Contradiction/breach 2nd law? Simply with carnot engine + negative temperature

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The discussion centers on the concept of negative temperatures in the context of reversible heat engines and the second law of thermodynamics. It explains that for a reversible heat engine operating between two temperatures, the heat ratio is defined by the temperatures, with heat flowing from a higher to a lower temperature. When considering ideal paramagnets at negative temperatures, the behavior contradicts conventional expectations, as heat flows from the negative to the positive temperature, suggesting that negative temperatures can be "hotter" than positive ones. Participants debate the implications of this phenomenon on the second law of thermodynamics, questioning whether traditional equations still apply and how work is involved in these scenarios. The conversation highlights the complexities and potential misunderstandings surrounding the application of thermodynamic principles to systems with negative temperatures.
  • #61
The main problem that I see is that a system at negative temperature is not in an equilibrium state- one can't use such a metastable state as a thermal reservior. Energy must constantly be supplied to keep the system in its metastable state.

Heat engines can operate via latent heat rather than specific heat (i.e. phase changes), but I don't see how to apply metastable systems as reservoirs.

Of course, the whole notion of allowing a thermodynamic negative temperature (as opposed to a statistical notion of 'effective temperature') is flawed.
 
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  • #62
Andy Resnick said:
Of course, the whole notion of allowing a thermodynamic negative temperature (as opposed to a statistical notion of 'effective temperature') is flawed.

Agreed.
 
  • #63
Andy Resnick said:
Of course, the whole notion of allowing a thermodynamic negative temperature (as opposed to a statistical notion of 'effective temperature') is flawed.

Agreed also.

I believe it's what myself and Drakkith have been getting at from the start!
 
  • #64
jarednjames said:
Agreed also.

I believe it's what myself and Drakkith have been getting at from the start!

That, and i was trying to explain how i thought the error with the equation could be resolved by converting the negative temp to a positive number.
 
  • #65
Hello Andy Resnick,

Hm, in what way do you mean "a semistable state"? I don't know what you mean.

And as for the negative temperature: is you calling it "flawed" expression of a personal preference or something objective?

Thank you.
 
  • #66
Drakkith said:
That, and i was trying to explain how i thought the error with the equation could be resolved by converting the negative temp to a positive number.

Of course, again I agree.
 
  • #67
Andy Resnick said:
Of course, the whole notion of allowing a thermodynamic negative temperature (as opposed to a statistical notion of 'effective temperature') is flawed.
Some time ago, in a long discussion people showed you that negative temperature is a perfectly valid equilibirum state and you agreed in the end.
All you need is a system or two whose state energy is bound. Then you put in so much energy as to almost saturate the energy capacity. In such a case the temperature of both systems is negative. Right?
 
  • #68
Andy Resnick said:
The main problem that I see is that a system at negative temperature is not in an equilibrium state- one can't use such a metastable state as a thermal reservior. Energy must constantly be supplied to keep the system in its metastable state.
This is not correct. A system at negative temperature is not in equilibrium with any system at positive temperature, but it can certainly be in equilibrium with another system at negative temperature. In such a situation energy does not need to be constantly supplied.

Andy Resnick said:
Of course, the whole notion of allowing a thermodynamic negative temperature (as opposed to a statistical notion of 'effective temperature') is flawed.
Careful here. This sounds like you (and Drakkith) are promoting personal theories. The idea of negative temperatures is a result of the standard statistical mechanics definition of temperature. I don't know what your "effective temperature" definition is, but Drakkith's idea is not only a personal theory but an untenable one. Temperature is a state variable, and by definition state variables depend only on the state of the system, not on the state of other systems.

Andy, Drakkith, and jarednjames, your objections to studying this are not relevant. The OP's question is based on mainstream physics, simply applied to an unusual but physically realizable system. Should we also not discuss Bose-Einstein condensates simply because they are also unusual? None of your objections are rational objections based on mainstream physics, only personal discomfort with the standard idea of negative temperature.
 
  • #69
DaleSpam said:
This is not correct. A system at negative temperature is not in equilibrium with any system at positive temperature, but it can certainly be in equilibrium with another system at negative temperature. In such a situation energy does not need to be constantly supplied.

Careful here. This sounds like you (and Drakkith) are promoting personal theories. The idea of negative temperatures is a result of the standard statistical mechanics definition of temperature. I don't know what your "effective temperature" definition is, but Drakkith's idea is not only a personal theory but an untenable one. Temperature is a state variable, and by definition state variables depend only on the state of the system, not on the state of other systems.

Andy, Drakkith, and jarednjames, your objections to studying this are not relevant. The OP's question is based on mainstream physics, simply applied to an unusual but physically realizable system. Should we also not discuss Bose-Einstein condensates simply because they are also unusual? None of your objections are rational objections based on mainstream physics, only personal discomfort with the standard idea of negative temperature.

My statements are as relevant as trying to use a negative temperature in the equations of a carnot cycle. Not only that, i was trying to explain a way to resolve the problems that others were running into with that equation. Instead of ANYONE explaining to me why my explanations were not valid, all i have received is personal scorn and ridicule. I readily asked for feedback telling me why i was incorrect, yet i have still not received any other than "Your wrong".

Nowhere in this thread have I tried to come up with personal theories or told anyone that they shouldn't study this effect. I see the whole thread as a big misunderstanding of physics and have attempted to explain that. I'm only sorry so few of you can see that.

Now, i ask again, someone EXPLAIN how i was wrong anywhere in this thread in my thinking.
 
  • #70
Drakkith said:
Instead of ANYONE explaining to me why my explanations were not valid, all i have received is personal scorn and ridicule. I readily asked for feedback telling me why i was incorrect, yet i have still not received any other than "Your wrong".
People have given examples where a negative temperature can occur. It's not our fault if you skip reading these paragraphs.

EDIT: I myself actually skipped one argument you gave. Here is the answer: you cannot simple convert negativ temperature to positive, because temperature is defined by T=dE/dS. The signs of dE and dS are well defined.
 
  • #71
Gerenuk said:
People have given examples where a negative temperature can occur. It's not our fault if you skip reading these paragraphs.

EDIT: I myself actually skipped one argument you gave. Here is the answer: you cannot simple convert negativ temperature to positive, because temperature is defined by T=dE/dS. The signs of dE and dS are well defined.

I understand perfectly what everyone is saying and nowhere will i say that you CANNOT have a negative temp. The negative temp is only applicable in a specific situation where you have a finite number of states.

Anyways, if you know the amount of energy that would be transferred from a negative temp, then why couldn't you convert that into a positive temperature in relation to the positive system? I definitely don't know the math behind all this, but I am fairly sure this wouldn't be impossible to do.
 
  • #72
Because temperature is defined by T=dE/dS. And all equations are based on this identity. You cannot arbitrarily introduce a minus sign there. Or at least it wouldn't make sense, because you had to rewrite all the other thermodynamics equation and thus going back to negative temperature.
 
  • #73
Gerenuk said:
Because temperature is defined by T=dE/dS. And all equations are based on this identity. You cannot arbitrarily introduce a minus sign there. Or at least it wouldn't make sense, because you had to rewrite all the other thermodynamics equation and thus going back to negative temperature.

In regards to the first post.

If -273 is Colder than -200, then you need to switch your T1 and T2 around.

For example. If t1=200 and T2 = 273, then its 200/273. The cooler temp is on the top.

Now, if T1 = -273 and T2 = -200, then its -273/-200. The energy in the system would flow from 2 to 1 because there is more energy in T2 than in T1, just like in the 1st example up top.

Is this correct?
 
  • #74
Now, let's say that T1 = 200 and T2 = -200. If we know the amount of energy that -200 would transfer into T1, then we can say that T2 is actually equal to a positive temp that is greater than T1. For the purposes of this argument let's say that if the two temps were equalized, T2 would introduce as much energy into T1 as a temperature of 300k would.

So, instead of 200/-200, its actually 200/300.

Even though a negative temp has more heat than any positive temperature, it still has a finite amount of energy that it can transfer to a lower temperature.

Does this make sense?

Edit: I'm not changing the actual temperature of T2 here, but merely converting it to a positive number that will work in the equation. In this case, T still equals dE/dS.
 
  • #75
Drakkith said:
Instead of ANYONE explaining to me why my explanations were not valid, all i have received is personal scorn and ridicule.
This is completely unsubstantiated. I have not once made any personal attack on you, have tried to teach the concepts involved, and have three times given different explanations of problems with your idea:

DaleSpam said:
Temperature is a state variable, and by definition state variables depend only on the state of the system, not on the state of other systems.

DaleSpam said:
You can arbitrarily define your system boundaries depending on what behavior you are interested in studying. There is no requirement that you compose your system such that there is always an infinite number of modes.

DaleSpam said:
It doesn't matter what kind of mode the energy is in. As long as you have a system with some limited number of possible modes then you can get negative temperatures.

In light of the above your assertion that you have not received any explanation and instead have received scorn is absurd. I have tried throughout this thread to both address the OP's question and to teach you and others about some interesting mainstream physics. I don't know what more I could possibly do, and your accusation here is both personally upsetting and factually unwarranted.
 
  • #76
mr. vodka said:
Hello Andy Resnick,

Hm, in what way do you mean "a semistable state"? I don't know what you mean.


Thank you.

I said 'metastable'- a system assigned a negative temperature can only remain in that state if it does not interact with anything else, or energy is supplied to the system to maintain it in that state.
 
  • #77
Gerenuk said:
Some time ago, in a long discussion people showed you that negative temperature is a perfectly valid equilibirum state and you agreed in the end.
All you need is a system or two whose state energy is bound. Then you put in so much energy as to almost saturate the energy capacity. In such a case the temperature of both systems is negative. Right?

Honestly, I don't recall- can you locate the thread? I'm not saying you are wrong.
 
  • #78
Dale, you haven't understood AT ALL what any of my posts have been getting at have you? Granted I probably haven't used the 100% correct terminology, but its not that hard to understand.

In following with the title of this thread, a negative temperature would ONLY relate to the spin states of a system. Since the carnot cycle DOES NOT use spin states as a way to get work, then the negative temperature doesn't matter.

You guys decided to get off topic and when I stuck to it and tried to claim that the carnot cycle wouldn't work in this circumstance under real world physics then everyone has a freakin aneurysm. I thought we stuck to mainstream science here, not wishful thinking. Because that's about all this is right now. We "MIGHT" be able to get an engine using the carnot cycle to use the spin states at some point in the future, but not right now.

Edit: Also, <br /> \Delta S = \int \frac{dQ}{T}<br /> must use a positive number for a temperature.
 
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  • #79
Drakkith said:
a negative temperature would ONLY relate to the spin states of a system.
This is incorrect and has already been addressed multiple times:

DaleSpam said:
It doesn't matter what kind of mode the energy is in. As long as you have a system with some limited number of possible modes then you can get negative temperatures. The spin states is just one nice example.
Gerenuk said:
Just any system where the maximum energy does not get infinite, can have negative temperature.

DaleSpam said:
You can arbitrarily define your system boundaries depending on what behavior you are interested in studying. There is no requirement that you compose your system such that there is always an infinite number of modes. And, in fact, in many QM systems you do have a limited number of modes. Statistical mechanics and negative temperature can become important for analyzing such systems.


Drakkith said:
Edit: Also, <br /> \Delta S = \int \frac{dQ}{T}<br /> must use a positive number for a temperature.
No, if S decreases for an increase in Q then T must be negative. That is the whole point.
 
  • #80
DaleSpam said:
Careful here. This sounds like you (and Drakkith) are promoting personal theories.

I can't speak for Drakkith, but:

http://prola.aps.org/pdf/PR/v104/i3/p589_1

Has a very cogent discussion (with additional references) spelling out the needed condition to establish a system with negative temperatures. None of these criteria have been part of the OP's thought experiment, nor the subsequent "analysis".

DaleSpam said:
Should we also not discuss Bose-Einstein condensates simply because they are also unusual? None of your objections are rational objections based on mainstream physics, only personal discomfort with the standard idea of negative temperature.

Sigh... The OP is proposing using *reservoirs* at negative temperatures to drive a heat engine. He did not propose the *existence* of a system at negative temperature. In fact, my objection was very clearly stated as such. Before claiming I am not making a rational objection, perhaps you could put forth a reference supporting your belief that a *thermal reservior* at negative temperatures is mainstream physics?
 
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  • #81
DaleSpam said:
This is incorrect and has already been addressed multiple times:

No, if S decreases for an increase in Q then T must be negative. That is the whole point.

No, it isn't incorrect. I'm using real world science applicable to this thread. I don't know what your using. I know that negative temp is in any systems with a finite number of states. We don't have any systems like that other than spin states currently though.

Its obvious to me that you are unwilling or unable to understand my posts, and you really havnt even addressed them other than to point out some made up inaccuracies that you think i have in them because you don't understand what I am getting at. I'm done talking to a brick wall for the now. Goodnight all.
 
  • #82
Andy Resnick said:
I can't speak for Drakkith, but:

http://prola.aps.org/pdf/PR/v104/i3/p589_1

Has a very cogent discussion (with additional references) spelling out the needed condition to establish a system with negative temperatures. None of these criteria have been part of the OP's thought experiment, nor the subsequent "analysis".
I can't access the link, I would be very interested.

Andy Resnick said:
Sigh... The OP is proposing using *reservoirs* at negative temperatures to drive a heat engine. He did not propose the *existence* of a system at negative temperature. In fact, my objection was very clearly stated as such. Before claiming I am not making a rational objection, perhaps you could put forth a reference supporting your belief that a *thermal reservior* at negative temperatures is mainstream physics?
AFAIK there is no real definition of what constitutes a "thermal reservoir". So I would have a hard time excluding a negative temperature system on that basis.

I don't think that the problem is in treating a negative temperature system as a reservoir, I think the problem is having a cycle in a negative temperature system. I don't know that such a system exists since I don't know enough negative temperature systems to know what other state variables they may have besides energy.
 
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  • #83
Drakkith said:
No, it isn't incorrect.
Yes, it is. Look at the formula.

If \Delta S is negative for a positive dQ then T is negative according to the formula you supplied. I don't know how you can reach any other conclusion.

Drakkith said:
I don't know what your using.
Basic statistical mechanics definitions.
 
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  • #84
Phew, quite the discussion.

Andy Resnick: you might be confused if you thought I was suggesting an actual gas as the engine? I was assuming the system doing work itself could also have negative temperature. DaleSpam pointed out the problem might be in the actual finding of a system that could function as such a negative temperature engine, so we'd agree with you if you were to object that we can't just postulate an engine doing work on negative temperature. But your objections might lay elsewhere, but I'm not sure where: negative temperature seems to do its work just fine and has a logical definition, so I don't know why one would object. Of course the idea can be odd, since what we're saying is basically that if you'd throw an ideal paramagnet in the sun, the paramagnet would heat the sun up, but of course on that level our assumptions (that we can isolate certain modes) fall down, but this doesn't mean we can't explore it theoretically, and that if the theory tells us it's feasible, I'm sure we can find certain conditions where it can be actually construed. On a side-note: I'm not actually expecting to find a breach in the 2nd law, just finding the flaw in this situation.

DaleSpam, what about magnetic work! I got the idea of http://www.phys.uri.edu/~gerhard/PHY525/wtex4.pdf (but they seem to have specifically stuck to positive temperature)
 
  • #85
I don't think there is any principal flaw in the system considered and I am not even too surprised that it requires work to thermalize the two systems reversibly.
However, take in mind that the working medium of the Carnot machine has also to be a system capable of assuming negative temperatures, e.g. a collection of spins in a magnetic field. Then it should be possible to visualize the process in a simple model. Work can be done by the medium by shifting the magnet generating the field. At negative temperatures, the material is diamagnetic, i.e. the working substance and the magnet repell. The repulsion is higher the more negative the temperature. Shifting the magnet while in contact with one of the reservoirs would constitute the isothermal part of the process. Changing the magnetic field with the inversion hold fixed the adiabatic part.
 
  • #86
This question must have been settled somewhere. In the 5th volume of Landau/Lifgarbagez (a 1979 German edition) there is a chapter on negative temperatures.
IIRC there is another system with negative temperatures: the population inversion needed in lasers and masers is also described by negative temperatures.
 
  • #87
DaleSpam said:
I can't access the link, I would be very interested.

I believe the article is now public domain- I have the pdf, but I can't figure out how to stick it here.


DaleSpam said:
AFAIK there is no real definition of what constitutes a "thermal reservoir".

You may claim these are "personal theories", but definitions can be found here:

Fermi, Thermodynamics, p.32
Sears and Salinger, Thermodynamics, Kinetic Theory, and Statistical thermodynamics, p.83
Halliday, Resnick,and Walker, Fundamentals of Physics, p438
Serway and Faughn, College Physics, p342
Tolman, Principles of Statistical Mechanics, p 556
Landau and Lifgarbagez, CTP, vol 5, pg 58
 
  • #88
mr. vodka said:
Phew, quite the discussion.

Andy Resnick: you might be confused if you thought I was suggesting an actual gas as the engine?

I am aware that you are trying to make a heat engine using Ramsey-type systems.
 
  • #89
Without reading Andy's resources, I was taught (in Thermo) that a heat reservoir was hot body such that

as you take sigmaQ (a small amount of heat compared to the total heat) from the reservoir to power your system, the reservoir's temperature stays the same.
 
  • #90
Couldn't find a definition in Fermi or Tolman on mentioned pages.
 

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