Difficulty: Easy
Correct Answer: True
Explanation:
Introduction / Context:
Magnetization arises from two broad mechanisms: (i) field-induced moments (e.g., diamagnetism and the linear part of paramagnetism) and (ii) permanent magnetic dipoles associated with unpaired electron spins and domain structures (paramagnets, ferromagnets). Understanding their independence clarifies magnetic responses across materials.
Given Data / Assumptions:
Concept / Approach:
The induced magnetic dipole moment is created by the field’s action on electronic orbits/spins and is proportional to the applied field for small fields: m_induced ∝ H (or B). The permanent moment, m_perm, is intrinsic to the material (e.g., unpaired spins, domains). To first order, m_induced is independent of m_perm; the total moment is m_total = m_perm + m_induced. Couplings can exist at large fields or in nonlinear regimes, but the basic statement about independence of the induced component from the inherent permanent moment is correct in standard linear-response theory.
Step-by-Step Solution:
Verification / Alternative check:
Materials with zero permanent moments (pure diamagnets) still exhibit induced magnetization; ferromagnets with large permanent moments also show an additional field-induced component (differential susceptibility).
Why Other Options Are Wrong:
Stating “False” assumes dependence; options restricting to special materials or extreme conditions ignore the general linear regime.
Common Pitfalls:
Confusing vector alignment effects of permanent moments with the creation of induced moments; mixing nonlinear saturation behavior with small-signal response.
Final Answer:
True
Discussion & Comments