Statistical Mechanics Flashcards
What is the goal of statistical mechanics?
Statistical mechanics considers how particles occupy their allowed quantized energy states and is used to relate molecular behavior to macroscopic thermodynamics.
Boyd, NEGD, Pg 84
Define the degree of molecular randomness.
The number of different ways that N particles can be distributed among their allowable quantum energy states without changing the total energy of the system E.
Boyd NEGD, Pg 84
What is a “microstate?”
If we can arrange N particles in a system such that the total energy E does not change, that particular arrangement of particles is called a microstate.
Boyd NEGD, Pg 85
Particles that have an even number of elementary units are called ______.
Bosons.
Boyd NEGD, Pg 85
True or False
Bosons are analyzed using Bose-Einstein statistics.
True.
Boyd NEGD, Pg 85
Give some examples of Bosons.
Hydrogen atoms
He^4
N_2
Photons
Boyd NEGD, Pg 85
Particles made up of an odd number of elementary particles are called ______.
Fermions.
Boyd NEGD, Pg 85
True or False
Fermions are analyzed using Bose-Einstein statistics.
False. They are analyzed using Fermi-Dirac statistics.
Boyd NEGD, Pg 85
True or False
No two Fermions can occupy the same state.
True.
Boyd NEGD, Pg 85
What are some examples of Fermions?
- Electrons, protons, and He^3
Boyd NEGD, Pg 85
True or False
For Bosons, there is no limit on the number of particles in each energy state.
True.
Boyd NEGD, Pg 88
True or False
Bosons follow the Pauli exclusion principle.
False. Fermions follow this principle.
Wikapedia
Give the general purpose of Bose-Einstein statistics.
Bose-Einstein statistics describe the statistical distribution of indistinguishable particles called bosons that can occupy the same quantum state.
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What is the general purpose of Fermi-Dirac statistics?
The purpose of Fermi-Dirac statistics in statistical mechanics is to provide a framework for understanding the distribution of fermions among quantum states.
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What is a “partition function?”
Physically, the partition function encapsulates the various ways energy can be distributed among the different quantum states of a system. It describes the total number of states available to a system at a given temperature.
It is a mathematical expression that sums up the contributions of all possible energy levels, each weighted by the Boltzmann factor, which accounts for the probability of that energy level being occupied due to the system’s temperature.
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