Course Instructors: Aveek Bid and Shibananda Das
Start Date: 02/01/2025
End Date: 21/04/2025
• We are going to focus on the equilibrium properties that are described best through
thermodynamics. We start with thermodynamics. Basically, it's a phenomenological
approach, so you essentially look at something as a kind of black box, without knowing what
the ingredients are, and try to give some kind of description of how its function and properties
change. These can be captured, for the case of thermal properties of matter, through the laws of
thermodynamics, which we will set out in this first section, which will roughly take us the first
four lectures of the course.
• Then we learn that statistical mechanics is a probabilistic approach – to deal with a large
number of degrees of freedom.
• But then we said large number of degrees of freedom. So what are these degrees of freedom?
In thermodynamics, you look at the system as a black box and try to develop laws based on
observations. We know that this box contains atoms and molecules that follow very specific
laws, either from Newtonian mechanics or quantum mechanics. And so if we know everything
about how atoms and molecules behave, then we should be able to derive how large collections
of them behave. And get the laws of thermodynamics as a consequence of these microscopic
degrees of freedom and their dynamics. And so that's what we will discuss in the third part of
the course that is devoted to kinetic theory.
• It is beneficial to, rather than follow individual particles in a system, adopt a probabilistic
approach and think about densities and how those densities evolve according to Liouville's
Theorem.
• What we will also try to establish is a very distinct difference that exists between
thermodynamics, where things are irreversible and going in one direction, and Newtonian, or
quantum mechanics, where things are reversible in time. And we'll see that really it's a matter
of adapting the right perspective in order to see that these two ways of looking at the same
system are not in contradiction.
• So having established these elements, we will discuss statistical mechanics in terms of some
postulates about how probabilities behave for systems that are in equilibrium. And how based
on those postulates, we can then derive all the laws of thermodynamics and all the properties
of thermodynamics systems.
• Classical systems-- description of particles following classical laws of motion. And, again, as a
first simplification, we will typically deal with non-interacting systems, such as ideal gas. And
make sure that we understand the properties of this important fundamental system from all
possible perspectives.
• Realistic classical systems where there are interactions among these particles. And there are
two ways to then deal with interactions.
• You can either go by the way of perturbation theory. We can start with the ideal system and add
a little bit of interaction and see how that changes things. Or, you can take another perspective,
and say that because of the presence of interactions, the system really adopts a totally different
type of behavior.
• And there's a perspective known as mean-field theory that allows you to do that. Then see how
the same system can be present in different phases of matter, such as liquids and gas, and how
this mean field type of prescription allows you to discuss the transitions between the different
types of behavior.
• Quantum description of the microscopic degrees of freedom. We will see how the differences
and similarities between quantum statistical mechanics and classical statistical mechanics
emerge.
• The place where quantum statistical mechanics shows its power is in dealing with identical
particles, which classically, really are kind of not a very well-defined concept, but quantum-
mechanically, they are very precisely defined, what identical particles mean. And there are two
classes-- fermions and bosons--and how even if there's no interaction between them, quantum
statistics leads to unusual behavior for quantum systems of identical particles, very distinct for
fermions and for bosons.
Pathria, Beale - Statistical Mechanics. (totally followed)
Mehran Kardar - Statistical Mechanics of particles.
Reif - Statistical Physics.
Statistical Mechanics of particles - Mehran Kardar, MIT: https://ocw.mit.edu/courses/8-333-statistical-mechanics-i-statistical-mechanics-of-particles-fall-2013/.