Introduction to Thermostatics and Statistical Mechanics A typical physical system has N A = X particles. Each particle has 3 positions and 3 momentums. Thus there are around degrees of freedom But we see that in day to day life, we do not need to specify that many variables For example we need to specify only temperature (T), volume (V), and number of moles (N) of the gas in the room and we specify the system completely. This is almost a miracle. The reason for this miracle is that: We are interested in processes that are slow on time-scales of atomic vibrations and occur at larger length scales than the atomic spacing. The symmetries of most system work in such a way that of the degrees of freedom we are left with only a few variables. The variables are called microvariables. The variables (for example, T, V, N) are called macrovariables.

Microstates and Macrostates Described by microstate {p i, q i }. The position and momentum of all particles. 3 positions, q i and 3 momentums, p i per particle. So in all (3+3) X microvariables. Macrostate described by 3 quantities T, V, N. Example 1: Gas in a Box

Microstates and Macrostates The microstate described a particular configuration of the chain on the lattice. If there are N links on the chain, there are N variables. Macrostate described by just the thermodynamic radius R of the chain. Example 2: Polymer Chain

Microstates and Macrostates The gas binds on the binding sites on the substrate with favorable energy. The microstate described by a particular binding configuration of the gas on the substrate. Macrostate described by just the average number of particles bound to the substrate. Example 3: Gas Adsorption

Goal There are many microstates. We get experimentally reproducible behavior from only a few macrovariables. If that macrovariable is, say, E, define where, p i is the probability that the system is in state i. We want to find, p i. Given.

Means: Gibbs Entropy Recipe is to maximize Gibbs entropy Subject to constraints on the system Hence find p i. Once we know p i. We can find any other quantity B as:

Boltzmann Distribution Consider a system at temperature, T in thermal equilibrium with the heat bath. The thermodynamic energy, of the system is constant. We maximize Gibbs entropy subject to this constraint. We use the method of lagrange multipliers. Writing a modified entropy Normalization refers to the fact that, Maximizing w.r.t p i and using the normalization constraint we will get.

Partition Function The denominator of is the most important quantity. It is called partition function. It is denoted by Z. Substituting the p i obtained in Gibb’s entropy formula, we get, Differentiating S w.r.t and using above eqn, we get

Properties of partition function The free energy of the system is hence: Thus derivative of ln Z w.r.t to the lagrange multiplier gives corresponding average quantity.

Example 1: Ideal Gas Law

Example 2: Force-Displacement relation for a chain