What is the reason for absolute zero temperature?

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Discussion Overview

The discussion centers on the concept of absolute zero temperature and the reasoning behind its existence as the lowest thermodynamic temperature. Participants explore the relationship between temperature and entropy, historical perspectives on their definitions, and the implications of negative temperatures.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants question the empirical reasoning behind the assumption of absolute zero, seeking a non-entropy-based argument for why positive temperatures exist.
  • Others assert that entropy is more fundamental than temperature, suggesting that temperature may be a derived concept.
  • A participant argues that historically, temperature was defined before entropy, raising the need for a non-statistical argument for positive temperature.
  • One participant states that temperature is a measure of the motion of matter, implying that zero motion corresponds to zero temperature.
  • Another participant challenges the notion that temperature must be tied to motion, presenting hypothetical systems that could have temperature without motion.
  • Some participants introduce the concept of negative temperatures, discussing their implications and how they differ from traditional definitions of temperature.
  • There is mention of the Carnot engine as a basis for deriving temperature in classical thermodynamics.
  • One participant emphasizes that while entropy may be fundamental, it cannot be measured directly, unlike temperature.
  • Another participant notes that temperature is often defined in relation to thermal equilibrium between objects.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between temperature and entropy, the definition of absolute zero, and the implications of negative temperatures. The discussion remains unresolved with no consensus reached.

Contextual Notes

Participants highlight limitations in definitions and the historical context of temperature and entropy, noting that some arguments may depend on specific interpretations or assumptions about thermodynamic systems.

Jano L.
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What is the empiric reason behind the assumption that there is lowest thermodynamic temperature (absolute zero)? And that all other temperatures of bodies in thermodynamic equilibrium are always higher ?

I am looking for a reason not using the entropy concept, as the entropy was derived historically with the assumption that there is lowest temperature which ideal gas can have. So the argument using entropy would be circular.

Or do you think that entropy is more fundamental than temperature and positive thermodynamic temperature is a just a consequence the properties of entropy ?
 
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Jano L. said:
Or do you think that entropy is more fundamental than temperature and positive thermodynamic temperature is a just a consequence the properties of entropy ?
This. Entropy is far more fundamental than temperature.
 
I know such view is quite common, but if I want to avoid statistical physics, it is hard to introduce entropy first and then temperature as a derived concept. Historically, the temperature is assumed first and the entropy is derived, by the consideration of Carnot cycles - this is the way entropy was discovered. So I wonder whether there is some non-statistical, non-entropic argument for the positive temperature, which would make the historical path more sensible.
 
I guess I don't even understand your question. Temperature is a measure of the motion of matter. If there is no motion, the temperature is zero. What's confusing about that?
 
Jano L. said:
I know such view is quite common, but if I want to avoid statistical physics, it is hard to introduce entropy first and then temperature as a derived concept. Historically, the temperature is assumed first and the entropy is derived, by the consideration of Carnot cycles - this is the way entropy was discovered. So I wonder whether there is some non-statistical, non-entropic argument for the positive temperature, which would make the historical path more sensible.
That may of been the order the phenomena were discovered but that doesn't change the fact that entropy is more fundamental to nature. Newtons laws may of been discovered before QM, but QM is still more fundamental, for example.
 
If there is no motion, the temperature is zero. What's confusing about that?

Well, I do not necessarily want to use the idea that temperature is direct measure of motion. It is conceivable that one has a system that has temperature and no motion - take model of two state spins for example, which can have energy and entropy but no motion. Or take ideal fluid defined by the equation of state

$$
pV = nRT
$$

and total energy

$$
U = ncT.
$$

with some constant ##c##. According to the second equation, temperature is a measure of total energy ##U##. But energy is an abstract concept, which can be negative in principle. (It will be other contributions to energy are negative and great enough). Then according to the second equation, the temperature will be negative too.
 
Curl said:
Also 0 is not the lowest possible temperature:
http://en.wikipedia.org/wiki/Negative_temperature
In a sense, it still is though if one uses the more fundamental β= 1/T. Then temperature flows from low to high β and negative temperature corresponds to hotter than anything.
 
Curl,
I know of " negative temperatures" as sometimes applied to spins and laser, but those are different thing from what I have in mind. As wikipedia says,
By contrast, a system with a truly negative temperature in absolute terms on the Kelvin scale is hotter than any system with a positive temperature.
Such temperatures do not have the standard meaning of temperature, which is that heat flows from body with higher to body with lower temperature. When you connect such spin system with -5 K to 5 K system, the -5 K system has more energy and will give it to the system with 5 K. Such concept of temperature defines negative temperatures to conform to the laws of entropy.

But this is not without objection - such systems are not stable so it can be argued they do not have temperature at all.

I am thinking of a concept of temperature applied only to systems in equilibrium, with which, when a body has temperature -5 K, one says the body is truly colder than the system with 0 K, so heat will flow from 0 K to -5 K.
 
  • #10
Entropy may be more fundamental than temperature, but it cannot be measured directly, unlike temperature.
 
  • #11
I have never seen temperature defined in terms of anything other than entropy, and in some books, using carnot engines.

I guess another way to describe it is "temperature is the thing that is the same for two objects if they are in thermal equilibrium". Then you can say that when an object cannot give any more thermal energy, it is at 0K. But obviously this is a very weak statement and in no way a definition.
 

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