Question

(a) Calculate the partition function $z$ of one spinless atom of mass $M$ moving freely in a cube of volume $V=L^3$. Express your result in terms of the quantum concentration $$ n_q=\left(\frac{M k T}{2 \pi}\right)^{3 / 2} . $$ Explain the physical meaning of $n_q$. (b) An ideal gas of $N$ spinless atoms occupies a volume $V$ at temperature $T$. Each atom has only two energy levels separated by an energy $\Delta$. Find the chemical potential, free energy, entropy, pressure and heat capacity at constant pressure.

   (a) Calculate the partition function $z$ of one spinless atom of mass $M$ moving freely in a cube of volume $V=L^3$. Express your result in terms of the quantum concentration
$$
n_q=\left(\frac{M k T}{2 \pi}\right)^{3 / 2} .
$$

Explain the physical meaning of $n_q$.
(b) An ideal gas of $N$ spinless atoms occupies a volume $V$ at temperature $T$. Each atom has only two energy levels separated by an energy $\Delta$. Find the chemical potential, free energy, entropy, pressure and heat capacity at constant pressure.
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Problems and Solutions on Thermodynamics and Statistical Mechanics
Problems and Solutions on Thermodynamics and Statistical Mechanics
U.S.T. of China… 1st Edition
Chapter 2, Problem 128 ↓

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** The partition function \( z \) for a single particle in a three-dimensional box can be expressed as: \[ z = \frac{1}{h^3} \int e^{-\beta H} \, d^3p \, d^3q \] where \( H \) is the Hamiltonian, \( \beta = \frac{1}{kT} \), \( h \) is Planck's constant, \( p \)  Show more…

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(a) Calculate the partition function $z$ of one spinless atom of mass $M$ moving freely in a cube of volume $V=L^3$. Express your result in terms of the quantum concentration $$ n_q=\left(\frac{M k T}{2 \pi}\right)^{3 / 2} . $$ Explain the physical meaning of $n_q$. (b) An ideal gas of $N$ spinless atoms occupies a volume $V$ at temperature $T$. Each atom has only two energy levels separated by an energy $\Delta$. Find the chemical potential, free energy, entropy, pressure and heat capacity at constant pressure.
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Key Concepts

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Pressure
Pressure is defined as the force per unit area exerted by the particles of a system, often derived from the derivative of the free energy with respect to volume. It is an essential thermodynamic parameter that relates to how systems respond to changes in volume and is critical to understanding the behavior of gases and fluids in equilibrium.
Partition Function
The partition function is a central concept in statistical mechanics. It is the sum over all possible microstates of the system, each weighted by an exponential factor of the negative energy divided by kT. This function encapsulates the statistical properties of the system, providing a bridge between microscopic quantum states and macroscopic thermodynamic quantities such as internal energy, free energy, and entropy.
Quantum Concentration
Quantum concentration is a measure of the density of particles at which quantum effects become significant. It is defined in terms of the thermal de Broglie wavelength and mass of the particles, providing a criterion for when the wave functions of the particles start to overlap. This concept helps in identifying the regime where classical statistics are no longer valid and quantum statistics must be applied.
Two-Level Systems
A two-level system is a simplified model in which each particle or atom can only occupy one of two distinct energy states. This model is often used to describe various physical phenomena ranging from magnetic spins in an external field to simplified models of electronic transitions. The energy difference between the two levels plays a crucial role in determining the thermodynamic behavior of the system, particularly in the presence of thermal excitations.
Chemical Potential
Chemical potential is a thermodynamic parameter that represents the change in a system’s free energy when an additional particle is introduced, keeping temperature and volume constant. It is crucial for describing particle exchange, equilibrium conditions in multi-component systems, and phase transitions. In statistical mechanics, it also determines the occupation probabilities of energy states in ensembles where the particle number fluctuates.
Free Energy
Free energy, such as the Helmholtz free energy, is a thermodynamic potential that measures the amount of work a system can perform at constant temperature and volume. It combines the system's internal energy and entropy in a way that predicts the direction of spontaneous processes and helps determine equilibrium properties.
Entropy
Entropy is a fundamental measure of the disorder or randomness in a system. It quantifies the number of possible microstates corresponding to a given macrostate and plays a central role in the second law of thermodynamics. In statistical mechanics, entropy links the microscopic configuration of a system to its macroscopic thermodynamic behavior.
Heat Capacity
Heat capacity at constant pressure is a measure of the amount of energy needed to raise the temperature of a system by one degree while maintaining a constant pressure. This response function provides insights into the energy storage and phase transition behaviors of the system and plays an important role in characterizing thermal properties.

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