2. This problem focuses on a system that contains two indistinguishable bosons. If there are two...
basic Molecular Thermodynamics 2. This problem focuses on a system that contains two indistinguishable bosons. If there are two energy levels available for each of them, then the list of possible states will look like the list in the table in Problem 1, except that the two-particle states numbered 2 and 3 are not different states, in this case. There is only one state that has one of the bosons in ɛj and one in ɛ2, because the bosons cannot...
Consider a system of two particles and assume that there are only two single-particle energy levels ε1, ε2. By enumerating all possible two-body microstates, determine the partition functions if these two particles are (a) distinguishable and (b) indistinguishable.
Question 9 Consider a quantum system comprising two indistinguishable particles which can occupy only three individual-particle energy levels, with energies 81 0, 82 2 and E3 38.The system is in thermal equilibrium at temperature T. (a) Suppose the particles which can occupy an energy level. are spinless, and there is no limit to the number of particles (i) How many states do you expect this system to have? Justify your answer (ii) Make a table showing, for each state of...
Calculate the internal energy, entropy and the equation of states for a system composed of N indistinguishable and non-interacting particles with the partition function (9) given below (a, b and C are constants): q = C(kt)}(V – Nb) eVKY
1-r' Problem 16.12 (30 pts) This chapter examines the two-state system but consider instead the infinite-state system consisting of N non-interacting particles. Each particle i can be in one of an infinite number of states designated by an integer, n; = 0,1,2, .... The energy of particle i is given by a = en; where e is a constant. Note: you may need the series sum Li-ori = a) If the particles are distinguishable, compute QIT,N) and A(T,N) for this...
1. Consider a quantum system comprising three indistinguishable particles which can occupy only three individual-particle energy levels, with energies ε,-0, ε,-2e and ε,-3. The system is in thermal equilibrium at temperature T. Suppose the particles are bosons with integer spin. i) How many states do you expect this system to have? Justify your answer [2 marks] (ii) Make a table showing, for each state of this system, the energy of the state, the number of particles (M, M,, N) with...
[1 44= 9 marks ] Question 5 Consider two identical particles in 1D which exist in single-particle (normalised) (x), and are in such close proximity they can be considered as indistinguishable. wave functions /a(x) and (a) Write down the symmetrised two-particle wave function for the case where the particles are bosons (VB) and the case where the particles are fermions (Vp). (b) Show that the expectation value (xjr2)B,F is given by: (T122) в,F — (а:)a (х)ь + dx x y:(")...
Statistical_Mechanics 2 20 points) 2D ideal Fermi gas 24 Consider an ideal Fermi gas in 2D. It is contained in an area of dimensions L x L. The particle mass is m. (a) Find the density of states D(e) N/L2 (b) Find the Fermi energy as a function of the particle density n = (c) Find the total energy as a function of the Fermi energy ef. (d) Find the chemical potential u as a function of n and T....
Part B All this are multiple questions Part C Part D Part E Question 3 (MCQ QUESTION) [8 Marks) A hypothetical quantum particle in 10 has a normalised wave function given by y(x) = a.x-1.b, where o and bare real constants and i = V-1. Answer the following: a) What is the most likely x-position for the particle to be found at? Possible answers forder may change in SAKAI 14] a - b + ib a 0 Question 3 (MCQ...
2. Fermi-Dirac Statistics. Verify for both the Fermi-Dirac and Bose-Einstein grand partition functions Ż (Equations 7.21 and 7.24 respectively) that the occupancies D (Equation 7.23) and BE (Equation 7.28) can be computed by -1 až where h kT 7.2 Bosons and Fermions called the Fermi-Dirac distribution; I'll call it TFD (7.23) FDT ibution goes to zero when u, and goes to 1 when energy much less than u tend to be occupied, while states r than u tend to be...