Why is physical time-asymmetry vs dynamical law time-symmetry a problem?

In summary, John Baez says that the time reversal asymmetry of the world is not in conflict with the time reversal symmetry of dynamical laws, but at the end of the review he states that the main remaining mystery is why the state of the universe is grossly asymmetric under time reversal, even though the dynamical laws of physics are almost - but not quite! - symmetric. It would be nice if there was some sort of fundamental physical dynamic that made these 'possible' events, which are so improbable that they'll never happen, actually impossible.
  • #1
ThomasT
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I had always thought of this as sort of a pseudo-problem. After all, I would think, why shouldn't the dynamical laws be symmetric wrt time-reversal.

As John Baez stated in a review of H. D. Zeh's The Physical Basis of the Direction of Time (which I haven't read) http://math.ucr.edu/home/baez/time/time.html:

"Our world is evidently in a state that is not even approximately invariant under time reversal; there are many processes going on whose time-reversed versions never seem to happen. But this is logically independent from the question of whether the dynamical laws of physics admit time reversal symmetry."

Which seemed to reinforce my notion that the time reversal asymmetry of the world isn't necessarily in conflict with the time reversal symmetry of dynamical laws.

But at the end of the review he states:

"The main remaining mystery, then, is why the state of the universe is grossly asymmetric under time reversal, even though the dynamical laws of physics are almost - but not quite! - symmetric."

Did I miss something in Baez' review. If the time reversal asymmetry of the world and the time reversal symmetry of the dynamical laws are logically independent, then what exactly is the problem?

Is it that physics doesn't offer an underlying general dynamic for the apparently pervasive time reversal asymmetry of the physical universe? Or is it more complicated than that?

Thanks in advance for any comments.
 
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  • #3
Even ignoring the fact that there are time asymmetric laws of physics the point is that the laws of physics do not alone determine the evolution of a system. You also must also specify the boundary conditions. Even time symmetric laws will demonstrate asymmetric evolution from an extremely asymmetric boundary condition (like the Big Bang).

Also, I think it is fundamentally wrong to ignore the asymmetric laws as is so often done in such discussions, i.e. Baez' description as "one small exception". It is asymmetric and it is a law of physics, the classification as "big" or "small" is purely aestetic.
 
  • #4
DaleSpam said:
Even ignoring the fact that there are time asymmetric laws of physics the point is that the laws of physics do not alone determine the evolution of a system. You also must also specify the boundary conditions. Even time symmetric laws will demonstrate asymmetric evolution from an extremely asymmetric boundary condition (like the Big Bang).

Also, I think it is fundamentally wrong to ignore the asymmetric laws as is so often done in such discussions, i.e. Baez' description as "one small exception". It is asymmetric and it is a law of physics, the classification as "big" or "small" is purely aestetic.
Thanks DaleSpam.

Another aspect of this pseudo-problem that I've seen is the question of why we don't see advanced waves.

Also, I'm not comfortable with statements (vis statistical thermodynamics) that it's just very very unlikely, but not impossible, for (say) broken cups to reassemble themselves, or fried eggs to unfry themselves, etc.

It would be nice if there was some sort of fundamental physical dynamic that made these 'possible' events, which are so improbable that they'll never happen, actually impossible.

Do you forsee the formulation of any such fundamental physical law? Do you think that that is even possible?
 
  • #5
ThomasT said:
Another aspect of this pseudo-problem that I've seen is the question of why we don't see advanced waves.
I have always wondered about that. If we jiggle a charge we get a retarded wave moving outward in the characteristic dipole fashion. If we have a dipole wave moving inward towards a charge won't it jiggle and isn't that what an advanced wave is? I am pretty sure this means that the asymmetry of advanced and retarded waves is also just due to boundary conditions.
 
  • #6
DaleSpam said:
I have always wondered about that. If we jiggle a charge we get a retarded wave moving outward in the characteristic dipole fashion. If we have a dipole wave moving inward towards a charge won't it jiggle and isn't that what an advanced wave is? I am pretty sure this means that the asymmetry of advanced and retarded waves is also just due to boundary conditions.
I was thinking of an advanced wave as a wavefront that contracts toward its source rather than expanding away from it -- like a circular disturbance suddenly appearing on the surface of a smooth pool of water and then contracting to a rock that suddenly appears and then rises from the water.

We never see that. And it's not explained by the boundary conditions. It's not explained by the 2nd law of thermodynamics either, because it's not a dynamical law.

Is there a fundamental dynamic regarding the evolution of our universe that makes it impossible for advanced waves to happen?
 
  • #7
ThomasT said:
We never see that. And it's not explained by the boundary conditions.
What makes you think it's not explained by the boundary conditions? I think it is.
 
  • #8
I was thinking a little more about this topic today. The second law of thermo is clearly time asymmetric, so we don't expect time symmetry in any process where it is involved. However, the 2nd law of thermo is often attributed purely to the boundary conditions (as I have done) and essentially relegated to a statistical rule-of-thumb on the micro-state of a system. However, is it possible that, due to the statistical nature of quantum particles the microstate itself is statistical and cannot be defined to arbitrary precision even in principle? That could potentially refute the usual "if you reverse the initial velocity of every particle you would get the broken cup repairing itself" and establish the 2nd law of thermo as more than just a rule-of-thumb.

I cannot assert the validity of this argument as I lack the QM background. Take it for what it is, very rough and unsubstantiated preliminary musings.
 
  • #9
DaleSpam said:
What makes you think it's not explained by the boundary conditions? I think it is.
You asked if I was sure about boundary conditions not being an explanation. Well ... no, I'm not. :smile: (I've been spending as much time as possible researching stuff I should already have learned.)

I was thinking of boundary conditions as being more or less arbitrary constraints.

Anyway, I'm not sure about anything (being somewhat semantically challenged when it comes to physics) -- that's why I ask questions here, and appreciate it when I get replies. :smile:

DaleSpam said:
I was thinking a little more about this topic today. The second law of thermo is clearly time asymmetric, so we don't expect time symmetry in any process where it is involved. However, the 2nd law of thermo is often attributed purely to the boundary conditions (as I have done) and essentially relegated to a statistical rule-of-thumb on the micro-state of a system.
Yes, the 2nd LoT says that systems will evolve from states of lower to higher entropy, or, using phase space modelling, from states of lower to higher probability, toward equilibrium (the most probable state). But this is just kinematics. There's no underlying dynamic, or deeper kinematics, that can be said to necessitate that behavior, afaik. So, it's possible, however remotely, that a highly improbable evolution, such as an expanding surface wave spontaneously contracting, can happen.

Nevertheless, the normal practice is to act as if certain evolutions really are impossible, not just highly improbable, because all observations suggest that that's the most reasonable belief.

So, why not assume that the arrow of time, wrt any behavioral scale, is an unalterable and necessary fact of nature? Then the question is, what's the underlying dynamic that makes it so? Can the cosmological arrow of time be used?

Which is deeper, the large scale or the quantum scale behavior of the universe?

DaleSpam said:
However, is it possible that, due to the statistical nature of quantum particles the microstate itself is statistical and cannot be defined to arbitrary precision even in principle?
In principle wrt what? In principle wrt the principles of any theory constrained by the randomness of individual experimental results (and therefor necessarily statistical).

DaleSpam said:
That could potentially refute the usual "if you reverse the initial velocity of every particle you would get the broken cup repairing itself" and establish the 2nd law of thermo as more than just a rule-of-thumb.
It would, except that the terms random and statistical don't apply to microstates but rather to the accumulation of the data that's used to support (or falsify)inferences regarding them.

DaleSpam said:
I cannot assert the validity of this argument as I lack the QM background. Take it for what it is, very rough and unsubstantiated preliminary musings.
I thought that's what I was doing. :smile: Welcome to the party!

Any further thoughts (or corrections to anything that I myself have mused) you might have on this or related topics -- please post them.
 

1. Why is it important to study time-asymmetry and time-symmetry in physics?

Understanding the nature of time and its asymmetry and symmetry is crucial in developing a complete and accurate understanding of the physical world. Time is a fundamental concept in physics and plays a critical role in many physical laws and theories. Investigating time-asymmetry and time-symmetry helps us to better understand the fundamental laws of nature and the underlying principles that govern the behavior of the universe.

2. What is the difference between physical time-asymmetry and dynamical law time-symmetry?

Physical time-asymmetry refers to the fact that the arrow of time in our universe appears to only move in one direction, from past to future. This is in contrast to dynamical law time-symmetry, which refers to the idea that the fundamental laws of physics are symmetric with respect to time. In other words, the laws of physics remain the same regardless of whether time is moving forward or backward.

3. Why is the arrow of time important in understanding time-asymmetry?

The arrow of time is important because it provides a direction for events to occur in the universe. It allows us to differentiate between the past and the future, and is closely related to the concept of causality. The arrow of time is also crucial in understanding the second law of thermodynamics, which states that the entropy of a closed system will always increase with time.

4. What are some examples of physical processes that exhibit time-asymmetry?

One of the most well-known examples of time-asymmetry is the process of aging. We observe that living organisms age and deteriorate over time, but we do not see the reverse process of rejuvenation occurring. Another example is the expansion of the universe, which is a result of the Big Bang and is constantly moving forward in time.

5. How does the concept of time-symmetry challenge our understanding of the universe?

The concept of time-symmetry challenges our understanding of the universe because it suggests that the laws of physics are the same regardless of the direction of time. This raises questions about the origin of the arrow of time and why we only observe time moving in one direction. It also challenges our understanding of causality and the idea that cause and effect must occur in a specific order in time.

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