1. | \(13.6\) eV | 2. | \(\dfrac{13.6} {2}\) eV |
3. | \(2 \times 13.6\) eV | 4. | \(10.2\) eV |
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
(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 |
(A) | \(VR\) | (B) | \(RE\) |
(C) | \(\large\frac VE\) | (D) | \(\large\frac R E\) |
1. | (A) and (B) only |
2. | (C) and (B) only |
3. | (C) only |
4. | (A) and (C) only |
1. | \(-3.4~\text{eV}\) | 2. | \(-6.8~\text{eV}\) |
3. | \(-10.2~\text{eV}\) | 4. | \(-13.6~\text{eV}\) |
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 |
Assertion (A): | \(n.\) | The magnetic moment of a hydrogen-like atom is higher when it is in a state of higher quantum number
Reason (R): | \(n.\) | The magnetic moment of hydrogen-like atom, as calculated from Bohr's theory, is directly proportional to the principal quantum number
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). |
1. | \(\dfrac he\) | 2. | \(\dfrac h{2e}\) |
3. | \(\dfrac {2h}e\) | 4. | \(\dfrac h{2\pi e}\) |