Time-reverse symmetry of the principle of relativity

[Chrisc]

Please look at the attached diagram and let me know
if there is a reason for the asymmetric dynamics due
to the relative position of rest or, if I have incorrectly
interpreted the mechanics.
Kev, I haven't forgotten.

 

[Chrisc]

Not a single response tells me either it is too confusing in the
graphic form I posted, or I've pointed out something no one can
rationalize with relativity.
In case it's the former, I've included below a less detailed
text version of the question.

The time-reverse symmetry of the dynamics in a simple two body collision seems
to hold only when the observer is initially at rest with the lessor of the two massive bodies.

If this is as straight forward as I think it is, it has significant implications for
the principle of relativity.
Have I misinterpreted the mechanics, or is this stumping everyone?

 

[Vanadium 50]

Not a single response tells me either it is too confusing in the
graphic form I posted, or I've pointed out something no one can
rationalize with relativity.

I think it's more likely that people don't want to spend the time hunting down your mistake. Relativistic mechanics is time symmetric.

 

[DrGreg]

Please look at the attached diagram and let me know
if there is a reason for the asymmetric dynamics due
to the relative position of rest or, if I have incorrectly
interpreted the mechanics.

I can't work out what you think the problem is. As far as I can see, everything in your diagrams is time-symmetric and you haven't explained why you think there is asymmetry.

However, your diagrams are correct only in Newtonian mechanics, not in relativistic mechanics.

In relativity, momentum is

p = \frac {mv} {\sqrt{1 - v^2/c^2}}​

and velocities are transformed from one frame to another using

w = \frac {u - v} {1 - uv/c^2}​

Rest mass m is not conserved in collisions but energy

E = \frac {mc^2} {\sqrt{1 - v^2/c^2}}​

is conserved in elastic collisions.

 

[Chrisc]

I can't work out what you think the problem is. As far as I can see, everything in your diagrams is time-symmetric and you haven't explained why you think there is asymmetry.

When the observer is initially at rest with B1(#5), the time-reverse symmetry of the kinematics shown in #8 violate the laws of dynamics.
B2 will not bring B1 to rest. The kinematics all appear time-reverse symmetric as kinematics are the quantitative expressions of the mechanics with T set to negative.
When the observer is initially at rest with B1, the correct time-reverse dynamics of #5 would present the same as #2.
The time-reverse symmetry of this event is only upheld when the observer is initially at rest with B2,
a situation that implies there is a problem with the symmetry of relativistic mechanics through time-reversal.

 

[MeJennifer]

B2 will not bring B1 to rest.

What do you mean by bringing something to rest. Rest is a relational not an absolute concept in relativity. Something is only at rest in relation to something else.

 

[Chrisc]

What do you mean by bringing something to rest. Rest is a relational not an absolute concept in relativity. Something is only at rest in relation to something else.

I mean with respect to the observer.
When the observer is initially at rest with respect to one of the two bodies (B1 and B2)
they observe differing but valid mechanics after the collision.
The problem arises when the same event is considered through time-reversal.
In the first case where the observer is initially at rest with respect to B2, the
time-reverse mechanics are valid.
When the observer is initially at rest with respect to B1, the time-reverse
mechanics (when held to the symmetry of the forward-time kinematics)
require dynamics that violate or contradict the laws (Newton's).

 

[MeJennifer]

IWhen the observer is initially at rest with respect to B1, the time-reverse mechanics (when held to the symmetry of the forward-time kinematics)
require dynamics that violate or contradict the laws (Newton's).

Not true.

 

[Dale]

f = dp/dt is obviously time symmetric. If you have some scenario which is not time symmetric then it cannot follow the laws of mechanics.

 

[Chrisc]

Not true.

Not helpful.

 

[Chrisc]

f = dp/dt is obviously time symmetric.

A body B1 with mass M and velocity v wrt to the observer collides with a body B2 with mass 1/2M at rest with respect to the observer.
The mass B1 comes to rest wrt the observer and the body B2 moves away with velocity 2v wrt the observer.
This is the (invalid) time-reverse description of the (valid) time forward event. It does not happen in nature as it conserves momentum via increased kinetic energy.
So it appears as a statement of kinematics, f = dp/dt is time-reverse symmetric, but it is not necessarily always time-reverse symmetric as a statement of dynamics.

If you have some scenario which is not time symmetric then it cannot follow the laws of mechanics.

I am not pointing out a scenario that is not time-reverse symmetric and upholds the laws, I am pointing out a scenario that appears time-reverse symmetric in its kinematics but as such its dynamics must violate the laws.
If you take that to mean that it is just not time reverse symmetric in the first place, then you are recognizing what I am saying as it is the same event that is time-reverse symmetric when the observer is at rest wrt B2.

 

[George Jones]

A body B1 with mass M and velocity v wrt to the observer collides with a body B2 with mass 1/2M at rest with respect to the observer.
The mass B1 comes to rest wrt the observer and the body B2 moves away with velocity 2v wrt the observer.

This is the (invalid) time-reverse description of the (valid) time forward event. It does not happen in nature as it conserves momentum via increased kinetic energy.

Chrisc, it seems to that you're asking

"Why is there a thermodynamic arrow of time?"

 

[JesseM]

A body B1 with mass M and velocity v wrt to the observer collides with a body B2 with mass 1/2M at rest with respect to the observer.
The mass B1 comes to rest wrt the observer and the body B2 moves away with velocity 2v wrt the observer.

This would be true in Newtonian mechanics but it doesn't work in SR.
Total momentum before collision: \frac{M*v}{\sqrt{1 - v^2/c^2}}
Total momentum after: \frac{(M/2)*(2v)}{\sqrt{1 - (2v)^2/c^2}}
These are not equal, so this can't be correct (momentum should be conserved in collisions in SR just like it is in Newtonian mechanics).

 

[George Jones]

This would be true in Newtonian mechanics but it doesn't work in SR.

I don't think that this affects Chrisc's argument. Chrisc's argument is that inelastic collsions occur only one way in time.

Roughly, heat (internal energy) is more disordered then translational kinetic energy of an entire object, hence, by thermodynamics, inelastic collisions only happen one way in time.

 

[JesseM]

I don't think that this affects Chrisc's argument. Chrisc's argument is that inelastic collsions occur only one way in time.

Ah, he didn't specifically refer to the collision as inelastic, but now I see that he mentions the kinetic energy changes (in Newtonian terms as well as relativistic ones). And yes, inelastic collisions involve a change in entropy (kinetic energy of the center of mass being transformed into heat, which is random kinetic energy of many molecules in different directions) which is why they are extremely unlikely to happen in reverse, although in terms of the fundamental non-thermodynamic laws of physics there is nothing physically impossible about the reversed scenario.

 

[Dale]

A body B1 with mass M and velocity v wrt to the observer collides with a body B2 with mass 1/2M at rest with respect to the observer.
The mass B1 comes to rest wrt the observer and the body B2 moves away with velocity 2v wrt the observer.
This is the (invalid) time-reverse description of the (valid) time forward event. It does not happen in nature as it conserves momentum via increased kinetic energy.
So it appears as a statement of kinematics, f = dp/dt is time-reverse symmetric, but it is not necessarily always time-reverse symmetric as a statement of dynamics.

I'm sorry, but what you are saying here doesn't make any sense. Newton's laws are the laws of dynamics. Newton's laws are time symmetric. Therefore dynamics are time symmetric. Kinematics are just dynamics w/o the forces, so if the dynamics are time symmetric then the kinematics are also time symmetric. This is obvious and clear from the laws themselves, you don't need to worry about specific cases because the laws are symmetric in general.

In your example, the explanation is simple, in the forward case momentum is conserved through a decrease in KE (KE->thermal energy), in the reverse case momentum is conserved through an increase in KE (thermal energy->KE). The fact that the reverse case doesn't happen in nature is due to the non-time symmetry of thermodynamics, not any asymmetry in dynamics.

A minor point is that your analysis is non-relativistic.

 

[yuiop]

Please look at the attached diagram and let me know
if there is a reason for the asymmetric dynamics due
to the relative position of rest or, if I have incorrectly
interpreted the mechanics...

Your diagrams are obviously non relativistic. There seems to be an error in the calculations in your diagrams when the calculations are done using the Newtonian equations.

The equation for a head on elastic collision is given here: http://hyperphysics.phy-astr.gsu.edu/Hbase/elacol2.html#c1

Using the notation given in that link, you have initial conditions:

Ball B1: m_1=2m, v_1=2v
Ball B2: m_2=1m, v_2=0v

The final velocity of mass m1 is:

v_1' = v1 \frac{m1-m2}{m1+m2} = 2v\frac{2m-1m}{2m+1m} =2/3v

The final velocity of mass m2 is:

v_2' = v1 \frac{2m_1}{m_1+m_2} = v\frac{4m}{2m+1m} =8/3v

The initial total momentum of the system is (m_1 v_1 )+(m_2 v_2) = 4mv

The final total momentum of the system is (m_1 v_1')+(m_2 v_2') = 4/3mv+8/3mv = 12/3mv = 4mv

Total momentum before and after the collision is conserved.

The total initial kinetic energy of the system is:

1/2m_1 (v_1)^2 + 1/2m_2 (v_2)^2 = 4mv^2

The total final kinetic energy of the system is:

1/2m_1 (v_1')^2 + 1/2m_2 (v_2')^2 = m(2/3v)^2 + 1/2m(8/3)^2 = 4mv^2

Total KE before and after the collision is conserved.


The final conditions in your diagram of:

Ball B1: m_1=2m, v_1'=v

Ball B2: m_2=1m, v_2'=2v

do not satisfy the conservation of momentum AND conservation of KE laws.

Another condition that is normally satisfied in a head on elastic collision, is that the velocity of approach equals the velocity of separation. In the example I gave the velocity of approach is 2v and the velocity of separation is also 2v (8/3v - 2/3v). The velocity of approach in your diagram is 2v while the velocity of separation is 1v.

I am pretty sure that when you do the forward calculations correctly, they will time reverse correctly.

 

[George Jones]

Your diagrams are obviously non relativistic. There seems to be an error in the calculations in your diagrams when the calculations are done using the Newtonian equations.

The equation for a head on elastic collision is given here: http://hyperphysics.phy-astr.gsu.edu/Hbase/elacol2.html#c1

Have you read posts #12 through #16? The equations in the link don't apply, since they are for elastic collisions. Chrisc analyzes inelastic collisions that are physically realistic, and that cannot be excluded from consideration.

Consider a more extreme example.

Two equal mass objects collide and stick together. Before the collision, the objects move with equal speeds in opposite directions with respect to a particular frame. By conservation of momentum, the combined object does not move after the collision.

This is a completely plausible physical scenario, i.e., think putty.

The time reverse of the collision is not plausible at all. A blob of putty does not separate into two smaller blobs spontaneously, with each of the two smaller blobs moving in different directions.

This is in accord with the laws of thermodynamics and statistical mechanics.

I am pretty sure that when you do the forward calculations correctly, they will time reverse correctly.

I think Chrisc has done the forward calculations correctly for plausible inelastic collisions. Even though Chrisc didn't make an error by choosing to analyze inelastic collisions, as they happen all the time in the real world, I think Chrisc would agree that elastic collisions are time reversible.

 

[yuiop]

Have you read posts #12 through #16? The equations in the link don't apply, since they are for elastic collisions. Chrisc analyzes inelastic collisions that are physically realistic, and that cannot be excluded from consideration.

In the diagram he attached to post#1 he shows the case for the elastic collision in frames 1 to 4 and the inelastic case in frames 5 to 8. I took the time to check his calculations in frames 1 to 4 (the elastic case) and when I found them to be in error and I did not really pursue the thread further. Ignoring the fact that there is an error in his elastic case I can see now that he is making the case that elastic collisions appear to be reversible while inelastic collisions do not appear to be reversible.

Consider a more extreme example.

Two equal mass objects collide and stick together. Before the collision, the objects move with equal speeds in opposite directions with respect to a particular frame. By conservation of momentum, the combined object does not move after the collision.

This is a completely plausible physical scenario, i.e., think putty.

The time reverse of the collision is not plausible at all. A blob of putty does not separate into two smaller blobs spontaneously, with each of the two smaller blobs moving in different directions.

This is in accord with the laws of thermodynamics and statistical mechanics.I think Chrisc has done the forward calculations correctly for plausible inelastic collisions. Even though Chrisc didn't make an error by choosing to analyze inelastic collisions, as they happen all the time in the real world, I think Chrisc would agree that elastic collision are time reversible.

Looking at the equation for an inelastic collision http://hyperphysics.phy-astr.gsu.edu/Hbase/inecol.html#c1 the final velocity of the combined mass of B1 and B2 should be 4/3v and not the 1v shown in frames 4 to 8. Despite the fact Chrisc has made an error in both the elastic and inelastic cases it should not distract us from the case he is making that inelastic collisons appear to be non-reversible. As I understand it, classical dynamics does not forbid a blob of putty separating into two smaller blobs spontaneously, with each of the two smaller blobs moving in different directions when analysed at the molecular scale. All it says is that it is statistically unlikely. A freek set of unlikely collisons at the molecular level producing that sort of reverse reaction is unlikely but not imposssible. It is basically an example of the arrow of time and increasing entropy. Another example is a glass falling off a table and breaking into a million pieces. The reverse situation of the glass reassembling itself and ending back up on top of the table is not impossible, just statistically extremely unlikely in classical dynamics.

Basically it comes down to the fact that converting coherant motion (the parallel motion of the molecules that make up the ball) to incoherant random motion (heat) is more likey than the reverse in nature, (but not impossible). An example of the reverse in nature would be the thermal heat of magma beneath the surface of the Earth being converted into coherant motion of the water and steam being ejected from a geyser.

 

[George Jones]

In the diagram he attached to post#1 he shows the case for the elastic collision in frames 1 to 4 and the inelastic case in frames 5 to 8. I took the time to check his calculations in frames 1 to 4 (the elastic case) and when I found them to be in error and I did not really pursue the thread further. Ignoring the fact that there is an error in his elastic case I can see now that he is making the case that elastic collisions appear to be reversible while inelastic collisions do not appear to be reversible.

Looking at the equation for an inelastic collision http://hyperphysics.phy-astr.gsu.edu/Hbase/inecol.html#c1 the final velocity of the combined mass of B1 and B2 should be 4/3v and not the 1v shown in frames 4 to 8. Despite the fact Chrisc has made an error in both the elastic and inelastic cases it should not distract us from the case he is making that inelastic collisons appear to be non-reversible.

I admit that I only checked Chrisc's calculation in post #11; I didn't have the stamina to examine the whole thread in detail. Post #11 was enough to show me Chrisc's point. In the real world, inelastic collisions are not reversible. I checked to see if anyone made the connection with thermodynamics.

As I understand it, classical dynamics does not forbid a blob of putty separating into two smaller blobs spontaneously, with each of the two smaller blobs moving in different directions when analysed at the molecular scale. All it says is that it is statistically unlikely. A freek set of unlikely collisons at the molecular level producing that sort of reverse reaction is unlikely but not imposssible. It is basically an example of the arrow of time and increasing entropy. Another example is a glass falling off a table and breaking into a million pieces. The reverse situation of the glass reassembling itself and ending back up on top of the table is nto ot impossible, just statistically extremely unlikely in classical dynamics.

This just isn't going to happen in the real world. The difference in phase space volumes is more than enormous.

 

[yuiop]

Hi George and JesseM,

I admit that I only checked Chrisc's calculation in post #11; I didn't have the stamina to examine the whole thread in detail. Post #11 was enough to show me Chrisc's point. In the real world, inelastic collisions are not reversible. I checked to see if anyone made the connection with thermodynamics...

This just isn't going to happen in the real world. The difference in phase space volumes is more than enormous.

OK, I will restate it as, the reverse process is more than enormously statistically improbable.

 

[George Jones]

So, Chrisc, why are inelastic collisions not time reversible? Because of the second law of thermodynamics.

Why is there a second law of thermodynamics? I don't know if there is agreement on this, but some physicists, including Roger Penrose and Sean Carroll, think that the second law has a cosmological origin. In the blog entry

http://cosmicvariance.com/2007/06/11/latest-declamations-about-the-arrow-of-time/

Sean Carroll concludes

But if you want to describe why the Second Law actually works in the real world in which we actually live, cosmology inevitably comes into play.

 

[George Jones]

I have split this thead. The rest appears as the new thread Entropy and Cosmology

https://www.physicsforums.com/showthread.php?t=244736

in the Cosmology forum.

Any comments about the entropy and the second law of thermodynamics with respect to cosmology should be placed in the new thread.

 

[Dale]

In your example, the explanation is simple, in the forward case momentum is conserved through a decrease in KE (KE->thermal energy), in the reverse case momentum is conserved through an increase in KE (thermal energy->KE). The fact that the reverse case doesn't happen in nature is due to the non-time symmetry of thermodynamics, not any asymmetry in dynamics.

I just realized that the reverse case can in fact happen in nature. All that is necessary is that in the forward case the energy is stored, e.g. in a locking spring, instead of dissipated into thermal energy. Then in the forward case momentum is conserved through a decrease in KE (KE->elastic energy), in the reverse case momentum is conserved through an increase in KE (elastic energy->KE).

 

[Chrisc]

I had hoped to get back to this sooner but I'm in the middle of a "money pit" renovation that is
taking all my free time, so I can't address every post right now, but George Jones has made it easier
for me to address the point I'm trying to make.
These are inelastic collisions designed to show the principle of time-reversal is not only or always
a simple matter of mathematical symmetry that conserves momentum (total energy of the system).
There is a difference between the time-reverse symmetry of the laws and the time-reverse symmetry of mechanics.
The laws must, in principle, uphold under time-reversal or they would be expressions of or indications of
faulty axiomatic foundations.
Mechanics on the other hand are not so easily reversed. The kinematics of an event are the measurable dimensions
of the system, which are easily reversed as they are simply "quantitative" expression of dimension.
To reverse the direction of time you simply flip the sign to negative and everything runs (equates) backwards.
The dynamics are the problem, as they define the forces (classically) that give rise to the kinematics.
This means a translation of momentum between differing masses must consider the "empirical" evidence
of the second law of thermodynamics. Just because Newton's laws are "quantitatively" symmetric through
time-reversal, (i.e.: equal and opposite) does not mean we will ever see a fly stop a freight train.

The problem as I see it is the "qualitative" expression of the laws under time-reversal.
My point, or question is not why is there a second law of thermodynamics, it is that the second law
conditions the mechanics according to our frame of reference.
The mechanics of time-reversal measured by an observer are different according to their frame of reference.
This is a trivial observation in most cases, but in the example I've given it makes the difference between
the law of conservation of momentum displaying increased entropy or decreased entropy.
In other words, from one of only two frames, both involved in the event, the second law is upheld
in one and contradicted in the other.
This seems to indicate a "preferred" frame with respect to the laws of mechanics.
More importantly it says something fundamentally significant about the principle of relativity
and time. The (ideal) instantaneous exchange of momentum in the collision of two differing
masses, presents a "qualitative" change in dimension depending on the frame of the observer.

 

[Chrisc]

I just posted when I noticed you split this thread.
I understand that it was moving to a discussion of thermodynamics but to my OP it is
a question of relativity that becomes apparent in thermodynamics. So I would hope
to keep this thread here and steer back to my point which is more "relative" to
this forum.

 

[George Jones]

I just posted when I noticed you split this thread.
I understand that it was moving to a discussion of thermodynamics but to my OP it is
a question of relativity that becomes apparent in thermodynamics. So I would hope
to keep this thread here and steer back to my point which is more "relative" to
this forum.

Any aspects of thermodynamics and relativity that pertain to your scenarios can be posted here. I didn't mean to give the impression that this thread is dead.

Any general posts about the cosmological origin of the second law of thermodynamics should go in the new thread.

 

[JesseM]

There is a difference between the time-reverse symmetry of the laws and the time-reverse symmetry of mechanics.
The laws must, in principle, uphold under time-reversal or they would be expressions of or indications of
faulty axiomatic foundations.

Why do you say that? It is perfectly possible to imagine mathematical laws that are not invariant under time-reversal, which physically just means that if you saw a movie of a physical system played backwards, you would see it was not obeying the same fundamental equations as in the forward version. In fact, in our own universe the laws of physics are not purely T-symmetric but actually exhibit a symmetry called CPT-symmetry; physically this means that if you play a movie of a system backwards, you also have to reverse the labels of positive and negative charges (so matter becomes antimatter and vice versa), and also flip the system to its mirror image on each of the 3 spatial axes (reversing 'parity'), in order for the backwards movie to appear to be obeying precisely the same fundamental laws as the forwards movie in all possible circumstances.

This means a translation of momentum between differing masses must consider the "empirical" evidence
of the second law of thermodynamics.

The second law can be derived theoretically from the underlying laws using statistical mechanics. The basic idea is that when we ignore all the microscopic details of a system and characterize it by macroscopic parameters like pressure and temperature, then there may be many more "microstates" (exact microscopic details of the system's state) for some "macrostates" (a particular set of values for the macroscopic parameters) than for other macrostates, and the ones with more microstates have a higher entropy. The evolution of the system's microstate over time, guided by the underlying physical laws, is statistically more likely to take it to macrostates that have a higher number of microstates.

Just because Newton's laws are "quantitatively" symmetric through
time-reversal, (i.e.: equal and opposite) does not mean we will ever see a fly stop a freight train.

I think you're confused here, the fact that we never see a fly stop a freight train has nothing to do with thermodynamics, even if the collision is perfectly elastic you'd never see a situation where the collision causes a major change in the train's velocity, unless the fly is moving at a significant fraction of light speed. The time-reversed situation isn't seen either--you never see a fly cause a freight train at rest to acquire a significant velocity.

My point, or question is not why is there a second law of thermodynamics, it is that the second law
conditions the mechanics according to our frame of reference.
The mechanics of time-reversal measured by an observer are different according to their frame of reference.

No idea what you mean here. If some behavior before and after a collision is thermodynamically improbable in one frame, then when you translate that to another frame, it's equally improbable. There's no frame-dependence in the likelihood of particular types of collisions.

This is a trivial observation in most cases, but in the example I've given it makes the difference between
the law of conservation of momentum displaying increased entropy or decreased entropy.
In other words, from one of only two frames, both involved in the event, the second law is upheld
in one and contradicted in the other.

What two frames are you talking about? Different frames in SR don't disagree on which direction of time is the forward direction--if event B happens after event A on the worldline of some object in one frame, then B happens after A in every frame. So if you are thinking of viewing a given collision both forwards and backwards, this cannot be a valid example of the same situation viewed from the perspective of two different SR frames. And as long as you stick to SR frames related by the Lorentz transformation, you'll always find that if the second law is upheld in one frame, then the second law is also upheld when you view the same events in another frame.

 

[yuiop]

First, my appologies for sending this thread on a large detour into thermodynamics in the context of cosmology. George was right to split the thread and I am sorry about the extra work I created for George. My only excuse is that I spend a lot of time in both the Relativity forum and the Cosmology forum and I probably forget which forum I am in most of the time. (I know... poor excuse )

...
There is a difference between the time-reverse symmetry of the laws and the time-reverse symmetry of mechanics.
The laws must, in principle, uphold under time-reversal or they would be expressions of or indications of
faulty axiomatic foundations.
Mechanics on the other hand are not so easily reversed. The kinematics of an event are the measurable dimensions
of the system, which are easily reversed as they are simply "quantitative" expression of dimension.
To reverse the direction of time you simply flip the sign to negative and everything runs (equates) backwards.
The dynamics are the problem, as they define the forces (classically) that give rise to the kinematics.
This means a translation of momentum between differing masses must consider the "empirical" evidence
of the second law of thermodynamics. Just because Newton's laws are "quantitatively" symmetric through
time-reversal, (i.e.: equal and opposite) does not mean we will ever see a fly stop a freight train.

The problem as I see it is the "qualitative" expression of the laws under time-reversal.
My point, or question is not why is there a second law of thermodynamics, it is that the second law
conditions the mechanics according to our frame of reference.
The mechanics of time-reversal measured by an observer are different according to their frame of reference.
This is a trivial observation in most cases, but in the example I've given it makes the difference between
the law of conservation of momentum displaying increased entropy or decreased entropy.
In other words, from one of only two frames, both involved in the event, the second law is upheld
in one and contradicted in the other.
This seems to indicate a "preferred" frame with respect to the laws of mechanics.
More importantly it says something fundamentally significant about the principle of relativity
and time. The (ideal) instantaneous exchange of momentum in the collision of two differing
masses, presents a "qualitative" change in dimension depending on the frame of the observer.

There are examples of the "arrow of time" and increasing entropy even when perfectly elastic collisions are considered. A classis example is a cluster of gas molecules in one corner of a box. Random (elastic) collisions between the gas molecules, disperses the gas throughout the box. The time reverse, where random motion of the gas molecules initially spread out in the box, results in all the gas molecules clustered in one corner is not impossible, but statistically it is enormously improbable.

In the inelastic case, when the part of the kinetic energy of the ball of putty is converted into thermal energy, a close examination of the interactions during the collision at the molecular level reveals that a lot of the molecular interactions are also elastic collisions. The difference is that the linear kinetic energy of the ball becomes randomly directed kinetic motion of the individual molecules which is one form of what we call heat. The situation gets more complicated if the individual molecules get sufficiently excited that they radiate photons or if chemical bonds are formed when the molecules are in close proximity. That would be a bit like the "locking spring" Dalespam refers to.

So whether elastic or inelastic collisions are considered, the principle of increasing entropy is basically about what is statistically more probable. While classical Newtonian physics does not rule out time reversal of kinetic interactions, thermodymanics suggests that events occurring in one direction are much more probable that events happening in the reverse sequence.

However, time does not require a "thermodynamic arrow of time" in order to advance. Take this example of throwing a ball up in the air and taking a photograph of the ball on its way up and another photograph of the ball at the same height but on its way down. With a very fast camera, so that any blur due to motion is undetectable, you would not be able to tell which is the picture of the ball on its way up and which is the picture of the ball on its way down. Thermodynamic considerations would not predict what is statistically more likely to happen next to the ball in any given picture. The arrow of time, in this case, is determined by momentum, or put another way, what will happen in the next instant is determined by the current instant and what happened in the previous instant.

 

[Dale]

I had hoped to get back to this sooner but I'm in the middle of a "money pit" renovation that is taking all my free time

Good luck on your projects!

There is a difference between the time-reverse symmetry of the laws and the time-reverse symmetry of mechanics.

You are mistaken here. If the laws that describe a process exhibit some symmetry then that process also exhibits that symmetry. There is no difference between the time-reverse symmetry of the laws and the time-reverse symmetry of mechanics. There is likewise no difference between the asymmetry of the laws of thermodynamics and the asymmetry of thermodynamic processes.

 

[Chrisc]

There's a lot of unexpected confusion or ambiguity in the premise of my question.
Obviously I didn't pose it as concise as I should have.

My question comes down to this: the "measured" exchange of momentum
between differing masses in collisions of uniform motion, is(appears to be) a relative
measure that upholds or violates the laws through time reversal depending on the
frame of the observer.

The inertial energy (rest mass) of a small mass will not overcome (is less than) the
energy of momentum of a larger mass, therefore the small mass at rest will not bring
the larger mass in motion to rest.
When collisions of this type (ideal, inelastic collisions of rigid, non-composite bodies -
hypothetical events designed for the purpose of considering the principles of the laws,
not the real mechanics of the event) are observed from a position of rest with respect
to each of the two masses involved, Newton's laws are upheld and Einstein's SR principle
of relativity accounts for the differing but valid observations between each observer.
To test the extent of the principle of these classical laws, I considered the same events reversed in time.
One would assume the second law of thermodynamics predicts the exchange of
momentum is both conserved and leads to observable "decrease" in entropy under
time reversal. Which is to say the law of inertia would simply reverse such that a
small mass would bring a larger mass to rest - a clear indication of the reversal
of the second law.
This is in fact the case when the observer is initially at rest with the larger mass.
It is not the case when the observer is initially at rest with the smaller mass.
The statistical nature of the second law is irrelevant to this asymmetry as this
inconsistency is directly correlated to the masses involved.
My question is whether there is any known reason this symmetry holds from
one frame (larger mass) and fails from the other (smaller).
At first glance it appears this asymmetry suggests time-reversal reveals a preferred
or privileged frame of reference. It seems to suggest the dynamical laws are upheld
only when one of the masses (either) is defined as the mass in motion.
In other words the relativity of momentum is not as clear cut as the relativity of motion.

 

[JesseM]

My question comes down to this: the "measured" exchange of momentum
between differing masses in collisions of uniform motion, is(appears to be) a relative
measure that upholds or violates the laws through time reversal depending on the
frame of the observer.

I still don't understand where the "frame of the observer" comes into it. Do you understand that different frames in SR don't disagree on the direction of future vs. past for causally related events? If so, would you agree that if a particular inelastic collision is thermodynamically unlikely in one frame, it's thermodynamically unlikely in every frame? So what is it that "depends on the frame of the observer" here, specifically?

When collisions of this type (ideal, inelastic collisions of rigid, non-composite bodies -
hypothetical events designed for the purpose of considering the principles of the laws,
not the real mechanics of the event) are observed from a position of rest with respect
to each of the two masses involved, Newton's laws are upheld and Einstein's SR principle
of relativity accounts for the differing but valid observations between each observer.
To test the extent of the principle of these classical laws, I considered the same events reversed in time.
One would assume the second law of thermodynamics predicts the exchange of
momentum is both conserved and leads to observable "decrease" in entropy under
time reversal. Which is to say the law of inertia would simply reverse such that a
small mass would bring a larger mass to rest - a clear indication of the reversal
of the second law.
This is in fact the case when the observer is initially at rest with the larger mass.

Huh? An observer at rest with respect to the larger mass is not going to see a reversal of the second law! He'll see the total kinetic energy of the centers of mass decrease rather than increase, as should be true for any inelastic collision that obeys the second law (because some of the kinetic energy of the centers of mass is converted to heat). If you think otherwise, please explain your reasoning.

 

[Chrisc]

I do and I would until I thought about this example and the time-reverse dynamics required to explain it.
1.
A large mass M is moving with constant velocity v toward a small mass m as measured by an observer R
initially at rest with respect to m.
After a collision through the center of their masses, R measures the velocity of M to be 1/2v and the velocity of m to be v.

Now take the time reverse this event.
2.
R observes the large mass M moving toward him at 1/2v and the smaller mass m moving toward him at v.
M and m collide and m comes to rest with respect to R and M continues at v.

The forward and time-reverse of this event holds to the laws mechanics.
If you could view the time reverse version it would appear as any natural collision of the same proportions forward in time.

Now place the observer initially at rest with respect to M and they observe the following.
3.
The smaller mass m moves toward R and M with velocity v.
After the collision, m is at rest with R and M moves away at 1/2v.

Now take the time reverse of this event.
4.
R observes M moving toward m at 1/2v.
After the collision M is at rest with R and m moves away at v.
Under these mechanics, all large masses should come to rest upon colliding with smaller masses.

So it would seem (4.) is correct in that a reversal of time should result in the reversal of the second law and the converse of the law of inertia.
The problem is with (2) as it presents mechanics that uphold the second law under time-reversal and the law of inertia.
That they differ is my point. They differ when they are the "same" event viewed from different inertial frames.

 

[yuiop]

There's a lot of unexpected confusion or ambiguity in the premise of my question.
Obviously I didn't pose it as concise as I should have.

Hi Chrisc,

Your right. I was a bit confused about what you were getting at and after checking it all out again I think I have a better handle on it now and it turns out the calculations in your diagram are correct for a inelastic collision.

The solution to the apparent paradox is this.

First case (observer is initailly at rest with the small ball)
Total momentum of the system before and after collison is 4mv.
Total KE before collision is 4 mv^2
Total KE after collision is 3 mv^2

There is a loss of 1 mv^2 as heat during the collision. When the process is time reversed the system starts with 3 mv^2 of energy and finishes with 4 mv^2 of energy so an input of heat is required and this is shown as the freak lightning bolt that hits the balls as they collide in the attached diagram.


Second case (observer is initially at rest with the large ball)
Total momentum of the system before and after collison is 2mv.
Total KE before collision is 2 mv^2
Total KE after collision is 1 mv^2

There is a still a loss of 1 mv^2 as heat during the collision. When the process is time reversed the system starts with 1 mv^2 of energy and finishes with 2 mv^2 of energy and this is again shown as the freak lightning bolt that hits the balls as they collide in the attached diagram. It is the additional energy supplied by the lightning bolt that brings the large ball to a complete stop.

The thermodynamic arrow of time is clear here. It is statistically unlikely that heat (or lightning) from the surrounding environment concentrates and imparts coherent momentum to the large ball exactly as required at the moment of collision in the reverse time scenario. Or as George would say, "it's not going to happen" :P

Perhaps I should add that the results are consistent from which ever inertial reference frame you look at it from. All the velocities in the second case are simply the velocities in the first case minus 2v. Also it should be clear that inelastic collisions are not time reversible in general.

 

[JesseM]

I do and I would until I thought about this example and the time-reverse dynamics required to explain it.
1.
A large mass M is moving with constant velocity v toward a small mass m as measured by an observer R
initially at rest with respect to m.
After a collision through the center of their masses, R measures the velocity of M to be 1/2v and the velocity of m to be v.

OK, for simplicity let's just use Newtonian formulas, which will be approximately correct if v is small compared to the speed of light. Before the collision the total momentum is Mv, afterwards it's Mv/2 + mv, and since momentum is conserved in inelastic collisions this means m = M/2. So, the kinetic energy before the collision is (1/2)*Mv^2, and afterwards it's (1/2)*M*(v/2)^2 + (1/2)*(M/2)*v^2 = (1/8)*Mv^2 + (1/4)*Mv^2 = (3/8)*Mv^2. So, the kinetic energy decreases as would be expected in an inelastic collision.

Now take the time reverse this event.
2.
R observes the large mass M moving toward him at 1/2v and the smaller mass m moving toward him at v.
M and m collide and m comes to rest with respect to R and M continues at v.

The forward and time-reverse of this event holds to the laws mechanics.
If you could view the time reverse version it would appear as any natural collision of the same proportions forward in time.

The time-reversed version would be mechanically possible, but it would also be a "thermodynamic miracle" since it would require a huge number of random vibrations in the molecules of the objects (heat) to all coincidentally synchronize at the moment of the collision and increase their combined kinetic energy in this frame, from (3/8)*Mv^2 to (4/8)*Mv^2.

Now place the observer initially at rest with respect to M and they observe the following.
3.
The smaller mass m moves toward R and M with velocity v.
After the collision, m is at rest with R and M moves away at 1/2v.

Sure. And still we see that kinetic energy has decreased, as would be expected from thermodynamics. Before the collision, total kinetic energy in this frame is (1/2)*(M/2)*v^2 = (1/4)*Mv^2. After the collision, total kinetic energy in this frame is (1/2)*(M)*(v/2)^2 = (1/8)*Mv^2.

Now take the time reverse of this event.
4.
R observes M moving toward m at 1/2v.
After the collision M is at rest with R and m moves away at v.
Under these mechanics, all large masses should come to rest upon colliding with smaller masses.

But again, the time-reversed version requires a thermodynamic miracle where random heat vibrations suddenly synchronize and give a kick to the masses, doubling their combined kinetic energy in this frame.

So it would seem (4.) is correct in that a reversal of time should result in the reversal of the second law and the converse of the law of inertia.
The problem is with (2) as it presents mechanics that uphold the second law under time-reversal and the law of inertia.

I don't follow. The time-reversed scenario (2) violates the second law just like the time-reversed scenario (4); each one involves heat being spontaneously converted into extra kinetic energy for the center of masses.

 

[yuiop]

Hi JesseM,

I take it from our last two posts that we are in agreement that what Chrisc is missing is that linear kinetic energy is converted into heat energy in the forward direction and that it is extremely unlikely that random heat energy would be spontaneously converted to linear motion in the reverse time direction.

A much simpler example is dropping a ball of putty to the floor from 2 meters. Let's assume the putty does not bounce and just comes to stop. Some of the initial kinetic energy is used up in deforming the putty and the remainder isdisperced as heat and vibrations in the floor and the flattened putty. The time reversal of random heat vibrations spontaneously focusing to eject the putty 2 metres into the air (and reform it into a perfect ball) is unlikely.

 

[Chrisc]

Kev and JesseM, you've both taken this out of its original context.
I had qualified this as a system of rigid, non-composite bodies in order to simplify and focus the
dynamics by removing molecular motion (heat). The idea is to consider the principle of the laws
by examining the exchange and/or conversion of the energies involved (mass, inertia and momentum) through time.
It would be "a miracle" for the constituent particles of a body to align their momentum in such a way
as to "kick" an adjacent body (as a whole) into motion. But this "miracle" would happen in the time-reverse scenario.
It must happen if the laws are correct in the time forward scenario. This miracle is just a collective
molecular example of the simpler version I presented which is a smaller mass brings a larger mass to rest.

You have both described the mechanics that justify our concept of a thermodynamic "direction" of time.
The crux of what I'm trying to figure out is whether the principle of relativity posses enough symmetry
to survive a translation in time, i.e.: is the principle of relativity time-reverse symmetric?
In the observable mechanics of motion (relative velocity) it seems obvious it would. Velocity is kinematical,
as such there is no need to consider dynamics in a causal sense. So the time-reverse symmetry of the
kinematics of Special relativity seems pretty straight forward - it holds.
But, when mass is part of the consideration of the time-reverse symmetry of relativity, its measure and
the laws governing its interactions seem to break the relativistic principle. Holding the dynamical laws
to time-reverse symmetrical appears to reveal a break in the symmetry of the principle of relativity.
It seems there is a "special" case where one can claim a preferred frame of reference.
It is the frame where the dynamics of a single event do NOT break the time-reverse symmetry of the dynamical laws.
I hope that makes sense.
If you consider the collisions as a complete transfer of momentum and inertial energy without dissipating
any energy to heat, you will see the mechanics conflict with the laws. Once the conflict is apparent you
can put the heat energy back in and consider the same event in terms of the direction of heat transfer.
It does not solve the conflict it just changes the mechanics to a more complex collection of smaller masses
where the same issue arises in any collision through the center of mass.

 

[JesseM]

Kev and JesseM, you've both taken this out of its original context.
I had qualified this as a system of rigid, non-composite bodies in order to simplify and focus the
dynamics by removing molecular motion (heat).

But you can't have inelastic collisions that don't involve heat (or radiation I suppose). Energy must be conserved; if the total linear kinetic energy of the two bodies decreases after the collision, where does that energy go, if not to increasing the energy of the random vibrations in the molecules of each body (heat)? And the collision you described in your example was clearly an inelastic one where linear kinetic energy was not conserved. If you have some other physically realistic possibility in mind for where that energy went, please explain.

It would be "a miracle" for the constituent particles of a body to align their momentum in such a way
as to "kick" an adjacent body (as a whole) into motion. But this "miracle" would happen in the time-reverse scenario.
It must happen if the laws are correct in the time forward scenario. This miracle is just a collective
molecular example of the simpler version I presented which is a smaller mass brings a larger mass to rest.

What do you mean "it must happen"? Do you just mean it must be possible according to the laws of mechanics (which I would agree with), or are you saying it must be just as likely as the time forward scenario (which I would disagree with)?

The crux of what I'm trying to figure out is whether the principle of relativity posses enough symmetry
to survive a translation in time, i.e.: is the principle of relativity time-reverse symmetric?

The "principle of relativity" as it's normally understood is not intended to cover time-reversed coordinate systems. However, it is true that the laws of classical physics are T-symmetric, so that they should work the same in time-reversed coordinate systems, and in quantum field theory the laws are CPT-cymmetric, which means they work the same in coordinate systems where the labels of "forward in time" and "backward in time" have been reversed and where the positive and negative direction on all the spatial axes have been reversed (a change in 'parity', the P in CPT) and where the labels for positive and negative charge have been reversed (the C in CPT).

But, when mass is part of the consideration of the time-reverse symmetry of relativity, its measure and
the laws governing its interactions seem to break the relativistic principle. Holding the dynamical laws
to time-reverse symmetrical appears to reveal a break in the symmetry of the principle of relativity.

Only in a statistical sense that the time-reversed scenario is less likely, the time-reversed scenario doesn't violate any of the fundamental laws so it's certainly not forbidden. And this difference in likelihood has to do with cosmology and the fact that our universe apparently started off in a very low-entropy state (for reasons that aren't really understood at present), so that entropy has increasing ever since; if the universe were already at equilibrium, then statistically we'd expect that random fluctuations taking systems from higher entropy to lower would be just as common as fluctuations taking systems from lower to higher (though the vast majority of these fluctuations would be small and not noticeable on macroscopic scales).

It seems there is a "special" case where one can claim a preferred frame of reference.

You're misusing the language here. "Frame of reference" only refers to the different coordinate systems related by the Lorentz transformation, which all agree on the order of causally-related events; a coordinate system whose definition of forward in time and backwards in time is reversed is not a valid "frame of reference" in SR.

If you consider the collisions as a complete transfer of momentum and inertial energy without dissipating
any energy to heat, you will see the mechanics conflict with the laws.

But in your example there clearly was not a complete transfer of "inertial energy", since the combined linear kinetic energies of the two balls after the collision was different than their combined kinetic energy before the collision. If you consider an elastic collision where combined kinetic energy is conserved, then you will see that this kind of collision is just as likely in the time-reversed version.

 

[DrGreg]

Chrisc, maybe the point you haven't realized is that conservation of momentum is not sufficient to solve the problem of what happens after the collision in post #33. Your solution is one of many that conserve momentum; you need to consider energy, too, to find a unique solution.

If we restrict ourselves to Newtonian mechanics instead of relativistic (i.e. assume small velocities), then to conserve momentum, if I've done the maths right, the post-velocity u of (M = 2m) can take any value between v/3 and v, and the post-velocity of (m) is then 2(v - u).

For an elastic collision, u = v/3 and the post-velocity of (m) is 4v/3 -- this is symmetric as the difference of velocities is v before and after.

 

[Chrisc]

I'm sorry. I see why this makes no sense. I've been misusing the term "inelastic" collision.
I did not mean to use it in the conventional sense.
To be clear, below is the definitions as I understand them, for elastic and inelastic collisions.
An inelastic collision is used to describe the collision of bodies that, due to their inability
to deflect incident kinetic energy of the collision to the internal motion of their constituent parts,
must disperse (radiate)the energy in excess of the total energy of the system in some other form such as heat.
An elastic collision describes the collisions between bodies that are capable of such deflection,
resulting in the total energy being conserved in the sum of the main body momentums and
the motion of their constituent parts (or molecules).

Again, I am sorry for not checking the proper use.
I meant neither, but inelastic in the sense of a single, non-composite, rigid body that does not flex
and has no constituent parts onto which it can defer the energy internally.
A body that moves according to the exchange of the inertial and kinetic energy of the collision.
This is thought experiment centered on the principles of the laws, not a real description of collisions.

The total energy of the system is symmetric in all cases when the collisions are considered as mentioned above.(conserved after collision)
The lack of symmetry is not in the total energy before and after the collision, it is in the physical dynamics before and after the collision.

I had mentioned earlier, and forgot to follow up on the objections, that the time-reverse symmetry of
the laws must be distinguished from the time-reverse symmetry of the mechanics.
If time-reversal is taken as just the reversal of "clock-ticks", then the same laws must define
the observed reverse kinematics.
If time-reversal is taken to include the reversal of physical dynamics, then the same laws must be
considered in their full time-reverse symmetry.
For example: when we consider the broken glass collecting its pieces together and jumping back up onto the table,
we are considering the probability of all the momentum of the pieces being properly directed such that the
glass becomes unbroken and the continued momentum of the glass launches itself back up on the table.
It is extremely improbable, but not impossible according to the laws. (assuming there is nothing more to know about the nature of time)
This analogy considers the reverse kinematics (clock-ticks) driven by the "same" laws not the reversal of the laws.

When this analogy is considered under the time-reversal of the laws, the physical dynamics of the laws are reversed.
Gravity is a repelling force. The table will not be waiting for the glass to leap back up. It is impossible to consider
the kinematics being exactly reversed in this type of time-reversal. The dynamics giving rise to the kinematics may express
a symmetry of reversal (the axis being a point in time where the reversal is considered) but the kinematics from that point on
are exactly reversed of what the laws predict in forward time. Small masses bring large masses to rest.
Masses repel others proportional to the sqrt of their distance.

This being the case, the example I gave represents both types of time-reversal.
In (2.) the same laws accurately predict the dynamics necessary to give rise to the kinematics observed.
There is nothing unusual in the time-reverse of (2) If you were to look at a film of (1) running backward you would find no conflict with the laws.
In (4) although the total energy of the system is conserved as in (1,2, and 3), it is at the expense of contradicting the laws.
If you watched a film of (3) running backward you would see (4) and claim "the film is running backward".
Because a small mass cannot bring a larger mass to rest.
So if (2) and (4) are distinctly different in the dynamics required to give rise to such kinematics,
they are a result of the frame of the observer being initially at rest with respect M or m.

 

[yuiop]

This being the case, the example I gave represents both types of time-reversal.
In (2.) the same laws accurately predict the dynamics necessary to give rise to the kinematics observed.
There is nothing unusual in the time-reverse of (2) If you were to look at a film of (1) running backward you would find no conflict with the laws.
In (4) although the total energy of the system is conserved as in (1,2, and 3), it is at the expense of contradicting the laws.
If you watched a film of (3) running backward you would see (4) and claim "the film is running backward".
Because a small mass cannot bring a larger mass to rest.
So if (2) and (4) are distinctly different in the dynamics required to give rise to such kinematics,
they are a result of the frame of the observer being initially at rest with respect M or m.

Back in post#35 JesseM showed you that the total kinetic energy of the experiment you described in post#33 is not conserved. If you do not want to consider energy dissapated as thermal energy then you can not say the total energy of the system is conserved. You need to consider a perfectly elastic collison to be able to justify the conservation of energy in a system that does not include thermal energy or thermodynamic miracles. Back in post#17 I showed that with initial conditions as described in your first post:

Ball B1: m_1=2m, v_1=2v
Ball B2: m_2=1m, v_2=0v

the final velocities would be 2/3v and 8/3v for B1 and B2 respectively in a perfectly elastic collision. All positive velocities are to the right with respect to the inertial observer in the reference frame that ball B2 is initially at rest in.

Now if you considerthe point of view of a different observer who has velocity 2/3v relative to the first observer, the final velocities of the balls according to him are 0v for B1 and 2v for B2. So in this perfectly elastic collison the second observer sees the large ball (B1) as being brought to a stop by the smaller ball. This can be observed in any collision simply by choosing a reference frame for the observer that coincides with the final velocity of the larger mass. There is no law of physics that says a large ball can not be brought to rest by a smaller ball but there are laws about conservation of momentum and total energy. You have to account for all the energy.

 

[JesseM]

Again, I am sorry for not checking the proper use.
I meant neither, but inelastic in the sense of a single, non-composite, rigid body that does not flex
and has no constituent parts onto which it can defer the energy internally.
A body that moves according to the exchange of the inertial and kinetic energy of the collision.
This is thought experiment centered on the principles of the laws, not a real description of collisions.

But even in a thought experiment, we must respect principles of physics like conservation of energy. Do you not see that in your example above, if we calculate the kinetic energy for each body according to the standard formula (1/2)*mv^2, then the total kinetic energy after the collision was different from the total kinetic energy before? If you want a thought experiment involving bodies that move "according to the exchange of the inertial and kinetic energy" (although I don't know what you mean by 'inertial energy', are you talking about momentum?), then you need one where energy is conserved. Do you wish to provide a new example where energy is conserved, or do you not understand that in your example energy was not conserved, if none of the kinetic energy was transformed into heat?

The total energy of the system is symmetric in all cases when the collisions are considered as mentioned above.(conserved after collision)
The lack of symmetry is not in the total energy before and after the collision, it is in the physical dynamics before and after the collision.

If you pick an example where both momentum and kinetic energy are conserved--which, by definition, is an "elastic collision"--then there will be no "lack of symmetry", the collision will be just as consistent with all laws (and just as probably thermodynamically) in the time-reversed version as in the forward-time version.

I had mentioned earlier, and forgot to follow up on the objections, that the time-reverse symmetry of
the laws must be distinguished from the time-reverse symmetry of the mechanics.

Could you explain what you mean by this distinction? Time-reverse symmetry of the laws logically implies that for any physical scenario consistent with the laws (like a collision), if you look at a backwards movie of that system's behavior, you could in principle set up a different physical system with different initial conditions such that its behavior in the forward-time direction looks precisely like the backwards movie of the first system. Is this different than what you meant by "time-reverse symmetry of the mechanics"?

If time-reversal is taken as just the reversal of "clock-ticks", then the same laws must define
the observed reverse kinematics.

Huh? Why? It is perfectly possible to imagine laws of physics (different from the actual laws of physics in our universe) where the reverse kinematics are not governed by the same laws. For example, imagine that objects in a gravitational field could only move down as time moves forward, never up (in reality of course an object can bounce on the ground and move up). If you switch which direction in time you label "forward", objects in a gravitational field could only move up as time moves forward, never down. This would require a different set of equations to describe the object's motion as a function of time.

For example: when we consider the broken glass collecting its pieces together and jumping back up onto the table,
we are considering the probability of all the momentum of the pieces being properly directed such that the
glass becomes unbroken and the continued momentum of the glass launches itself back up on the table.
It is extremely improbable, but not impossible according to the laws. (assuming there is nothing more to know about the nature of time)
This analogy considers the reverse kinematics (clock-ticks) driven by the "same" laws not the reversal of the laws.

I don't know why you consider kinematics as "clock ticks", and I don't understand what you mean by "reversal of the laws" as opposed to "reverse kinematics driven by the same laws". Could you explain specifically how these terms apply to your example?

When this analogy is considered under the time-reversal of the laws, the physical dynamics of the laws are reversed.
Gravity is a repelling force.

No no no, you're totally misunderstanding the idea of time-reversal symmetry here! The symmetry means that the laws do not change in any way in the time-reversed version, the scenario where the broken glasses are shot upwards can still be understood in terms of the same old attractive gravitational force. The point is that when you reverse all the molecular dynamics, the random motions of molecules due to heat suddenly synchronize and give the pieces of glass an upwards "kick" which shoots it into the air, just like you can send a soccer ball up into the air by kicking it with your foot--this certainly doesn't require gravity to be repulsive! As I said before, time-reversal symmetry means that by setting up precisely the right initial conditions (and assuming deterministic laws), you can create a physical situation whose behavior in the forward time direction looks precisely the same as the backwards movie of the first situation. In classical terms, if you take a snapshot of the positions and velocities of every particle at some time after the glass has fallen to the floor, and then you create a new set of initial conditions where all the positions are the same but all the velocities are reversed in direction, then when you evolve this new set of initial conditions forward, it will behave just like the backwards version of the original system.

Small masses bring large masses to rest.
Masses repel others proportional to the sqrt of their distance.

Nope, if the laws of physics are time-symmetric, the laws are precisely the same in the backwards version as the forwards version. And of course your "small masses bring large masses to rest" is very vague--it is quite possible to come up with collisions where large masses are brought to rest by small ones in the forward-time direction, it just depends on the details of each object's speed and mass.

This being the case, the example I gave represents both types of time-reversal.

The example you gave is simply impossible unless some kinetic energy is dispersed as heat, because the combined kinetic energy of both masses before the collision was different than the combined kinetic energy of both masses afterwards. Do you disagree?

In (2.) the same laws accurately predict the dynamics necessary to give rise to the kinematics observed.
There is nothing unusual in the time-reverse of (2) If you were to look at a film of (1) running backward you would find no conflict with the laws.

Again, the only possible way (2) could happen is if heat suddenly becomes kinetic energy, since in (2) the kinetic energy of both masses after the collision is larger than the kinetic energy of both masses before. I suspect the problem here is that you are just thinking of the laws in terms of vague qualitative terms, you think that (2) is OK because it doesn't involve a "large mass being stopped by a small mass" like in (4), but it really is necessary to make a quantitative calculation of the energy before and after the collision in order to have a sensible discussion of whether this is consistent with the laws of physics.

In (4) although the total energy of the system is conserved as in (1,2, and 3), it is at the expense of contradicting the laws.

Total energy is conserved?? Where are you getting this? I already gave you a detailed analysis in post #35 showing that the combined kinetic energy is not conserved in any of your scenarios, did you even read that? Do you understand that kinetic energy is given by the formula (1/2)*mv^2, and that in order for momentum to be conserved in your scenario, the larger object must have twice the mass of the smaller one, so if the larger object has mass M and the smaller has mass m, then m = M/2? If you agree with that, then once again, in scenario (1) you said:

large mass M is moving with constant velocity v toward a small mass m as measured by an observer R
initially at rest with respect to m.
After a collision through the center of their masses, R measures the velocity of M to be 1/2v and the velocity of m to be v.

So before the collision the first object has mass M and velocity v, so its kinetic energy is (1/2)*Mv^2, while the second object has velocity v=0 and mass m = M/2, so its kinetic energy is (1/2)*(M/2)*(0)^2 = 0. So, the total kinetic energy before the collision is (1/2)*Mv^2. Then after the collision, the first object still has mass M but now has velocity (v/2), so its kinetic energy is (1/2)*(M)*(v/2)^2 = (1/8)*Mv^2, while the second object has mass m = M/2 and velocity v so its kinetic energy is (1/2)*(M/2)*v^2 = (1/4)*Mv^2. So, the combined kinetic energy after the collision is (1/8)*Mv^2 + (1/4)*Mv^2 = (3/8)*Mv^2. So, the total kinetic energy of both objects has decreased from (1/2)*Mv^2 to (3/8)*Mv^2, meaning that unless some of that kinetic energy is dispersed as heat or electromagnetic waves or some other form, the scenario would be physically impossible because energy is not conserved. If you disagree, what part of my analysis do you object to?

 

[Dale]

When this analogy is considered under the time-reversal of the laws, the physical dynamics of the laws are reversed.
Gravity is a repelling force. ... Masses repel others proportional to the sqrt of their distance.

Forces are invariant under time reversal. Remember: a = d²x/dt². So the power of 2 on the dt means acceleration is "even" under time reversal. Since acceleration is even and force is proportional to acceleration then force is also even under time reversal. Time reversed Newtonian gravity is still an attractive force.

You may want to do a little study before coming back to this. I don't really see why you care about time symmetry, but if it is important to you then you really should approach it in a little more organized manner.

Again, you don't need to focus on a specific example, you need only consider the laws themselves. If the laws exhibit some symmetry then any example you provide must either exhibit the same symmetry or it must not follow the laws.

 

[Chrisc]

So, the total kinetic energy of both objects has decreased from (1/2)*Mv^2 to (3/8)*Mv^2, meaning that unless some of that kinetic energy is dispersed as heat or electromagnetic waves or some other form, the scenario would be physically impossible because energy is not conserved. If you disagree, what part of my analysis do you object to?

The energy is conserved in the momentum of the system measured in the frame of the observer.
The 1/8*Mv^2 that you claim is missing is the inertia of m.
The force required to set a body in motion must equal or exceed its inertia.
You cannot move a body from rest to a velocity less than that of the body
imparting the force without also slowing the latter.
This is why M continues after the collision at 1/2v not v, and why m is set
in motion with velocity v not 1/2v.
The missing energy of motion is not missing in the total energy of the system
it is converted to momentum.
This is a thought experiment, the bodies are non-composite, so consider the
heat energy if you must, as the motion of the whole body instead of the motion
of its constituents, as it has no constituents.
Momentum and kinetic energy are frame dependent quantities.
The issue here is that the inertia of M is greater than the inertia of m therefore
as a frame dependent quantity, the total momentum of the system as measured
by the observer when at rest with M, is less than the total momentum of the
system when they are at rest with m.
So although the velocity of M and m is the same in both cases (relative), the total energy is not.
If we simply consider a change in the observers position of rest with respect to each
mass before and after collision, the dynamics are valid with respect to the frame
in each case.
But, in the time-reverse version this symmetry of the dynamics holds in the case
where the observer is initially at rest with respect to m, but fails when initially
at rest with respect to M.

 

[JesseM]

The energy is conserved in the momentum of the system measured in the frame of the observer.

That makes no sense at all. Do you understand that "momentum" and "energy" are entirely separate quantities, with the momentum of an object with mass m and velocity v being given by the formula m*v, while the kinetic energy of the same object is given by the formula (1/2)*m*v^2? There are of course other forms of energy, like potential energy and heat (which is really just the combined kinetic energy of all the molecules of the object moving relative to the object's center of mass). But momentum is definitely not a form of energy--in the MKS system of units, momentum has units of kilograms*meters/second, while all forms of energy have units of kilograms*meters^2/second^2.

The 1/8*Mv^2 that you claim is missing is the inertia of m.
The force required to set a body in motion must equal or exceed its inertia.

I'm sorry, but you are obviously using terminology without having bothered to read the accepted definitions here (as you were in the case of inelastic vs. elastic collisions). "Inertia" is understood as the tendency of objects to resist acceleration, and can be understood in terms of the Newtonian formula F = m*a, where F is the force on an object, m is its inertial mass, and a is the amount of acceleration it experiences when that force is applied. You can see that for a given applied force F, then the greater the inertial mass m, the smaller the acceleration a. But if F is the only force on the object--if there is no counter-force in the opposite direction to balance it out, like friction--then an object will always accelerate a little bit when force is applied, so your statement "the force required to set a body in motion must equal or exceed its inertia" is totally wrong. It is also totally wrong to treat "inertia" as a form of energy.

You cannot move a body from rest to a velocity less than that of the body
imparting the force without also slowing the latter.

Sure, that's obvious just based on conservation of momentum. If the body started at rest then its momentum m*v was zero, so after the collision its momentum increases, which means the momentum of the other object must decrease by the same amount in order for momentum to be conserved. However, just because momentum is conserved, that alone is not enough to guarantee that the collision is a physically realistic one; you must also check whether energy is conserved, if it's not then your scenario is every bit as impossible as the scenario where both objects' velocities increase.

The missing energy of motion is not missing in the total energy of the system
it is converted to momentum.

Again, this is nonsense. Momentum is not a form of energy, and energy can only be converted to another form of energy, like linear kinetic energy being converted to heat or to potential energy (like a ball thrown upward in a gravitational field).

This is a thought experiment, the bodies are non-composite, so consider the
heat energy if you must, as the motion of the whole body instead of the motion
of its constituents, as it has no constituents.

Heat is always just the combined kinetic energy of all the different parts of the object moving relative to one another, so this doesn't really make much sense. I suppose you could imagine a continuous jello-like object that wasn't made out of discrete components like atoms, but which was nonrigid so that different points in the object could be in motion relative to one another, but it definitely wouldn't make sense to talk about the heat of a rigid, non-composite object.

Momentum and kinetic energy are frame dependent quantities.
The issue here is that the inertia of M is greater than the inertia of m therefore
as a frame dependent quantity, the total momentum of the system as measured
by the observer when at rest with M, is less than the total momentum of the
system when they are at rest with m.
So although the velocity of M and m is the same in both cases (relative), the total energy is not.

It's true that momentum and energy are frame-dependent. However, within any single frame, it is required by the laws of physics that the total momentum of a system as measured by that frame must be constant as long as there are no external forces acting on the system (just imagine a collision in deep space), and that the total energy of the system as measured by that frame must be constant as well. It works out so that if the momentum and energy are conserved in one inertial frame, that guarantees that the momentum and energy will also be conserved in every other inertial frame, even though different frames have different numbers for the total momentum and energy.

When I pointed out that in your scenario, total linear kinetic energy went from (1/2)*M*v^2 before the collision to (3/8)*M*v^2 afterwards, this was from the perspective of a single frame, not two different frames. So again, unless you can provide a physically reasonable explanation as to what other form of energy that missing kinetic energy was converted to, your scenario is violating the basic laws of physics of our universe, and so is completely impossible.

 

[Dale]

That makes no sense at all. Do you understand that "momentum" and "energy" are entirely separate quantities ... But momentum is definitely not a form of energy--in the MKS system of units, momentum has units of kilograms*meters/second, while all forms of energy have units of kilograms*meters^2/second^2.

Not only that, but momentum is a vector and energy is a scalar. Even if they had the same units they would still not be the same thing.

 

[Chrisc]

JesseM, I have attempted to explain this from a number of different perspectives with the intent of helping you
to see the core concepts in question.
I can only assume your fixation with the literal interpretation of the equations has provided you with
a level of understanding beyond my comprehension.
Perhaps in another thread when I have more time to properly consider it, I will ask you to explain
your justifications for arguing the proper interpretation of energy.

Until then, and in order to see if you have an answer to my question, consider the collisions as having
any real properties of matter you see fit. (i.e. the production of heat, radiation, conservation of
kinetic energy, momentum, and frame dependency of all throughout the collisions)

From your previous posts as well as those of others, I will assume, and please correct me if I'm wrong,
that your explanation for the "time-reverse" mechanics that violate the laws of dynamics is as follows:
That all the kinetic energy of the constituent particles of the larger mass might be completely directed
to the acceleration of the smaller mass, thereby bringing the larger to rest, is so extremely improbable
that it has never been observed, but is not impossible and therefore does not violate the laws.
If this is correct, I can present the core concept in these terms.
If not, please explain how the smaller mass brings the larger to rest in the "time-reverse" version
without violating the laws.

 

[JesseM]

JesseM, I have attempted to explain this from a number of different perspectives with the intent of helping you
to see the core concepts in question.
I can only assume your fixation with the literal interpretation of the equations has provided you with
a level of understanding beyond my comprehension.
Perhaps in another thread when I have more time to properly consider it, I will ask you to explain
your justifications for arguing the proper interpretation of energy.

It's very basic physics that momentum and inertia are not forms of energy, that energy always has units of mass*distance^2/time^2, and that energy is always conserved. Feel free to ask any of the mentors on this forum and I'm sure they'll tell you the same thing.

Until then, and in order to see if you have an answer to my question, consider the collisions as having
any real properties of matter you see fit. (i.e. the production of heat, radiation, conservation of
kinetic energy, momentum, and frame dependency of all throughout the collisions)

If the linear kinetic energy is constant (an elastic collision), then the collision is just as possible in the time-reversed version as it is in the forward version. If the linear kinetic energy decreases, it must be because some of it was converted to light or heat, in which case thermodynamics explains why the time-reversed version is much less likely in our universe than the forward version, although there will always be some probability larger than zero of seeing it happen in reverse.

From your previous posts as well as those of others, I will assume, and please correct me if I'm wrong,
that your explanation for the "time-reverse" mechanics that violate the laws of dynamics is as follows:
That all the kinetic energy of the constituent particles of the larger mass might be completely directed
to the acceleration of the smaller mass, thereby bringing the larger to rest, is so extremely improbable
that it has never been observed, but is not impossible and therefore does not violate the laws.

Your comment about "bringing to rest" is much too vague. It is perfectly possible to have an elastic collision where a smaller mass brings a larger one to rest, and there would be no time asymmetry in this situation. It is only in the case of an inelastic collision, where linear kinetic energy changes before vs. after the collision, that thermodynamics becomes relevant, and the time-reversed version is more or less likely than the time-forward version.

For an example of an elastic collision where a larger mass is brought to rest, suppose we have two masses, the smaller with mass m and the larger with mass 2m, and the smaller is moving to the right at speed (1/3)*v, while the larger is moving to the left at speed (2/3)*v. After the collision, the smaller will be moving to the left at speed v, while the larger will have come to rest. Both before and after the collision, the total momentum of the system is mv to the left. And both before and after the collision, the total kinetic energy is (1/2)*mv^2. This is perfectly reasonable in the forward direction, and there would also be absolutely nothing about a reversed movie of this collision that would give away to a physicist that the movie was being played backwards.

 

[Dale]

Chrisc, here is one more attempt to get you to see that there is no asymmetry in the laws of dynamics in general.

Lets talk about two arbitrary point masses with arbitrary initial velocity that interact with each other through some force f.
<br /> \begin{array}{111}<br /> \text{1)} &amp; \text{equation:} &amp; f = m a = m x&#039;&#039;\\<br /> \text{2)} &amp; \text{forces:} &amp; f \text{ and } -f\\<br /> \text{3)} &amp; \text{masses:} &amp; m1 \text{ and } m2\\<br /> \text{4)} &amp; \text{initial position:} &amp; x1_0 \text{ and } x2_0\\<br /> \text{5)} &amp; \text{initial velocity:} &amp; v1_0 \text{ and } v2_0\\<br /> \end{array}<br />

So 1) is Newton's 2nd law and 2) is Newton's 3rd law. Together they comprise "the laws of dynamics" as you keep saying. And 3)-5) are the initial conditions. So, solving we get the equations of motion:

<br /> \begin{array}{11}<br /> \text{6)} &amp; x1(t) = x1_0 + v1_0 t + \frac{f}{2m} t^2\\<br /> \text{7)} &amp; x2(t) = x2_0 + v2_0 t - \frac{f}{2m} t^2\\<br /> \end{array}<br />

Now, let's see what happens under time reversal

<br /> \begin{array}{11}<br /> \text{8)} &amp; \tau = -t\\<br /> \text{9)} &amp; x1(\tau) = x1_0 - v1_0 \tau + \frac{f}{2m} \tau^2\\<br /> \text{10)} &amp; x1&#039;&#039; = f/m\\<br /> \text{11)} &amp; x2(\tau) = x2_0 - v2_0 \tau - \frac{f}{2m} \tau^2\\<br /> \text{12)} &amp; x2&#039;&#039; = -f/m\\<br /> \end{array}<br />

Note that 10) and 12) together are the same as 1) and 2), the laws of dynamics. Therefore the laws of dynamics are time-reverse symmetric. The masses and initial velocities were left arbitrary, as were the forces, so this applies for any interaction of any masses in any reference frame.

 

[Antenna Guy]

Now, let's see what happens under time reversal

<br /> \begin{array}{11}<br /> \text{8)} &amp; \tau = -t\\<br /> \text{9)} &amp; x1(\tau) = x1_0 - v1_0 \tau + \frac{f}{2m} \tau^2\\<br /> \text{10)} &amp; x1&#039;&#039; = f/m\\<br /> \text{11)} &amp; x2(\tau) = x2_0 - v2_0 \tau - \frac{f}{2m} \tau^2\\<br /> \text{12)} &amp; x2&#039;&#039; = -f/m\\<br /> \end{array}<br />

Note that 10) and 12) together are the same as 1) and 2), the laws of dynamics. Therefore the laws of dynamics are time-reverse symmetric. The masses and initial velocities were left arbitrary, as were the forces, so this applies for any interaction of any masses in any reference frame.

Shouldn't f change sign under time reversal?

Regards,

Bill