The Tale of Two Systems
Imagine you are looking at the simplest atom in the universe: Hydrogen. It has just one proton and one electron. Because there is only one electron, there is absolutely no electron-electron repulsion.
In this single-electron utopia, the energy of an electron depends solely on its principal quantum number, n. It doesn't care about the shape of the orbital, whether it's s, p, or d. If they share the same shell, they share the same energy.
But what happens when we add an extra electron to create the H− ion? Everything changes.
Suddenly, we have two electrons repelling each other. This electron-electron repulsion shatters the perfect symmetry. The energy now depends on both the principal quantum number n and the azimuthal quantum number l. This is the multi-electron reality, governed by the (n+l) rule.
The Hydrogen Atom
A Single-Electron Utopia
Let's first map out the energy levels of the neutral Hydrogen atom.
The ground state is simply n=1, which contains the 1s orbital.
When the electron gets excited, it moves to the first excited state, which is the entire n=2 shell. Because energy only depends on n, the 2s and 2p subshells have the exact same energy.
Moving up again, the second excited state is the n=3 shell. This shell contains the 3s, 3p, and 3d subshells, all sitting at the exact same energy level.
Degeneracy is simply the number of orbitals that share the same energy. For the second excited state (n=3) of Hydrogen, we have one 3s orbital, three 3p orbitals, and five 3d orbitals.
Adding them up: 1+3+5=9. This perfectly matches the degeneracy of 9 given in the question!
The H- Ion
The Multi-Electron Reality
Now, let's shift our focus to the H− ion. Because it is a multi-electron system, the subshells within the same shell split in energy.
Following the
(n+l) rule (Aufbau principle), the energy order becomes:
1s<2s<2p<3s<3p<…
The ground state is the lowest energy level, which is the 1s subshell.
The first excited state is the next available energy level, which is strictly the 2s subshell.
And the second excited state? It is the next level up, which is the 2p subshell. Notice how different this is from the neutral Hydrogen atom!
Finding the Degeneracy
We have successfully identified that the second excited state of the H− ion is the 2p subshell.
The question asks for the degeneracy of this state, specifically instructing us not to consider electronic spin.
The 2p subshell consists of exactly three orbitals: px, py, and pz.
Since these three orbitals share the exact same energy, the degeneracy is simply 3.
The Final Verdict and a Word of Caution
Our final answer is 3.
But let's think like a true JEE advanced student. What if the question hadn't explicitly said "not considering the electronic spin"?
If we had to consider spin, each of those three 2p orbitals could hold two electrons—one with spin up (+1/2) and one with spin down (−1/2).
In that scenario, the degeneracy would double, becoming 3×2=6.
This is a classic trap! Always read the question carefully to see if spin is included or excluded. Great job navigating through this conceptual nuance!