1. Principles of Equal a Priori Probability  All distributions of energy are equally probable  If E = 5 and N = 5 then                   All configurations have equal probability, but possible number of way (weight) is different.

2. A Dominating Configuration  For large number of molecules and large number of energy levels, there is a dominating configuration.  The weight of the dominating configuration is much more larger than the other configurations. Configurations WiWi {n i }

3. Dominating Configuration                   W = 1 (5!/5!)W = 20 (5!/3!)W = 5 (5!/4!) Difference in W becomes larger when N is increased ! In molecular systems (N~10 23 ) considering the most dominant configuration is enough for average

4. 8.4 The most probable distribution, equilibrium distribution, and Boltzmann distribution  8.4.1 The principle of equal a priori probabilities Statistical thermodynamics is based on the fundamental assumption that all possible configurations of a given system, which satisfy the given boundary conditions such as temperature, volume and number of particles, are equally likely to occur.

5.  Example Consider the orientations of three unconstrained and distinguishable spin-1/2 particles. What is the probability that two are spin up and one spin down at any instant?  Solution Of the eight possible spin configurations for the system,  ↑↑↑ ↑↑↓ ↑↓↑ ↓↑↑ ↑↓↓ ↓↑↓ ↓↓↑ ↓↓↓  The second, third, and fourth comprise the subset "two up and one down". Therefore, the probability for this particular configuration is  P = 3/8