A paramagnetic salt sits on a metal sample holder inside a magnet

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

A paramagnetic salt sits on a metal sample holder inside a magnet. The salt carries NN non-interacting electron moments on fixed sites, each with two allowed orientations of energy ∓μmB\mp\mu_{\rm m}B in the applied field BB (aligned and anti-aligned); the field energy is not counted in UU. Salt and holder are both at T=290 KT = 290\,\mathrm{K}, and B=0.50 TB = 0.50\,\mathrm{T}. Take μm=μB=9.27×10−24 J T−1\mu_{\rm m} = \mu_{\rm B} = 9.27\times10^{-24}\,\mathrm{J\,T^{-1}}. ((a)) From the orientation energies and the partition function, derive the total moment M(B,T)M(B,T) along the field, then expand it for μmB≪kBT\mu_{\rm m}B \ll k_BT to obtain Curie's law. State the condition for the expansion and check that it holds here, then find the fractional alignment M/NμmM/N\mu_{\rm m}. ((b)) The holder is modelled as an Einstein solid of NaN_{\rm a} atoms, each vibrating in three directions with a single frequency ν\nu, one oscillator having levels 0,hν,2hν,…0, h\nu, 2h\nu, \dots with the lowest at zero. Derive CVC_V from the single-oscillator partition function, give its high- and low-temperature limits, and evaluate CV/3NakBC_V/3N_{\rm a}k_B at 290 K290\,\mathrm{K} for θE=hν/kB=200 K\theta_E = h\nu/k_B = 200\,\mathrm{K}.

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