Definition(s) of "reversible" -- thermodynamics vs mechanical?

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SUMMARY

The discussion centers on the definitions of "reversible process" in mechanical systems versus thermodynamics. It establishes that while thermodynamic reversibility focuses on equilibrium states and material properties, mechanical reversibility is often simplified to the absence of friction. The conversation also highlights the theoretical nature of reversibility in mechanical processes, suggesting that a block sliding on a frictionless plane can conceptually reverse its path, but this does not align with thermodynamic principles. Additionally, it touches on the complexities of entropy measurement in both contexts, referencing Rolf Landauer's principle regarding computational reversibility.

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  • Understanding of thermodynamic principles, specifically "reversible process" and "equilibrium states."
  • Familiarity with mechanical systems and concepts of friction and motion.
  • Knowledge of entropy, including thermodynamic and Shannon's measures.
  • Basic principles of reversible computing and Landauer's principle.
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  • Research the implications of Landauer's principle in computational theory.
  • Explore the distinctions between thermodynamic and mechanical definitions of reversibility.
  • Study the role of entropy in both thermodynamics and information theory.
  • Investigate the concept of equilibrium in mechanical systems versus thermal equilibrium.
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Is there a definition for "reversible process" that applies to mechanical systems (such as a block sliding down a frictionless inclined plane) that is distinct from the definition of "reversible process" in thermodynamics?

If we apply the thermodynamic definition of "reversible process" to the situation of the block sliding down a frictionless inclined plane (and make the tacit assumption that the material of the block and the material in the plane are in thermal equilibrium) then the fact that block is moving with respect to the plane is irrelevant since we are only considering thermodynamic properties of the materials and no heat is being generated.

The definition of "reversible" process for mechanical systems is often ineffectively explained merely by saying that, in real life situations, mechanical processes are irreversible due to friction. This invites the reader to formulate a "default" definition for a "reversible" mechanical process and to define it as a process where there is no friction. That, in turn, would be consistent with the thermodynamic definition, which focuses on the properties of the materials that make up the mechanical system, not their motion with respect to each other.

However, there is a vague intuitive notion of reversibility for mechanical processes that says the process is reversible if it could go "backwards" in time. For a block sliding down a frictionless inclined plane we could imagine an (equally theoretical) structure consisting of a second frictionless upward sloping plane so the block would run up the upward slope, slide back down and replay its journey on the first inclined plane backward in time. However, unlike the thermodynamic definition of "reversible process" the block's path back to its initial state would not be taking a path through equilibrium states.
 
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To the best of my knowledge, these two concepts of reversibility are the same. It is also the same basic concept used in reversible computing (i.e., deleting information is related to creation of entropy).
 
DrClaude said:
To the best of my knowledge, these two concepts of reversibility are the same.
How disappointing! However, I've found nothing on the web to contradict that. At least there is a concept of "equilibrium" ("no unbalanced forces") that is defined for mechanical systems and is a different concept than thermal equilibrium.

It is also the same basic concept used in reversible computing

If I happen upon a block with mass 1 kg sliding along a frictionless horizontal surface at a velocity of 8 m/sec, can I compute what its state was 15 seconds ago? For example, do I necessarily know that it got its velocity from sliding down an inclined plane 7 seconds ago ? - and how would adding a little friction change the problem of predicting the past ?

The analysis of such situations depends on how we define the state variables of the process. However, at first glance, the conditions for "reversibility" in "reverse computing" seem to be much more demanding than thermodynamic reversibility.

Expositions of topics that mention "entropy" are often too glib because they don't specify how entropy is to be measured. If "entropy" refers to thermodynamic entropy then we lack any standard definition for the "entropy" of a state that is not in thermodynamic equilibrium. If "entropy" refers to Shannon's measure of information, we need to have a probability distribution defined.

The Wikipedia article you linked says:
As was first argued by Rolf Landauer of IBM,[4] in order for a computational process to be physically reversible, it must also be logically reversible. Landauer's principle is the rigorously valid observation that the oblivious erasure of n bits of known information must always incur a cost of nkT ln(2) in thermodynamic entropy.

I very curious about the claimed "rigorously valid observation". Is it an observed fact or is it a mathematical deduction from a series of definitions that make the "observation" true-by-definition?
 

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