Does the Energy Transfer Diagram Challenge the Second Law of Thermodynamics?

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Homework Help Overview

The discussion revolves around a problem related to the Second Law of Thermodynamics, specifically examining an energy transfer diagram that raises questions about efficiency and entropy. Participants analyze the implications of energy conservation and the relationship between heat and work in thermodynamic systems.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants explore the relationship between the first and second laws of thermodynamics, questioning whether the scenario presented violates these laws. There is uncertainty regarding the representation of energy flow and efficiency in the context of the given diagram.

Discussion Status

Some participants have offered insights into why the first law is not violated, emphasizing energy conservation, while others assert that the second law is indeed violated due to the engine's efficiency exceeding that of a Carnot engine. Multiple interpretations of the problem are being explored, and there is an ongoing exchange of ideas without a clear consensus.

Contextual Notes

Participants are working with a past IB Physics exam question, which may impose specific constraints or assumptions that are under discussion. There is also mention of a potential misunderstanding regarding the representation of energy in the cold reservoir.

rubix1225
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Homework Statement


Here is the question:
http://img93.imageshack.us/img93/9159/snap1k.jpg

Homework Equations


First law: Q=W+U
Second law: no thermodynamic system can convert heat into work 100%; heat flows from hot to cold reservoirs spontaneously; entropy always increases


The Attempt at a Solution


From the diagram, it looks like energy is conserved 100% as the heat taken from the hot reservoir (100J) is split into 75J of work and 25J carried over to the cold reservoir. Does this mean that it violates the 2nd law of thermodynamics because no system can be 100% efficient? But then again, the 2nd law heat cannot be 100% converted into WORK, and not the whole system. I'm really stumped for the 2nd law of thermodynamics in this case.

I'm not even sure what the 25J actually represents (the energy going into the cold reservoir). Does it represent the change in internal energy (U from Q=W+U)? From here, I really became stuck as to how to explain the 1st law of thermodynamics.

The answer is given as C. Could someone kindly explain why the 1st is not violated but the 2nd law is? Thanks :smile:
By the way, this question is from a past IB Physics paper and my exam is next week! Any help would be vastly appreciated.
 
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Entropy decrease of hot reservoir = 100/400 J/K
Entropy increase of cold reservoir = 25/300 J/K

Net entropy has decreased!
 


The first law is not violated because the work done by the engine is less than the net heat flow into the engine. Energy is conserved. (in one cycle, \Delta U is 0, and \Delta Q = 100 - 25 = 75 = W).

The second law is violated for the reason given by Davieddy. You can see that the second law is violated because this engine is more efficient than a Carnot engine operating between these two temperatures. (for Carnot \eta = 1 - Tc/Th = .25, which is less than the efficiency here: W/Qh = .75). This is not possible by the second law.

AM
 


Andrew Mason said:
The first law is not violated because the work done by the engine is less than the net heat flow into the engine. Energy is conserved.

The second law is violated for the reason given by Davieddy.

I think you mean = rather than <.
THX for the "endorsement".

I taught an Andrew Mason at St Paul's School (London) around 1974,
and his whizz kid younger brother Lionel.

No relation I suppose?

David Eddy
 


davieddy said:
I think you mean = rather than <
I think I meant "not greater than".
I taught an Andrew Mason at St Paul's School (London) around 1974,
and his whizz kid younger brother Lionel.
Sorry, no relation. I was in London in 1974. But I don't have a younger brother Lionel - none that I know of anyway...

AM
 


Andrew Mason said:
I think I meant "not greater than".
Sorry, no relation. I was in London in 1974. But I don't have a younger brother Lionel - none that I know of anyway...

AM

I suppose you could argue that some heat could go somewhere other
than the "cold reservoir", otherwise energy would not be "conserved".

Since your name is not uncommon, it was a bit of a long shot.
Similarly London 1974 is not an unbelievable coincidence.
 


Ah nonetheless, that is still quite a coincidence.
Anyway thank you for the help David and Andrew, appreciate it :biggrin:
 


rubix1225 said:
Ah nonetheless, that is still quite a coincidence.
:biggrin:

I thought he might be in the same time zone (time of posting) and
he has an English (as distinct from US) sounding name, and he knows
something about physics.

London is quite a big city, and there are quite a lot of us "babyboomers" around.

My enquiry would not have arisen if I hadn't taught someone with the same name.
I would be mildly surprised if that AM had completely forgotten me
(or at least the school) though!

But I agree, it is a nice coincidence.

David
 
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