Data: \(\frac{N}{V}\) = 2.0 × 1026 atoms/m3,
μ = 1.5 × 10-23 Am2, T = 27 + 273 = 300 K,
B = 3T, kB = 1.38 × 10-23 J/K, 1 eV = 1.6 × 10-19 J
(a) The maximum magnetization of the material,
Mz = \(\frac{N}{V}\)μ =(2.0 × 1026) (1.5 ×10-23)
= 3 × 103 A/m
(b) The maximum orientation energy per atom is
Um = -μB cos 180° = μB
= (1.5 × 10-23) (3) = \(\frac{4.5 \times 10^{-23}}{1.6 \times 10^{-19}}\)
= 2.8 × 10-4 eV
The average thermal energy of each atom,
E = \(\frac{3}{2}\) kBT
where kB is the Botzmann constant.
∴ E = 1.5(1.38 × 10-23)(300)
= 6.21 × 10-21 J = \(\frac{6.21 \times 10^{-21}}{1.6 \times 10^{-19}}\)
= 3.9 × 10-2 eV
Since the thermal energy of randomization is about two orders of magnitude greater than the magnetic potential energy of orientation, saturation magnetization will not be achieved at 300 K.