
| 1. | \(1\%\) | 2. | \(3\%\) | 
| 3. | \(4\%\) | 4. | \(5\%\) | 
 
| 1. | \(2 ~\text{NC}^{-1}\) | 2. | \(1~\text{NC}^{-1}\) | 
| 3. | \(0.5~\text{NC}^{-1}\) | 4. | zero | 
| 1. | fringe width decreases. | 
| 2. | fringe width increases. | 
| 3. | central bright fringe becomes dark. | 
| 4. | fringe width remains unaltered. | 
| 1. | \(\sqrt { \dfrac{T}{\rho g}}\) | 2. | \(\sqrt { \dfrac{2T}{\rho g}}\) | 
| 3. | \(\sqrt{\dfrac{2T\rho}{\pi g}}\) | 4. | \(\sqrt{\dfrac{2T} {\pi \rho g}}\) | 
| List-I | List-II | ||
| A. | \( \oint \vec{E} \cdot d \vec{A}=\dfrac{Q}{\varepsilon_0}\) | I. | Ampere-Maxwell's law | 
| B. | \( \oint \vec{B} \cdot d \vec{A}=0 \) | II. | Faraday's law | 
| C. | \( \oint \vec{E} \cdot d\vec{ l}=\dfrac{-d(\phi)}{d t} \) | III. | Gauss's law of electrostatics | 
| D. | \( \oint \vec{B} \cdot d\vec{l}=\mu_0 i_c+ \mu_0 \varepsilon_0 \dfrac{d\left(\phi_E\right)}{d t}\) | IV. | Gauss's law of magnetism | 
| 1. | A-III, B-IV, C-II, D-I | 2. | A-IV, B-III, C-II, D-I | 
| 3. | A-III, B-II, C-IV, D-I | 4. | A-IV, B-I, C-III, D-II | 
| List-I (Series) | List-II (Wave number in \(\text{cm}^{–1}\)) | ||
| A. | Balmer series | I. | \( R\left(\dfrac{1}{1^2}-\dfrac{1}{n^2}\right) \) | 
| B. | Lyman series | II. | \( R\left(\dfrac{1}{4^2}-\dfrac{1}{n^2}\right) \) | 
| C. | Brackett series | III. | \( R\left(\dfrac{1}{5^2}-\dfrac{1}{n^2}\right) \) | 
| D. | Pfund series | IV. | \( R\left(\dfrac{1}{2^2}-\dfrac{1}{n^2}\right)\) | 
| 1. | A-I, B-IV, C-III, D-II | 
| 2. | A-II, B-III, C-IV, D-I | 
| 3. | A-IV, B-I, C-II, D-III | 
| 4. | A-III, B-II, C-I, D-IV | 
| 1. | \(1~\text{atm}\) | 2. | \(2~\text{atm}\) | 
| 3. | \(3~\text{atm}\) | 4. | \(4~\text{atm}\) | 
| 1. | \(0.02~\text{mm}\) | 2. | \(0.05~\text{mm}\) | 
| 3. | \(0.10~\text{mm}\) | 4. | \(0.20~\text{mm}\) |