| List-I (Complex ion) | List-II (Spin only magnetic moment in B.M.) |
|---|---|
| (A) [Cr(NH$_3$)$_6$]$^{3+}$ | (I) 4.90 |
| (B) [NiCl$_4$]$^{2-}$ | (II) 3.87 |
| (C) [CoF$_6$]$^{3-}$ | (III) 0.0 |
| (D) [Ni(CN)$_4$]$^{2-}$ | (IV) 2.83 |
To match the complex ions in List-I with their respective spin-only magnetic moments in List-II, we need to understand the concept of spin-only magnetic moment, which is given by the formula:
\(\mu = \sqrt{n(n+2)}\) Bohr Magneton (B.M.),
where \(n\) is the number of unpaired electrons in the complex ion.
Thus, the correct match between List-I and List-II is:
The spin-only magnetic moment ($\mu$) in Bohr Magnetons (B.M.) is calculated using the formula: \[ \mu = \sqrt{n(n+2)} \, \text{B.M.}, \] where $n$ is the number of unpaired electrons.
(A) [Cr(NH$_3$)$_6$]$^{3+}$: \[ \text{Cr}^{3+}: 3d^3 \, (3 \, \text{unpaired electrons}). \]
\[ \mu = \sqrt{3(3+2)} = 3.87 \, \text{B.M.} \, (\text{II}). \]
(B) [NiCl$_4$]$^{2-}$: \[ \text{Ni}^{2+}: 3d^8 \, (2 \, \text{unpaired electrons}). \]
\[ \mu = \sqrt{2(2+2)} = 2.83 \, \text{B.M.} \, (\text{IV}). \]
(C) [CoF$_6$]$^{3-}$: \[ \text{Co}^{3+}: 3d^6 \, (4 \, \text{unpaired electrons}). \]
\[ \mu = \sqrt{4(4+2)} = 4.90 \, \text{B.M.} \, (\text{I}). \]
(D) [Ni(CN)$_4$]$^{2-}$: \[ \text{Ni}^{2+}: 3d^8 \, (\text{low spin, 0 unpaired electrons}). \]
\[ \mu = \sqrt{0(0+2)} = 0.0 \, \text{B.M.} \, (\text{III}). \]
The correct matching is: \[ \text{(A)-(II), (B)-(IV), (C)-(I), (D)-(III)}. \]

Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
