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SUMMARY

The discussion focuses on deriving the mean magnetic moment \( M \) of a paramagnetic crystal with \( N \) ions of spin \( \frac{1}{2} \) in a magnetic field \( B \) at constant temperature \( T \). The conclusion is that the mean magnetic moment is expressed as \( \mu \tanh\left(\frac{\mu B}{kT}\right) \). Key equations utilized include the Helmholtz Free Energy minimization, the relationship between magnetic work and magnetic field, and the partition function \( Z \). The derivation confirms the correctness of the formula, ensuring clarity for tutoring purposes.

PREREQUISITES
  • Understanding of Helmholtz Free Energy in thermodynamics
  • Knowledge of paramagnetic materials and their properties
  • Familiarity with statistical mechanics concepts, particularly partition functions
  • Basic principles of magnetism, including magnetic work and field relationships
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  • Study the derivation of the Helmholtz Free Energy and its applications in statistical mechanics
  • Explore the properties of paramagnetic materials and their behavior in magnetic fields
  • Learn about the partition function and its significance in thermodynamic calculations
  • Investigate advanced topics in magnetism, such as ferromagnetism and antiferromagnetism
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Students and educators in physics, particularly those focusing on thermodynamics and statistical mechanics, as well as researchers studying magnetic materials and their properties.

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Homework Statement



A paramagnetic crystal of N ions of spin 1/2, at constant temperature T, is subjected to a magnetic field B. Using the fact that the Helmholtz Free Energy is minimized show that the mean magnetic moment M is:

\mu tanh\frac{\mu B}{kT}

Homework Equations



Magnetic work:dW=-\mu_0 M dH

For paramagnetic material: H=\frac{B}{\mu_0}Energy of alignment with field: \mu B

The Attempt at a Solution



If Free Energy is minimum dF=dE-TdS=0

Using II Law of TD

dS=\frac{dQ}{T} \rightarrow TdS=dQ

and I Law of TD

dQ=dE+dW = dE-\mu_0 M dH

Gives:

dF=\mu_0 M dH = MdB

Therefore:

\frac{dF}{dM}=M

Using
F=-kT\ln Z

where
Z = exp\left(\frac{-\mu B}{kT}\right) + exp\left(\frac{\mu B}{kT}\right) = 2 cosh\left(\frac{\mu B}{kT}\right)

Differientiating with respect to B and doing some algebra gives.

\mu tanh\frac{\mu B}{kT}

QED

Anyone see any problems, I appreciate the help.
 
Last edited:
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Please anyone? I really need this because I'm tutoring and don't want to give a solution I'm not 100% about.
 

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