Concept:
Magnetic susceptibility ($\chi_m$) is a dimensionless proportionality constant that quantifies how a material responds to an externally applied magnetic field ($H$). It is defined by the fundamental constitutive vector equation:
\[
M = \chi_m H
\]
Where $M$ is the induced magnetization per unit volume.
Diamagnetism is a universal property found in all materials where atoms contain completely filled electronic shells, resulting in zero net permanent atomic magnetic moments ($\mu_{atom} = 0$) in the absence of an external field.
Step 1: Understanding Lenz's Law at the atomic scale.
When a diamagnetic material is placed inside an external magnetic field $H$, the changing magnetic flux alters the orbital motion of the paired electrons. According to Lenz's law of electromagnetism, these induced orbital currents adjust their paths to generate a microscopic magnetic field that directly opposes the applied external field.
Step 2: Determining the mathematical sign of magnetization and susceptibility.
Because the internally induced magnetization $M$ works in direct opposition to the applied field direction $H$, the vectors point in completely opposite directions. Expressing this mathematically:
\[
M \propto -H \quad \Rightarrow \quad M = \chi_m H
\]
This opposing behavior requires the proportionality coefficient $\chi_m$ to be strictly negative:
\[
\chi_m < 0
\]
Typically, for diamagnetic substances (like Copper, Water, and Bismuth), $\chi_m$ is a small, constant negative value ($\sim -10^{-5}$ to $-10^{-6}$) and is independent of temperature.
Step 3: Checking the other options.
• Option A: Diamagnets have zero permanent magnetic moments; permanent moments are characteristic of paramagnetic and ferromagnetic substances.
• Option C: Positive susceptibility ($\chi_m > 0$) is characteristic of paramagnets and ferromagnets.
• Option D: Hysteresis loops represent domain-wall friction and energy dissipation, which only occur in ferromagnetic and ferrimagnetic materials.
Hence, a negative magnetic susceptibility ($\chi_m < 0$) uniquely describes diamagnetic materials.