According to Thermodynamics Everything should Pop into Existence?

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Discussion Overview

The discussion revolves around the implications of thermodynamics, particularly the Gibbs free energy, in the context of spontaneous creation of matter in a system at constant temperature and pressure. Participants explore the mathematical relationships and assumptions underlying these concepts, questioning the validity of certain derivations and interpretations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant asserts that the Gibbs free energy, defined as G = U - TS + PV, is negative, suggesting that this implies spontaneous creation of matter under constant T and P.
  • Another participant challenges the interpretation of absolute free energy, arguing that it only has meaning in terms of changes, not absolute values.
  • A participant questions the assumption of constant energy when discussing changes in the amount of matter in a system, seeking clarification on how energy conservation is maintained.
  • Concerns are raised about the validity of replacing changes in entropy, volume, and internal energy with their absolute values in the derivation of Gibbs free energy.
  • One participant acknowledges a potential error in their reasoning regarding the relationship between entropy and Gibbs free energy, particularly under conditions of varying particle numbers.
  • Another participant emphasizes that the creation of matter must adhere to the principle of energy conservation, indicating a lack of clarity in the proposed system's adherence to this principle.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of Gibbs free energy and its implications for spontaneous processes. There is no consensus on the validity of the derivations presented, and several points remain contested, particularly regarding assumptions about energy conservation and the meaning of absolute free energy.

Contextual Notes

Participants highlight limitations in the assumptions made regarding constant energy and the treatment of changes in thermodynamic variables. The discussion reveals unresolved mathematical steps and the need for clearer definitions in the context of the proposed scenarios.

nonequilibrium
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(In the following discussion, when I use the word "always", I mean "as good as always" if you're willing to ignore exotic systems with negative temperature and such)

In the following discussion I will assume we're working in a heat bath with constant T and P:

So there are several ways to see the total Gibbs free energy of an object, defined G = U - TS + PV, is negative.

Two simple ways:
(*) Chemical potential is defined as [tex]\mu = -T \left( \frac{dS}{dN} \right)_{U,V}[/tex] and thus is always negative. We also can prove [tex]G = \mu N[/tex].

(*) We know [tex]T \Delta S \geq Q = Q + P \Delta V - P \Delta V \geq Q + P \Delta V + W = \Delta U + P \Delta V[/tex] so [tex]TS \geq U + PV[/tex] or [tex]G \leq 0[/tex].

So now the problem is, when we 'make something' its G function goes from zero to something negative (as was just shown in two ways). This implies it should happen spontaneously, since in constant T and P the second law becomes "G goes to a minimum".

So does this say things should randomly pop into existence? Obviously there is a thinking error?
 
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Like potential energy, the only meaning free energy has is in terms of *changes* (dG vs. G). Changes can be positive or negative. I'm not sure the (absolute) free energy has any meaning.

Sometimes (especially in biochemistry), you will enounter notation like [itex]\Delta \Delta G[/itex], which corresponds to changes to [itex]\Delta G[/itex].
 
Well, that's what I used, didn't I? First G = 0 and then G is negative, so the net change is negative (well the basic principle is that G goes down when something is created, check my math above)
 
mr. vodka said:
(*) Chemical potential is defined as [tex]\mu = -T \left( \frac{dS}{dN} \right)_{U,V}[/tex] and thus is always negative. We also can prove [tex]G = \mu N[/tex].

Here you are assuming constant energy. How do you propose to change the amount of matter in a system without changing the total energy?

mr. vodka said:
(*) We know [tex]T \Delta S \geq Q = Q + P \Delta V - P \Delta V \geq Q + P \Delta V + W = \Delta U + P \Delta V[/tex] so [tex]TS \geq U + PV[/tex] or [tex]G \leq 0[/tex].

How do you justify replacing [itex]\Delta S[/itex], [itex]\Delta V[/itex], and [itex]\Delta U[/itex] with S, V, and U? I don't see how that's valid.
 
Okay, drop my first "derivation" then.

About the second: well, if I create the whole system, V_i = 0 and V_f = V, same for S and U, don't you agree?

EDIT: Btw thanks for the critique, I hope to discover my error before my exam in the morning, it's quite troubling I can't see where my reasoning goes astray
 
As with the first derivation, I'm not seeing how this hypothesized system obeys energy conservation.
 
Everything enters as heat from the environment (that's the meaning of -TS in the definition of G, right? And in this case: TS > U + PV (as shown in the 2nd derivation)

But I've come to the conclusion "dS_tot > 0 <=> dG < 0" under constant P and T is only an equivalence if the system has a constant amount of particles! That's probably where I made my error. (G is still < 0, but now it just doesn't matter, really)
 

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