
Paramagnetic substances are characterized by their magnetic susceptibility ($\chi$) at temperatures above any ordering transition (like the ferromagnetic Curie temperature, $T_C$). Their behavior is typically described by the Curie's Law.
Curie's Law states that the magnetic susceptibility ($\chi$) of a paramagnetic material is inversely proportional to the absolute temperature ($T$) in Kelvin:
$ \chi = \frac{C}{T} $
Here, $C$ is the Curie constant, a material-specific positive constant.
To find the relationship for reciprocal susceptibility ($\frac{1}{\chi}$), we can rearrange Curie's Law:
$ \frac{1}{\chi} = \frac{T}{C} $
This equation shows a direct linear relationship between $\frac{1}{\chi}$ and $T$. The plot of $\frac{1}{\chi}$ versus $T$ should be a straight line.
The plot matching this description is shown in Option 3:

The Miller indices of the shown lattice plane in a simple cubic Bravais lattice are :

The R/S configuration of C - 2 and C - 3 in the given molecule will be :
| List-I | List-II |
| Electronic Configuration | First Ionisation energy (kJ mol$^{-1}$) |
| (A). ns$^2$ | (I). 2100 |
| (B). ns$^2$np$^1$ | (II). 1400 |
| (C). ns$^2$np$^3$ | (III). 800 |
| (D). ns$^2$np$^6$ | (IV). 900 |
| List-I | List-II |
| Spectroscopy | Property |
| (A). Raman | (I). Polarizability |
| (B). FTIR | (II). Dipole Moment |
| (C). UV-Visible | (III). Absorbance |
| (D). NMR | (IV). Spin |