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Heat Capacity. The constant volume heat capacity of a system with average energy $\langle E\rangle$ is given by $C_v=\left(\frac{\partial\langle E\rangle}{\partial T}\right)_{N, V}$ Use the canonical ensemble to prove that: $C$ is related to the meansquare fluctuation in the energy as follows: $$ C_v=\frac{1}{k T^2}\left\langle(E-\langle E\rangle)^2\right\rangle . $$

   Heat Capacity.
The constant volume heat capacity of a system with average energy $\langle E\rangle$ is given by $C_v=\left(\frac{\partial\langle E\rangle}{\partial T}\right)_{N, V}$

Use the canonical ensemble to prove that: $C$ is related to the meansquare fluctuation in the energy as follows:
$$
C_v=\frac{1}{k T^2}\left\langle(E-\langle E\rangle)^2\right\rangle .
$$
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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 116 ↓

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In the canonical ensemble, the probability of a system being in a state with energy \( E_i \) at temperature \( T \) is given by the Boltzmann distribution: \[ P_i = \frac{e^{-\beta E_i}}{Z} \] where \( \beta = \frac{1}{kT} \) and \( Z \) is the partition function  Show more…

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Heat Capacity. The constant volume heat capacity of a system with average energy $\langle E\rangle$ is given by $C_v=\left(\frac{\partial\langle E\rangle}{\partial T}\right)_{N, V}$ Use the canonical ensemble to prove that: $C$ is related to the meansquare fluctuation in the energy as follows: $$ C_v=\frac{1}{k T^2}\left\langle(E-\langle E\rangle)^2\right\rangle . $$
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Key Concepts

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Heat Capacity
Heat capacity is a thermodynamic property that measures the amount of heat required to change the temperature of a system by a given amount. It is formally defined as the derivative of energy with respect to temperature. In this problem, the constant volume heat capacity is expressed as the partial derivative of the average energy with respect to temperature, indicating how energy fluctuations respond to temperature changes.
Canonical Ensemble
The canonical ensemble is a statistical framework used to describe a system that is in thermal equilibrium with a heat reservoir at a fixed temperature. In this ensemble, the number of particles, volume, and temperature are held constant, and the system exchanges energy with the reservoir. It provides the basis for calculating ensemble averages, such as the average energy, which are pivotal in linking microscopic fluctuations to macroscopic thermodynamic quantities.
Partition Function
The partition function is a central quantity in statistical mechanics that encapsulates all the statistical properties of a system in the canonical ensemble. It is a sum over all possible states, weighted by the Boltzmann factor, and serves as a generating function for thermodynamic variables. The derivatives of the partition function with respect to temperature yield important thermodynamic quantities like average energy and heat capacity.
Ensemble Average
Ensemble averages are the expected values of physical quantities when considering all possible microstates of a system in a given ensemble. In the canonical ensemble, the average energy is computed as a weighted sum over states, where the weights are determined by the Boltzmann factors. Ensemble averages connect microscopic statistical properties with macroscopic observables such as heat capacity.
Energy Fluctuations
Energy fluctuations refer to the variations of the system's energy around its average value. In statistical mechanics, the mean-square fluctuation of energy quantifies the degree of these fluctuations. These fluctuations are directly related to the second derivative of the logarithm of the partition function with respect to temperature, linking microscopic randomness with macroscopic thermodynamic response functions.
Fluctuation-Dissipation Relation
The fluctuation-dissipation theorem establishes a fundamental connection between the system's response to external perturbations (such as changes in temperature) and its internal fluctuations. In the context of heat capacity, this relation shows that the constant volume heat capacity is proportional to the variance of the energy fluctuations, offering deep insight into how microscopic dynamics govern macroscopic thermal properties.

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The fluctuation in energy, denoted as ΔE, in the canonical ensemble is given by ΔE = (E - Ē)kBT/Cv, where T is the absolute temperature and Cv is the heat capacity at constant volume. Calculate ΔE for a system of photons in an enclosure of volume V at temperature T.

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