Gibbs distribution and Bose statistics

In summary: Therefore, the reasoning used for photon gas cannot be applied to Bose gas. In summary, the chemical potential for a photon gas is zero because the derivative of free energy with respect to the number of particles is zero in equilibrium. However, this reasoning cannot be applied to conclude that the chemical potential is always zero for a Bose gas, as the particles in a Bose gas can move between different quantum states, leading to a non-zero chemical potential even in equilibrium.
  • #1
ala
22
0
For photon gas chemical potential is zero. It is because derivate of free energy with respect to number (T, V fixed) of particles is zero in equilibrium. (free energy has minimum).
I was wondering why cannot I apply this reasoning to conclude (wrong) that chemical potential is zero for any Bose gas?

Explanation:

When deriving Bose statistics one applies Gibbs distribution for variable number of particles (grand canonical) to set of particles in the gas which are in a given quantum state. Then apply formula for grand potential (equal to -PV), mean number of particles in given quantum state is then obtained as derivate of grand potential with respect to chemical potential. So one gets Bose distribution. But if I say now that chemical potential is equal to derivate of free energy with respect to number of particles and latter is equal to zero (when gas is in equilibrium) I get wrong conclusion. Why?
 
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  • #2
Because for Bose gas it is not enough to just consider equilibrium thermodynamics. One should also take into account that particle in gas can move from one quantum state to another. This means that particle number in one or another quantum state can change and therefore chemical potential can no longer be considered as derivate of free energy with respect to number of particles. Even when gas is in equilibrium, there can be non-zero chemical potential if particles can move from one quantum state to another.
 
  • #3


The reasoning you have applied is incorrect because it is based on a misunderstanding of the concept of chemical potential. The chemical potential is not equal to the derivative of the free energy with respect to the number of particles. Rather, it is the change in free energy with respect to the change in number of particles at constant temperature and volume. In other words, it is a measure of the energy required to add one more particle to the system.

In the case of a photon gas, the chemical potential is zero because photons are massless particles and can be added to the system without any additional energy. However, this does not mean that the chemical potential will always be zero for any Bose gas. The chemical potential will depend on the properties of the particles in the gas, such as their mass and interactions with each other. Therefore, the reasoning cannot be applied to conclude that the chemical potential is always zero for any Bose gas.

Furthermore, the fact that the derivative of the free energy with respect to the number of particles is zero at equilibrium does not necessarily mean that the chemical potential is also zero. This is because the free energy is a function of temperature, volume, and number of particles, while the chemical potential is only a function of temperature and volume. Therefore, it is important to understand the fundamental differences between these two quantities and not make assumptions based on incorrect reasoning.
 

1. What is the Gibbs distribution?

The Gibbs distribution, also known as the canonical ensemble, is a statistical distribution that describes the probability of a system being in a particular state at a given temperature, volume, and number of particles. It is based on the principle of equal a priori probabilities, meaning that all accessible microstates of a system have an equal probability of occurring.

2. How is the Gibbs distribution related to thermodynamics?

The Gibbs distribution is closely related to thermodynamics as it provides a probabilistic explanation for the macroscopic behavior of a thermodynamic system. It allows us to calculate the thermodynamic properties of a system, such as the internal energy, entropy, and free energy, by considering the statistics of the particles that make up the system.

3. What are Bose-Einstein statistics?

Bose-Einstein statistics are a type of particle statistics that describes the behavior of identical particles, such as photons, bosons, and some types of composite particles. It was first proposed by Indian physicist Satyendra Nath Bose and further developed by Albert Einstein. In this statistics, particles are allowed to occupy the same quantum state, unlike in classical statistics where each particle must have a unique state.

4. How is Bose-Einstein statistics related to the Gibbs distribution?

The Bose-Einstein statistics are a special case of the Gibbs distribution, where the particles are indistinguishable and can occupy the same quantum state. This means that the probability of a particular state in the Gibbs distribution is given by the Bose-Einstein distribution, which takes into account the symmetry of identical particles.

5. What is the significance of Bose-Einstein statistics in physics?

Bose-Einstein statistics have a significant impact in various fields of physics, such as quantum mechanics, statistical mechanics, and thermodynamics. It has been used to explain the behavior of particles in Bose-Einstein condensates, superfluids, and other quantum phenomena. This statistics also led to the prediction and subsequent discovery of the Higgs boson, an elementary particle that gives mass to other particles.

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