Consider a localized ideal spin (with s = (3/2)) system at temperature T in a magnetic field B. Obtain the partition function z for a single spin in the canoncial ensemble, the Helmholtz potential F, the mean value of the total energy (E), the mean value of the total magnetic moment (M), and the susceptibility X and show that it follows the Curie's law (X=(C/T)) at high temperature limit with the Curie constant C = (5/4)*(N/V)*((g2µ2Bµ0)/(kB)).
Consider a localized ideal spin (with s = (3/2)) system at temperature T in a magnetic field B. Obtain the partition function z for a single spin in the canoncial ensemble, the Helmholtz potential F, the mean value of the total energy (E), the mean value of the total magnetic moment (M), and the susceptibility X and show that it follows the Curie's law (X=(C/T)) at high temperature limit with the Curie constant C = (5/4)*(N/V)*((g2µ2Bµ0)/(kB)).
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Consider a localized ideal spin (with s = (3/2)) system at temperature T in a magnetic field B. Obtain the partition function z for a single spin in the canoncial ensemble, the Helmholtz potential F, the mean value of the total energy (E), the mean value of the total magnetic moment (M), and the susceptibility X and show that it follows the Curie's law (X=(C/T)) at high temperature limit with the Curie constant C = (5/4)*(N/V)*((g2µ2Bµ0)/(kB)).
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