It is possible to express the magnetic susceptibility \(\chi_{m}\) in several
different units. For the discussion of this chapter, \(\chi_{m}\) was used to
designate the volume susceptibility in SI units, that is, the quantity that
gives the magnetization per unit volume \(\left(\mathrm{m}^{3}\right)\) of
material when multiplied by \(H\). The mass susceptibility
\(\chi_{m}(\mathrm{~kg})\) yields the magnetic moment (or magnetization) per
kilogram of material when multiplied by \(H ;\) similarly, the atomic
susceptibility \(\chi_{m}\) (a) gives the magnetization per kilogram-mole. The
latter two quantities are related to \(\chi_{m}\) through the relationships
$$
\begin{aligned}
&\chi_{m}=\chi_{m}(\mathrm{~kg}) \times \text { mass density (in } \mathrm{kg}
/ \mathrm{m}^{3} \text { ) } \\
&\left.\chi_{m}(\mathrm{a})=\chi_{m}(\mathrm{~kg}) \times \text { atomic
weight (in } \mathrm{kg}\right)
\end{aligned}
$$
When using the cgs-emu system, comparable parameters exist, which may be
designated by \(\chi_{m}^{\prime}, \chi_{m}^{\prime}(\mathrm{g})\), and
\(\chi_{m}^{\prime}(\mathrm{a})\); the \(\chi_{m}\) and \(\chi_{m}^{\prime}\) are
related in accordance with Table 20.1. From Table \(20.2, \chi_{m}\) for silver
is \(-2.38 \times 10^{-5}\); convert this value into the other five
susceptibilities