Consider a paramagnetic material made up of atoms, each with intrinsic magnetic moment of magnitude to with number density n atoms per unit volume. according to classical thermodynamics, the probability of each atom to be in a state of energy e is given by e p(e)=t exp (1) where t is the absolute temperature of the material, kp is the boltzmann constant, and t is a normalization factor determined by the requirement that the sum of all probabilities must be 1. if a magnetic field bo is applied to the material, quantum mechanics dictates that the atoms must be in one of two states: with magnetic moment parallel to the magnetic field, or antiparallel. the number of atoms in each state is governed by the above probability distri- bution. calculate the magnetization-magnetic moment per unit volume of this material, as a function of n, u, magnetic field magnitude bo, t, and assorted constants. disregard competing diamagnetic effects.