Problem on limits from chemistry

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    Chemistry Limits
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Discussion Overview

The discussion revolves around a calculus problem related to Gibbs Free Energy and the implications of using an infinitesimal positive quantity, denoted as epsilon, in the context of thermodynamics. Participants explore whether it can be proven that ΔG ≤ 0 given the inequality ΔG + εΔS < 0, where the sign of ΔS is unknown.

Discussion Character

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

Main Points Raised

  • One participant proposes that if ΔG > 0, then ε can be chosen such that ΔG + εΔS = 0, leading to a contradiction if ΔS is non-negative.
  • Another participant questions the existence of an infinitesimal ε in the real numbers, suggesting it may imply a hyperreal context.
  • Some participants express uncertainty about the implications of treating ε as an infinitesimal, with one suggesting it can be neglected, leading to ΔG < 0.
  • A later reply outlines two cases based on the sign of ΔS, arguing that both cases lead to the conclusion that ΔG must be negative if ε is sufficiently small.
  • Participants discuss the informal use of infinitesimals in scientific calculations without rigorous foundations, referencing techniques in calculus and thermodynamics.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of ε or the validity of the original proof. There are competing views on the treatment of infinitesimals and the conclusions that can be drawn from the inequalities presented.

Contextual Notes

Some participants note that the treatment of ε as an infinitesimal raises questions about its mathematical foundation and applicability in the context of real numbers versus hyperreals. There is also a concern about the accuracy of the original inequality stated in the problem.

Bipolarity
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I've been doing some chemistry, and come up with a confusing problem that I can't seem to solve. It's a problem I made up while trying to understand the Gibbs Free Energy, but I will try to phrase it solely as a calculus question.

It is known that

\Delta G + \epsilon \Delta S &lt; 0 and that \epsilon is an infinitely small positive quantity. Nothing is known about the sign of \Delta S.

Both \Delta G and \Delta S are finite.

Can I prove that \Delta G ≤ 0 ?

I appreciate all help on this matter. Thanks!

BiP
 
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By infinitely small do you mean that \epsilon can be made as small as we desire? If so:

Suppose that \Delta G &gt; 0. Then we can find \epsilon &gt; 0 such that \Delta G + \epsilon \Delta S = 0, namely \epsilon = -\Delta G/\Delta S

Well, this is positive as long as \Delta S is negative . What if \Delta S \geq 0? In that case, \epsilon \Delta S \geq 0 so if \Delta G &gt; 0 we're just adding positive numbers together and of course it can't be negative
 
Office_Shredder said:
By infinitely small do you mean that \epsilon can be made as small as we desire? If so:

Suppose that \Delta G &gt; 0. Then we can find \epsilon &gt; 0 such that \Delta G + \epsilon \Delta S = 0, namely \epsilon = -\Delta G/\Delta S

Well, this is positive as long as \Delta S is negative . What if \Delta S \geq 0? In that case, \epsilon \Delta S \geq 0 so if \Delta G &gt; 0 we're just adding positive numbers together and of course it can't be negative

By infinitely small, I mean that \epsilon &gt; 0 is less than any positive real number.

BiP
 
Bipolarity said:
By infinitely small, I mean that \epsilon &gt; 0 is less than any positive real number.

BiP

No such epsilon exists in the real numbers (how can \epsilon/2 &gt; \epsilon)? Is this supposed to be a problem in the hyperreals or something?
 
Hmm well I don't know to say it, all I mean is that \epsilon is a positive infinitesimal.

I reasoned that because of its being infinitesimal it can be neglected from the equation, yielding \Delta G &lt; 0. But I don't know if that's correct.

Also your original proof does not satisfy the main constraint of the problem, i.e. \Delta G - \epsilon \Delta S &lt; 0

But I think we're getting somewhere! Thanks!BiP
 
Bipolarity said:
Hmm well I don't know to say it, all I mean is that \epsilon is a positive infinitesimal.

I reasoned that because of its being infinitesimal it can be neglected from the equation, yielding \Delta G &lt; 0. But I don't know if that's correct.

Can you describe a bit the setup that led you to this equation? It will help sort out exactly what kind of requirements you really have on \epsilon - since if you know it's smaller than all positive numbers, and non-negative for example, then \epsilon=0 necessarily.
Also your original proof does not satisfy the main constraint of the problem, i.e. \Delta G - \epsilon \Delta S &lt; 0

This differs by a minus sign from the original post
 
Office_Shredder said:
Can you describe a bit the setup that led you to this equation? It will help sort out exactly what kind of requirements you really have on \epsilon - since if you know it's smaller than all positive numbers, and non-negative for example, then \epsilon=0 necessarily.This differs by a minus sign from the original post

Sorry I meant \Delta G + \epsilon \Delta S from the original post. The second post is a typo.

The setup for my problem is a little complicated thermodynamics. I don't wish to go into it, but the epsilon is basically the infinitesimal difference in temperature between two reservoirs that are basically the same temperature, except one is higher in temperature by an infinitesimal amount epsilon. Heat will transfer due to that infinitesimal difference. Though the heat transfer is also infinitesimal, it is important in the calculations, whereas the epsilon reduces to the inequality above. I would love to see this problem be solved, seeing as it has been reduced to a purely mathematical problem.

I thank you for your time and efforts, they have made me rethink infinitesimals.

BiP
 
It sounds like you really want to assume that epsilon is an arbitrarily small positive number (i.e. small enough that only first order effects occur). In this case the solution in my previous post essentially does it for us. There are two cases

1) \Delta S \geq 0. Then \epsilon \Delta S \geq 0 as well, and if \Delta G \geq 0 adding these two inequalities yields \Delta G + \epsilon \Delta S \geq 0 which we know isn't true. So it must be \Delta G &lt; 0

2) \Delta S &lt; 0. We will do a proof by contradiction: suppose that \Delta G &gt; 0. Then we will show that if \epsilon is small enough (smaller than a specific number which we will calculate), that \Delta G + \epsilon \Delta S &gt; 0 which is a contradiction.

If \epsilon &lt; -\Delta G / \Delta S (which is a positive number since by assumption, delta S is negative and delta G is positive), then \Delta G + \epsilon \Delta S &gt; \Delta G + (-\Delta G / \Delta S) \Delta S where the inequality is > because we're increasing the coefficient of delta S, which is a negative number by assumption. Of course, cancelling the fractions then gives us \Delta G + \epsilon \Delta S &gt; \Delta G - \Delta G = 0 which is a contradiction.Note that in this case we had to assume delta G was non-zero, otherwise epsilon would have been exactly zero. But if delta G is exactly zero there's nothing to prove.

So we had two cases: one where delta S was non-negative, and one where delta S was negative. In both cases we proved that delta G must be negative, as long as we can assume epsilon is small enough.
 
Great! Thanks! I guess I must've just not understood your original solution, but I get this one!

BiP
 
  • #10
Office_Shredder, all the time in the sciences like physics and chemistry, we do calculus involving infinitesimals. This can of course be put on a firm rigorous foundation in any number of ways, including hyperreals and differential forms, but we often just use techniques without always referring to their foundations. Just like you take limits all the time without writing out the epsilon-delta definition, we can write things like dA=rdrdθ without writing out the definition of the wedge product or proving Jacobi's theorem. In thermodynamics, things like δW=-PδV is often more useful for our purposes than taking an explicit derivatives, but we don't lay out the theory of inexact differentials in our calculations.
 

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