(I). | \( |\Psi|^2 \) is known as a probability density. |
(II). | The Schrödinger equation can be easily solved for a multi-electron atom. |
(III). | \( \Psi\) for an electron in an atom. | An atomic orbital is the wave function
List-I (quantum number) |
List-II (Orbital) |
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(A) | n = 2, \(\ell\) = 1 | (I) | 2s |
(B) | n = 3, \(\ell\) = 2 | (II) | 3s |
(C) | n = 3, \(\ell\) = 0 | (III) | 2p |
(D) | n = 2, \(\ell\) = 0 | (IV) | 3d |
(A) | (B) | (C) | (D) | |
1. | (III) | (IV) | (I) | (II) |
2. | (IV) | (III) | (I) | (II) |
3. | (IV) | (III) | (II) | (I) |
4. | (III) | (IV) | (II) | (I) |
1. | \({{1.196\times 10^{8}}\over{\lambda}}\) | 2. | \({{2.859\times 10^{5}}\over{\lambda}}\) |
3. | \({{2.859\times 10^{16}}\over{\lambda}}\) | 4. | \({{1.196\times 10^{16}}\over{\lambda}}\) |
(i). | n (principal quantum number) can have values 1, 2, 3, 4, ....... |
(ii). | The number of orbitals for a given value of l is (2l+1). |
(iii). | The value of spin quantum numbers is always \(\pm\frac12\). |
(iv). | For l=5, the total number of orbitals is 9. |
Assertion (A): | \(ns^2\). | Helium and berylium having the similar outer electronic configuration of type
Reason (R): | Both are chemically inert. |
1. | Both (A) and (R) are True and (R) is the correct explanation of (A). |
2. | Both (A) and (R) are True but (R) is not the correct explanation of (A). |
3. | (A) is True but (R) is False. |
4. | Both (A) and (R) are False. |