern, and there will be a general pattern since the forces acting are based on a single function, so..... you can't actually say it is unsolvable right? Cause imaging 3 bodies actually existed somwhere in this universe then nature isn't gonna wait till we predict it! And yea I have checked in many places that tiny changes cause large changes so it becomes chaos........ but still I just can't accept that it is impossible to solve...

Similar threads

Replies
8
Views
2K
Replies
1
Views
2K
Replies
1
Views
1K
Replies
10
Views
1K
Replies
84
Views
6K
Replies
4
Views
1K
Back
Top