Time Reversal Symmetry: Particle Motion

In summary, the conversation discusses the concept of time reversal symmetry and its relation to physical laws and specific systems. It is determined that time reversal symmetry is a property of physical laws, rather than specific systems, and is determined by the equations of motion. The conversation also touches on other symmetries, such as rotation and charge, and their relation to conserved quantities. The concept of symmetry and its role in determining the laws of physics is also discussed.
  • #1
eoghan
207
7
Hi there!
You have a particle moving to the left as time goes on. Now if you reverse the time the particle will move to the right. Does it mean that the system is not symmetric under time reversal?
 
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  • #2
Isn't time reversal symmetry a property of physical laws and not specific systems? The laws are symmetric if you can film a process and play the video backward and the video still makes physical sense.
 
  • #3
A better suited name is motion reversal symmetry. So the change in the direction of the motion doesn't imply that it's not time-reversal symmetric.
 
  • #4
The_Duck said:
Isn't time reversal symmetry a property of physical laws and not specific systems? The laws are symmetric if you can film a process and play the video backward and the video still makes physical sense.

On the contrary, rotation, parity, charge etc are symmetries of the specific system and not physical laws, aren't they?
 
  • #5
eoghan said:
On the contrary, rotation, parity, charge etc are symmetries of the specific system and not physical laws, aren't they?

It is precisely as The_Duck said. If I show you a movie of something physical process that is symmetric under time reversal you will not be able to tell me wether the movie is going forward or backward.

One always determines time symmetry for the equations of motion (or the principle they are derived from) of a system. If those equations do not change under t-> -t, then you have time symmetry and a specific motion is then determined by initial conditions.

You are mixing some stuff here. Parity and rotations are symmetries of nature (well, parity only is to some extent). From continuous symmetries we can deduce conserved quantities which in the case of rotations is angular momentum.
Charge is the conserved quantity to a complex rotation in the Lagrangian.
Another symmetry is charge conjugation, which exchanges particles and anti particles.
 
  • #6
The_Duck said:
Isn't time reversal symmetry a property of physical laws and not specific systems? The laws are symmetric if you can film a process and play the video backward and the video still makes physical sense.
This is correct.

For the situation presented by the OP the relevant law is Newton's first law. The forward time particle is initially going to the right and continues going to the right at the same speed per Newton's first law. The reverse time particle is initially going to the left and continues going to the left at the same speed per Newton's first law. Newton's first law is therefore symmetric under time reversal.
 
  • #7
betel said:
You are mixing some stuff here. Parity and rotations are symmetries of nature (well, parity only is to some extent). From continuous symmetries we can deduce conserved quantities which in the case of rotations is angular momentum.

But can we deduce conserved quantities from symmetries of the physics laws or we can do it just from symmetries of nature?
 
  • #8
We can, as long as the laws we have correctly describe nature.
Whenever there is discrepancy you have to correct your theory (not blame it on nature)

That was the case with parity. For a long time everybody assumed and was sure that is an exact symmetry of nature. Until somebody really measured decays on found one favourite chirality.
So now parity is only an approximate symmetry of nature.
 
  • #9
Uhm.. I can't understand.. let' start from a simpler question:
Let's suppose I have a particle on the top of a gaussian-shaped hill (i.e. a hill symmetric under rotations along vertical axis). If I rotate the system along the vertical axis I can't say that the system has been rotated, because it looks the same. So I say that the system is symmetric.
But if the particle was not on the top of the hill, but on a side, then if I rotate the system I can see that the particle is changing its position, so the system is not symmetric anymore under rotations... is it true?
 
  • #10
That is the difference between a specific situation and the laws governing the future evolution of the state.

In general a specific state will not be symmetric.
But the laws (equations of motion) are. Evolution will look exactly the same whether time is running forward or backward. The only difference you will have to allow for is different initial condition.

But the point with particle on the side not being symmetric is a good point, although this will lead to some sophisticated physics. May I ask what your level of physics is. Have heard about the Higgsparticle.?
 
  • #11
eoghan said:
Uhm.. I can't understand.. let' start from a simpler question:
Let's suppose I have a particle on the top of a gaussian-shaped hill (i.e. a hill symmetric under rotations along vertical axis). If I rotate the system along the vertical axis I can't say that the system has been rotated, because it looks the same. So I say that the system is symmetric.
But if the particle was not on the top of the hill, but on a side, then if I rotate the system I can see that the particle is changing its position, so the system is not symmetric anymore under rotations... is it true?
You are correct, the second system is not axisymmetric any more. However, usually time-reversal symmetry is discussed wrt the laws and not specific systems, so I don't understand the purpose of your question here in the context of the OP.

Do you understand the difference between a differential equation and the initial conditions? The laws of physics are cast as differential equations, and a specific system is represented by the initial conditions.
 
  • #12
Ok, so a system is said to be time reversal invariant if the laws of physics doesn't depend on time (i.e. if the laws of physics that govern the system are symmetric under a time reversal, and not if the specific system is "geometrically" symmetric). Is it true also with the others symmetries? I mean, a system is said to be symmetric under rotations (and so the angular momentum is conserved) if the specific system is symmetric or if the laws governing the system are symmetric?

betel said:
But the point with particle on the side not being symmetric is a good point, although this will lead to some sophisticated physics. May I ask what your level of physics is. Have heard about the Higgsparticle.?
I'm attending the third year in physics and I studied QM last semester and now I'm studying an introduction to elementary particles physics. But I've never studied symmetries deeply and now I'm a bit confused!
I heard about Higgs particle... but I've never understood that much :frown:
 
  • #13
eoghan said:
Ok, so a system is said to be time reversal invariant ...
I just have never ever heard of a system being described as time reversal invariant. I have only ever heard that description applied to laws of physics.
 
  • #14
DaleSpam said:
I just have never ever heard of a system being described as time reversal invariant. I have only ever heard that description applied to laws of physics.

That is not quite true. You usually attribute the symmetries to the Langrangian describing a system. Some quantities and their corresponding conserved quantities can only be read off from the Lagrangian and not the equations of motion, e.g. charge.

The Higgs particle utilizes the property that the general system is invariant under a cvertain symmetry but a certain state is not.
In this case the electroweak symmetry. The Lagrangian is invariant under this symmetry but the ground state (vacuum state) with the least energy does not respect this symmetry, so it is lost in everyday life, unless at very high energies (more than can be realized on earth).
 
  • #15
betel said:
You usually attribute the symmetries to the Langrangian describing a system.
Not in my experience, at least not for time-reversal symmetry.
 
  • #16
I'm going to back up a few posts.

eoghan said:
Hi there!
You have a particle moving to the left as time goes on. Now if you reverse the time the particle will move to the right. Does it mean that the system is not symmetric under time reversal?

Yes, the system is not symmetric under time reversal. Velocity V is replaced with -V.

I would be curious (but doubtful) to see how applying a Lagrangian to a quantum system, rather than the Newtonian F=ma, could change this.
 
  • #17
I thought I had already answered, but maybe I forgot to push the button...

The confusion in here stems from the fact that there is difference whether one considers the symmetries of a general system or a specific state in a given system.
In other words it always depends on the background you re working in.

For simplicity consider motion in free space.
Then the motion of any number of particles is symmetric under time reversal, that means for any given configuration of initial conditions I can find another set of initial conditions that will look like the same evolution if time is running backwards.
Now if you want to consider the background of one particle already moving in one fixed way in empty space, and ask how other particles would evolve in this background, then there will be no time reversal symmetry any more as you one set particle explicitly breaks the symmetry.
 
  • #18
That is reasonable. When I was speaking of systems I was thinking of the second case you mention where you are considering a specific state in a given system. I was not even considering the "middle case" between laws and specific systems which you describe as a general system.
 

1. What is time reversal symmetry in particle motion?

Time reversal symmetry is a fundamental concept in physics that states that the laws of physics should be the same if time was reversed. In particle motion, this means that the behavior of particles should remain unchanged if time were to run backwards.

2. Why is time reversal symmetry important in particle physics?

Time reversal symmetry is important because it helps us understand the behavior and interactions of particles in the universe. It allows us to predict the outcomes of particle interactions and study the fundamental forces that govern the universe.

3. How do scientists test for time reversal symmetry in particle motion?

Scientists test for time reversal symmetry by observing the behavior of particles in controlled experiments. They look for any changes in the behavior of particles when time is reversed, and if no changes are observed, then time reversal symmetry is said to hold.

4. Are there any known violations of time reversal symmetry in particle motion?

Yes, there are known violations of time reversal symmetry in particle motion. These are observed in certain subatomic particle interactions, such as kaon decays, where the behavior of particles differs when time is reversed.

5. How does the concept of time reversal symmetry relate to the arrow of time?

The concept of time reversal symmetry is closely related to the arrow of time, which is the notion that time moves in a particular direction and cannot be reversed. The violation of time reversal symmetry in certain particle interactions suggests that the arrow of time is not always absolute, and that there are certain cases where time can move in both directions.

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