Entropy and Thermal Equilibrium: Solving the Hotter-Colder Object Conundrum

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Homework Help Overview

The discussion revolves around the concept of entropy and thermal equilibrium, specifically addressing a problem involving the interaction between a hotter object and a colder object when placed together in an isolated system. Participants are exploring the implications of the second law of thermodynamics and the behavior of entropy in this context.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the change in entropy and its relation to heat transfer between the two objects. There is an emphasis on understanding the conditions under which entropy increases and the implications of the second law of thermodynamics. Some participants suggest examining the equations related to entropy changes and the assumptions regarding heat flow.

Discussion Status

The discussion is active, with participants offering insights into the relationship between heat flow and entropy changes. There are multiple interpretations being explored regarding the behavior of the system and the mathematical relationships involved. Some guidance has been provided on how to approach the problem using the change in entropy.

Contextual Notes

Participants are working within the constraints of using only the information provided in the problem statement. There is a focus on ensuring that the discussion adheres to the principles of thermodynamics without making assumptions beyond the given context.

zeithief
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I stumbled across this question in one of the physics competition selection test but after thinking like 2 days i still can't figure out homework to solve it.
I've been introduced to the equation: entropy, S=Q/T where Q is the heat energy and T is the temperature.
Then I've been told that the entropy of a system always remains constant or increase.
Then the question is to show that when a hotter object and a colder object are put together and isolated the hotter object always becomes colder and colder becomes hotter. We are expected to solve this with the information provided only.
Help anyone ?? :biggrin: ?
 
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zeithief said:
I stumbled across this question in one of the physics competition selection test but after thinking like 2 days i still can't figure out homework to solve it.
I've been introduced to the equation: entropy, S=Q/T where Q is the heat energy and T is the temperature.
Then I've been told that the entropy of a system always remains constant or increase.
Then the question is to show that when a hotter object and a colder object are put together and isolated the hotter object always becomes colder and colder becomes hotter. We are expected to solve this with the information provided only.
As Cyrus says, you must look at the change in entropy, which according to the second law of Thermodynamics, must be greater than or equal to zero. Assume the flow of heat is from the colder to the hotter object and determine whether the change in entropy of the system is greater than zero. See if it fits with the second law.

The change entropy of the system is the sum of the entropy changes in each object. Use the convention: heat flow into an object is positive and heat flow out is negative. dS = dQ/T

AM
 
zeithief said:
Then the question is to show that when a hotter object and a colder object are put together and isolated the hotter object always becomes colder and colder becomes hotter. We are expected to solve this with the information provided only.
Help anyone ?? :biggrin: ?

We already know the equation delta S = delta Q(reversible) / T

Now we want to explain the way in which spontaneous processes occur using the entropy. Assume two spaces, one space has temperature T1 and the other T2 and we isolate this system.

The difference between the two entropies delta S at equilibrium is given by:

delta S = delta S(1) + delta S(2)

(total entropy change of the system is the sum of the two separate entropy changes)

Now we can write: delta S(1) = delta Q(reversible)(1) / T(1) and delta S(2) = delta Q(reversible)(2) / T2. Now because the system is isolated, Q(rev)1 = -Q(rev)2 (heat released by 1 must be taken up by 2). We say Q = Q(rev)1 = -Q(rev)2

delta S = Q(1/T1 - 1/T2)

Now we say that when T2 > T1 then delta S > 0 (spontaneous process) when Q > 0, so heat flows into system 1 . When T1 > T2, delta S > 0 when Q < 0 and thus heat flows into system 2.
 
Last edited:
we see microsopic and macroscopic entropy differnetly ..
microscopic is about statistical view of entropy?
what can we say about the boltz man equation of entropy
 
ashu_manoo12 said:
we see microsopic and macroscopic entropy differnetly ..
microscopic is about statistical view of entropy?
what can we say about the boltz man equation of entropy

you mean S = k * ln W :p
 

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