1. | \(13.6\) eV | 2. | \(\dfrac{13.6} {2}\) eV |
3. | \(2 \times 13.6\) eV | 4. | \(10.2\) eV |
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1. | \(\mathrm{Li}^{2+}\) ions in \(n=2\) state. | Some radiation is absorbed by
2. | \(\mathrm{Li}^{2+}\) ions in \(n=3\) state. | Some radiation is absorbed by
3. | \(\mathrm{Li}^{2+}\) ions in \(n=1\) state. | Some radiations is absorbed by
4. | \(\mathrm{Li}^{2+}\) ions. | None of the radiation is absorbed by
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1. | \(13.6~\text{eV}\) |
2. | \(\dfrac{13.6} {2}~\text{eV}\) |
3. | \(13.6×\left(\dfrac{3}{4}\right)~\text{eV}\) |
4. | \(13.6×\left(\dfrac14-\dfrac19\right)~\text{eV}\) |
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(I) | \(E_K<E_L\) |
(II) | \(E_L>E_M\) |
(III) | \(E_L -E_K=E_{K\alpha}\), the energy of \(K_\alpha \) photon |
1. | (I) is true | 2. | (I), (III) are true |
3. | (II) is true | 4. | (I), (II) are true |
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Assertion (A): | When light consisting of wavelengths corresponding to the Balmer series is incident on a gas containing \(\mathrm{He}^{+}\) ions in the first three excited states - it can be absorbed by the \(\mathrm{He}^{+}\) ions. |
Reason (R): | All the energy levels of the \(\mathrm{He}^{+}\) ions are the same as those of the \(\mathrm{H}\) atoms. |
1. | (A) is True but (R) is False. |
2. | (A) is False but (R) is True. |
3. | Both (A) and (R) are True and (R) is the correct explanation of (A). |
4. | Both (A) and (R) are True but (R) is not the correct explanation of (A). |
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1. | \(-3.4~\text{eV}\) | 2. | \(-6.8~\text{eV}\) |
3. | \(-10.2~\text{eV}\) | 4. | \(-13.6~\text{eV}\) |
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1. | \(n=2\) state of \(\mathrm{He}^{+}\) \(\left(Z=2\right)\) ion |
2. | \(n=4\) state of \(\mathrm{He}^{+}\) \(\left(Z=2\right)\) ion |
3. | \(n=2\) state of \(\mathrm{Be}^{3+}\)\(\left(Z=4\right)\) ion |
4. | \(n=3\) state of \(\mathrm{Li}^{2+}\) \(\left(Z=3\right)\) ion |
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1. | the same phase. |
2. | the same energy. |
3. | the same direction. |
4. | the same phase, energy, and direction. |
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1. | 2 possible energy values. |
2. | 3 possible energy values. |
3. | 4 possible energy values. |
4. | 5 possible energy values. |
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