In a magnetic-cooling stage a paramagnetic salt holds identical magnetic moments on…

PHYSICS · Multi-part · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Condensed Matter, Materials & Soft Matter · Lattice dynamics and thermal properties of solids

Thermal Physics, Ch Two-level systems, paramagnets and the Einstein solid

Problem

In a magnetic-cooling stage a paramagnetic salt holds NN identical magnetic moments on fixed lattice sites. Each moment has two allowed orientations in the applied field BB, of energy −μmB-\mu_{\rm m}B when aligned with the field and +μmB+\mu_{\rm m}B when anti-aligned. The moments do not interact with one another, the field energy itself is not counted in UU, and the whole sample is in equilibrium at temperature TT. ((a)) Starting from the two orientation energies, write the single-moment partition function Z1Z_1, form ZNZ_N and the free energy FF, and hence derive the total moment along the field, M=−(∂F/∂B)TM = -(\partial F/\partial B)_T. Check the saturation limit. Then evaluate M/NμmM/N\mu_{\rm m} and MM for one mole of electron moments, μm=μB=9.27×10−24 J T−1\mu_{\rm m} = \mu_{\rm B} = 9.27\times10^{-24}\,\mathrm{J\,T^{-1}}, at T=2.0 KT = 2.0\,\mathrm{K} in B=3.0 TB = 3.0\,\mathrm{T}. ((b)) The lattice of the same salt is modelled as an Einstein solid: each of its NaN_{\rm a} atoms vibrates in three directions with one frequency ν\nu, one oscillator having levels 0,hν,2hν,…0, h\nu, 2h\nu, \dots with the lowest set at zero. Derive CVC_V from the single-oscillator partition function, state the high- and low-temperature limits, and evaluate CV/3NakBC_V/3N_{\rm a}k_B at 2.0 K2.0\,\mathrm{K} for a lattice with θE=hν/kB=150 K\theta_E = h\nu/k_B = 150\,\mathrm{K}.

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