No entropy/environment = no time flow?

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Discussion Overview

The discussion explores the relationship between time flow and the presence of an environment in closed systems, focusing on the implications of the Schrödinger equation and the second law of thermodynamics. Participants examine whether time evolution can be meaningfully discussed in isolation and the nature of observers in this context.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Exploratory

Main Points Raised

  • Some participants propose that time evolution in a closed system may not make sense without an environment, suggesting that without it, systems remain in superposition and do not exhibit time flow.
  • Others argue that the Schrödinger equation governs time evolution and does not require an environment, asserting that internal dynamics exist even in closed systems.
  • There is a contention regarding the interpretation of the Schrödinger equation, with some stating it does not necessitate time flow, while others maintain that it implies evolution based on initial conditions and Hamiltonian.
  • Some participants suggest that without the second law of thermodynamics, each subsystem could have its own arrow of time, complicating macroscopic comparisons.
  • One viewpoint emphasizes the importance of the observer's interaction history with the system, arguing that expectations of time evolution are observer-dependent and cannot arise from isolated systems.
  • Another perspective challenges the notion of a closed system being scientifically relevant, as it cannot be observed or verified, leading to questions about the operational meaning of such systems.
  • Some participants discuss the implications of the quantum Zeno effect as an illustration of the observer's role in time evolution.

Areas of Agreement / Disagreement

Participants express multiple competing views on the relationship between time flow and closed systems, with no consensus reached on the necessity of an environment for time evolution or the implications of observer interactions.

Contextual Notes

Limitations include the unresolved nature of assumptions regarding the role of the observer, the definitions of closed systems, and the implications of the second law of thermodynamics on time flow.

  • #31
xepma said:
Magic? Have you ever seen a proper derivation of the 2nd law? It's just probability theory. Probability theory of really, really large numbers.

The 2nd law is perfectly fine. Just look around you -- you see it in action every day.

What I've seen is a few circular definitions. Namely probability defined in terms of probability. Time defined in terms of time. Somewhat murky entropy definitions. The arrow of time referring to the direction of the entropy increase. And of course the 2nd law using all these terms.

-- Dmtr
 
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  • #32
The alternative is that there is some asymmetry on the better defined quantum level and it shows up as the thermodynamic arrow of time on the macro scale.

-- Dmtr
 
  • #33
dmtr said:
What I've seen is a few circular definitions. Namely probability defined in terms of probability. Time defined in terms of time. Somewhat murky entropy definitions. The arrow of time referring to the direction of the entropy increase. And of course the 2nd law using all these terms.

-- Dmtr

I'm not sure if I make the right associations to your thinking here, and at what level you picture this, but if you have objections about the use of probability theory and the notion of entropy then I can just add that I have such objections as well.

It is completely true however, that there is no different in principle between QM and classical physics. That however doesn't mean it's more sound, it just means the same unsatisfactory reasoning is used in both places :) This is why the context of which I would want to raise this objection is in the "beyond the standard model" context.

I don't know if this is what Dmtr also means, or not?? but by objection is that from the point of view of (what I personally seek) an intrinsic measurement theory, entropy measures are not uniqe. There are as we know several different definitions of entropy measures. They can be "derived" in severals ways, from cox axioms, or from other considerations. My opinion is that it makes no sense to consider a universally objective information measure. This has been briefly discussed in several threads mainly in the BTSM I think.

There are also some threads here discussing the relatvivity of entropy.

I've question continuum probability theory itself, on the basis thta the continuum notion implies (IMHO at least) an infinitely massive observer - which I think, makes no sense except as an APPROXIMATION (where instead of actually using large numbers, you describe it as a "continuum" - this is fine in the limit, but care must then be taken when you "scale it back" to the small number limit).

/Fredrik
 
  • #34
Fra said:
I'm not sure if I make the right associations to your thinking here, and at what level you picture this, but if you have objections about the use of probability theory and the notion of entropy then I can just add that I have such objections as well.

It is completely true however, that there is no different in principle between QM and classical physics. That however doesn't mean it's more sound, it just means the same unsatisfactory reasoning is used in both places :) This is why the context of which I would want to raise this objection is in the "beyond the standard model" context.

I don't know if this is what Dmtr also means, or not?? but by objection is that from the point of view of (what I personally seek) an intrinsic measurement theory, entropy measures are not uniqe. There are as we know several different definitions of entropy measures. They can be "derived" in severals ways, from cox axioms, or from other considerations. My opinion is that it makes no sense to consider a universally objective information measure. This has been briefly discussed in several threads mainly in the BTSM I think.

I have no objections to the use of the probability theory, entropy, or the 2nd law. These are very good instruments. For instance in the QM we can calculate probabilities which very often agree with the experiments very well. And we would be very much surprised if suddenly they wouldn't.

What I don't like however is when these instruments are used to give the ultimate definition of the arrow of time. Use of the 2nd law to define the time arrow makes sense only in the classical approximation, where the 2nd law is defined. It hardly makes sense even there, because time/causality is an axiom in the classical approximation.

An alternative to that is to think of some properties of the quantum state space that would ultimately result in the 2nd law and the familiar time arrow in the classical approximation.

-- Dmtr
 

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