First Vs. Second law of thermodynamics

In summary, the conversation discusses the concept of entropy and the behavior of an isolated methane molecule in a vacuum room. While the molecule may have a tendency to break its bonds and reach maximum entropy, this is not always the case and the molecule may remain unchanged due to the conservation of energy. Additionally, assigning a temperature to a single molecule may not accurately reflect its state as it could be already dissociated.
  • #1
big_bounce
102
3
Hello Pf's members

Suppose we isolated a methane's molecule at a room with 213 kelvin.
According to second law, methane's molecule tends to break it's bond for reaching whole system (methane's molecule and surroundings) to maximum entropy.
On the other hand for breaking these bonds we need energy but system is isolated and no external energy can income to the room.

Question:
If we have unlimited time , can methane break it's bonds Eventually?
 
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  • #2
The methane molecule can gain or lose energy by its contact to the room. The bond will break eventually, then form again (assuming the atoms don't form any other connections), break again, ...
 
  • #3
mfb said:
The methane molecule can gain or lose energy by its contact to the room. The bond will break eventually, then form again (assuming the atoms don't form any other connections), break again, ...

My question is how does it get energy? there is nothing in the room except a methane molecule.
there isn't any photons. there isn't any atoms.there isn't any molecules. room is like a vacuum and room is isolated. room can not exchange any matter and energy.
breaking bond means violate first law.
 
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  • #4
One cannot speak about the entropy of a single gas molecule, hence your problem is based on a false premise.
 
  • #5
If the room walls cannot exchange energy with the molecule, then temperature is a meaningless concept. Temperature is a thermodynamic limit for many particles, it does not exist for single particles.
 
  • #6
dextercioby said:
One cannot speak about the entropy of a single gas molecule, hence your problem is based on a false premise.
A gas molecule is made of atoms. we have permission for talking about entropy of it's atoms in the room.

mfb said:
If the room walls cannot exchange energy with the molecule, then temperature is a meaningless concept. Temperature is a thermodynamic limit for many particles, it does not exist for single particles.

Therefore, are you saying we couldn't understand a isolated vacuum room with a methane molecule inside it thermodynamically?
If true, is there any approach in physics for understanding and predicting the future of this methane molecule?

In addition: I still strongly believe methane molecule tends to break it's bond for reaching to maximum entropy and after that the atoms and protons decay. the decay satisfy the second law and this is the end.
 
  • #7
The second law is not to be confused with "the dark side of 'the force.' "
 
  • #8
big_bounce said:
Therefore, are you saying we couldn't understand a isolated vacuum room with a methane molecule inside it thermodynamically?
You can, but only as microcanonical ensemble. You cannot assign things like a temperature to it.
big_bounce said:
If true, is there any approach in physics for understanding and predicting the future of this methane molecule?
Sure, the easiest description is via Newton's laws.
big_bounce said:
In addition: I still strongly believe methane molecule tends to break it's bond for reaching to maximum entropy and after that the atoms and protons decay. the decay satisfy the second law and this is the end.
You misunderstand how entropy works. It cannot get smaller. But it does not have to increase. In your example of an isolated molecule it does not change at all.

Proton (or neutron) decay, if it happens at all, would eventually happen while the molecule is still a molecule, potentially ruining the chemistry and leading to something else, depending on which nucleon decays in which way.
 
  • #9
mfb said:
You misunderstand how entropy works. It cannot get smaller. But it does not have to increase. In your example of an isolated molecule it does not change at all.
According to below site:
http://hyperphysics.phy-astr.gsu.edu/hbase/Therm/entrop.html
Concept of entropy is that nature tends from order to disorder in isolated systems.
Now you said me which one is more disorder?

a) a isolated vacuum room with a methane molecules (this figure)
?temp_hash=ad30a7439c72ed2cb85ea3bd359964c3.png

b) a isolated vacuum room with 5 freely atoms? (this figure)
?temp_hash=ad30a7439c72ed2cb85ea3bd359964c3.png

Therefore, I think methane tends to break it's bond but it couldn't because first law is preceded to The second law.
 

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  • #10
big_bounce said:
Concept of entropy is that nature tends from order to disorder in isolated systems.
Your bound molecule already has the maximal disorder for its energy. Done. Nothing will happen.
 
  • #11
mfb said:
Your bound molecule already has the maximal disorder for its energy. Done. Nothing will happen.

I couldn't understand how you say methane has more entropy than it's components.

In this formula 2H2+C-->CH4

We have 3 mole of reactions and mole of production. so obviously methane has less entropy than 2 hydrogen molecules and 1 carbon and tends to break it's bond.
If temperature be enough the breaking will happen more likely. but system is isolated and no changing in temperature could occur.
 
  • #12
Your bound molecule already has the maximal disorder for its energy.
A single molecule doesn't have a temperature. It is just flying around forever without doing anything else.
 
  • #13
You can assign temperature even to a single methane molecule, but this means that you don't have full information about the state of the molecule. I.e. it could be that it is already dissociated at the very beginning.
 
  • #14
DrDu said:
You can assign temperature even to a single methane molecule
Not in any meaningful way.
 
  • #15
You can have a methane molecule in a room with walls of a given temperature. Then the molecule will be in thermal equilibrium after a short time and you can assign it a temperature. If you now replace the walls with adiabatic ones, the temperature of the particle won't change. This kind of experiments are standard for all kinds of particles inside some particle traps. So the answer to the OPs question is: By assigning a temperature to the molecule, you already lack information on whether the molecule is intact or dissociated from the very beginning.
 
  • #16
OP specified no thermal contact to the walls and an intact molecule to start with.
 
  • #17
All that is conserved is that there is one carbon and 4 hydrogen atoms. Whether they are bound or not is never certain at finite temperature.
 
  • #18
DrDu said:
Then the molecule will be in thermal equilibrium after a short time and you can assign it a temperature.
Echoing what has already been said...

You can meaningfully assign a temperature to a system of which a molecule is a part. But this does not entail that you can meaningfully and correctly assign that same temperature to all of the component parts of that system down to the level of individual molecules. In thermal equilibrium, there will be an energy distribution. Some molecules will have more energy at a given time. Some less. Even if you decide that the "temperature" of a single molecule is equivalent to its kinetic (plus vibrational plus rotational) energy, there is no guarantee that the energy of that molecule will be representative of the temperature of the larger system of which it is or had been a part.

Once you close the system and eliminate thermal contact with the walls, the total energy of that methane molecule is fixed. If there is not enough energy to break its molecular bonds, then those bonds will not break. Without that energy, an unbound set of five atoms is not a possible state to which the system can evolve.
 
  • #19
jbriggs444 said:
Even if you decide that the "temperature" of a single molecule is equivalent to its kinetic (plus vibrational plus rotational) energy, there is no guarantee that the energy of that molecule will be representative of the temperature of the larger system of which it is or had been a part.
That energy of a small system representative of a canonical ensemble with a given temperature isn't fixed is well known and not at variance with the concept of temperature.
 
  • #20
DrDu said:
That energy of a small system representative of a canonical ensemble with a given temperature isn't fixed is well known and not at variance with the concept of temperature.
That is certainly true.

Now then. If we had a single molecule in a room with perfectly reflective walls that neither absorb nor transmit energy, what would you mean by the "temperature" of the system?
 
  • #21
That would depend on the history of its preparation, better to say, on my knowledge about it. If I had no knowledge at all, I would assign it the temperature which maximizes its entropy, i.e. an infinitely high energy.
 
  • #22
DrDu said:
That would depend on the history of its preparation, better to say, on my knowledge about it. If I had no knowledge at all, I would assign it the temperature which maximizes its entropy, i.e. an infinitely high energy.
Thank you. That makes your picture (and the differences from my mental picture of the intended scenario) more clear.
 
  • #23
Don't get me wrong here. I don't mean this to be the only possible way to deal with the situation, but at least a possible one. If the OP really wants to describe a single molecule with a temperature, this can be done and may even be advantageous in certain settings.
We are also experiencing, that it may not always be correct, to describe even large systems in thermodynamical terms. Whole genome sequencing is an example.
People are collecting hundreds of terabytes of data about macroscopic ammounts of microscopic DNA sniplets. Maxwells demon has become alive and active!
 

Related to First Vs. Second law of thermodynamics

What is the first law of thermodynamics?

The first law of thermodynamics, also known as the law of conservation of energy, states that energy cannot be created or destroyed, but can only be transferred or converted from one form to another.

What is the second law of thermodynamics?

The second law of thermodynamics states that in any energy conversion or transfer, the total amount of energy in the universe remains constant, but the quality of energy decreases over time. This is due to the fact that some energy is always lost as heat in the process.

What is the key difference between the first and second law of thermodynamics?

The first law of thermodynamics focuses on the conservation of energy, while the second law focuses on the quality of energy and the direction in which energy flows.

How do these laws relate to entropy?

Entropy is a measure of the disorder or randomness in a system. The second law of thermodynamics states that the total entropy of a closed system will always increase over time, as energy is converted and dispersed. This means that the direction of energy flow is always towards higher entropy.

Can these laws be violated or broken?

No, the laws of thermodynamics are considered fundamental laws of nature and have been tested and proven through numerous experiments. They cannot be violated or broken under normal circumstances.

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