QUESTION 3 IS JUST ATTACHED FOR THE UNDERSTANDING
Problem 3: Imagine a system of N spins on lattice sites, but this time the spins can have three possible states. The three states contribute an energies ( and EpoH when a magnetic field H is applied. We are first going to treat this problem in the microcanoni- cal ensemble. Write down the number of ways there are to distribute the total energy U between a system of N1 particles contributing an energy Mo, N2 contributing an energy O and Nz contributing an energy - Mo. Write this expression just as a function of U and N = Ni + N2 + N3. You will quickly see why the microcanonical ensemble is not such a clever device. = Problem 4: Redo the previous problem but now using the canonical ensemble cal- culate the thermodynamic properties of entropy, energy, heat capacity. See how these quantities vary in the high and low temperature limits.
Problem 3: Imagine a system of N spins on lattice sites, but this time the spins can have three possible states. The thr
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Problem 3: Imagine a system of N spins on lattice sites, but this time the spins can have three possible states. The thr
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