Difficulty: Easy
Correct Answer: θ may be equal to less than or more Q_f
Explanation:
Introduction:
Magnetic phase transitions are characterized by the Curie temperature T_c (here denoted Q_f) at which a ferromagnet becomes paramagnetic. Above T_c, the Curie–Weiss law often describes susceptibility with a parameter θ called the paramagnetic Curie temperature. Understanding how θ compares with T_c in real materials is important for interpreting experimental susceptibility data.
Given Data / Assumptions:
Concept / Approach:
In the simplest mean-field model for an ideal ferromagnet, θ equals T_c. However, in real ferromagnetic and ferrimagnetic materials, θ extracted from high-temperature fits can differ from T_c due to short-range order, crystal-field effects, itinerant-electron contributions, or measurement range limitations. Consequently, θ may be slightly greater than, less than, or approximately equal to T_c (Q_f).
Step-by-Step Solution:
Verification / Alternative check:
Experimental 1/χ plots for different ferromagnets show varying θ relative to T_c; some itinerant ferromagnets yield θ > T_c, while localized systems may show θ ≈ T_c or θ < T_c depending on interactions.
Why Other Options Are Wrong:
Options A–C impose a strict inequality or limited relation that does not universally hold; Option E is arbitrary and incorrect.
Common Pitfalls:
Assuming ideal mean-field behavior applies perfectly to all materials; ignoring experimental uncertainties and fitting ranges that shift the apparent θ.
Final Answer:
θ may be equal to less than or more Q_f
Discussion & Comments