List-I (Application of Gauss Law) |
List-II (Value of \(|E|\)) |
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A | Field inside thin shell | I | \( \frac{\lambda}{2 \pi \varepsilon_0 r} \hat{n} \) |
B | Field outside thin shell | II | \( \frac{q}{4 \pi \varepsilon_0 R^2} \hat{r} \) |
C | Field of thin shell at the surface | III | \( \frac{q}{4 \pi \varepsilon_0 r^2} \hat{r}\) |
D | Field due to long charged wire | IV | zero |
1. | fringe width decreases. |
2. | fringe width increases. |
3. | central bright fringe becomes dark. |
4. | fringe width remains unaltered. |
List I | List II | ||
A | \( \oint \vec{E} \cdot d \vec{A}=\frac{Q}{\varepsilon_0}\) | I | Ampere-Maxwell's Law |
B | \( \oint \vec{B} \cdot d \vec{A}=0 \) | II | Faraday's Law |
C | \( \oint \vec{E} \cdot \overrightarrow{d I}=\frac{-d(\phi)}{d t} \) | III | Gauss Law of electrostatics |
D | \( \oint \vec{B} \cdot \overrightarrow{d l}=\mu_0 i_c+ \mu_0 \varepsilon_0 \frac{d\left(\phi_E\right)}{d t}\) | IV | Gauss law of magnetism |
List-I (Measured values) |
List-II (Significant figures) |
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A | \(0.001213\) | I | \(2\) |
B | \(2.1 \times 10^{16} \) | II | \(3\) |
C | \(3.70\) | III | \(1\) |
D | \(3000\) | IV | \(4\) |
1. | A-III, B-II, C-I, D-IV |
2. | A-III, B-I, CII, D-IV |
3. | A-I, B-II, C-IV, D-III |
4. | A-IV, B-I, C-II, D-III |
List-I (Series) |
List-II (Wave number in cm-1) |
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A. | Balmer series | I. | \( R\left(\frac{1}{1^2}-\frac{1}{n^2}\right) \) |
B. | Lyman series | II. | \( R\left(\frac{1}{4^2}-\frac{1}{n^2}\right) \) |
C. | Brackett series | III. | \( R\left(\frac{1}{5^2}-\frac{1}{n^2}\right) \) |
D. | Pfund series | IV. | \( R\left(\frac{1}{2^2}-\frac{1}{n^2}\right)\) |