Introduction
The quantum mechanical model, developed by Schrödinger, Heisenberg, and others in the 1920s, replaced Bohr’s model with a more accurate description of atomic structure based on probability rather than definite orbits.
Schrödinger Wave Equation
The Equation
$$\hat{H}\psi = E\psi$$or in full form for a hydrogen atom:
$$\frac{\partial^2 \psi}{\partial x^2} + \frac{\partial^2 \psi}{\partial y^2} + \frac{\partial^2 \psi}{\partial z^2} + \frac{8\pi^2 m}{h^2}(E - V)\psi = 0$$where:
- $\psi$ = wave function
- $E$ = total energy
- $V$ = potential energy
- $\hat{H}$ = Hamiltonian operator
Wave Function (ψ)
Physical Meaning
The wave function $\psi$ itself has no direct physical meaning, but:
$$|\psi|^2 = \text{Probability density}$$This gives the probability of finding an electron at a given point.
Key Properties
- $\psi$ must be single-valued (one value at each point)
- $\psi$ must be continuous (no breaks)
- $\psi$ must be finite (no infinite values)
- Total probability must equal 1: $\int |\psi|^2 dV = 1$
Orbitals vs Orbits
| Bohr’s Orbit | Quantum Orbital |
|---|---|
| Definite circular path | 3D region of probability |
| Electron has fixed position | Electron has probability distribution |
| 2D picture | 3D wave function |
Quantum Numbers
Four quantum numbers completely describe an electron’s state:
graph TD
A[Quantum Numbers] --> B["n: Principal
Shell, Size, Energy"]
A --> C["l: Azimuthal
Subshell, Shape"]
A --> D["mₗ: Magnetic
Orbital orientation"]
A --> E["mₛ: Spin
Electron spin"]1. Principal Quantum Number (n)
Definition
Describes the shell and determines the size and energy of the orbital.
Allowed Values
$$n = 1, 2, 3, 4, ... \text{ (positive integers)}$$Significance
| n | Shell | Max electrons (2n²) |
|---|---|---|
| 1 | K | 2 |
| 2 | L | 8 |
| 3 | M | 18 |
| 4 | N | 32 |
- Energy: $E \propto -\frac{1}{n^2}$ (for H-like atoms)
- Size: $r \propto n^2$
2. Azimuthal/Angular Momentum Quantum Number (l)
Definition
Describes the subshell and determines the shape of the orbital.
Allowed Values
$$l = 0, 1, 2, ..., (n-1)$$For each n, there are n possible values of l.
Subshell Notation
| l | Subshell | Shape | Number of orbitals |
|---|---|---|---|
| 0 | s | Spherical | 1 |
| 1 | p | Dumbbell | 3 |
| 2 | d | Double dumbbell | 5 |
| 3 | f | Complex | 7 |
Angular Momentum
$$L = \sqrt{l(l+1)} \cdot \frac{h}{2\pi}$$- n=1: only 1s (l=0)
- n=2: 2s, 2p (l=0,1)
- n=3: 3s, 3p, 3d (l=0,1,2)
- n=4: 4s, 4p, 4d, 4f (l=0,1,2,3)
No 1p, 2d, 3f etc.!
3. Magnetic Quantum Number (mₗ)
Definition
Describes the orientation of the orbital in space.
Allowed Values
$$m_l = -l, -(l-1), ..., 0, ..., (l-1), +l$$Total values = (2l + 1)
Examples
| Subshell | l | mₗ values | Number of orbitals |
|---|---|---|---|
| s | 0 | 0 | 1 |
| p | 1 | -1, 0, +1 | 3 |
| d | 2 | -2, -1, 0, +1, +2 | 5 |
| f | 3 | -3, -2, -1, 0, +1, +2, +3 | 7 |
Interactive Demo: Visualize 3D Orbital Shapes
Explore the shapes of s, p, d, and f orbitals in three dimensions.
4. Spin Quantum Number (mₛ)
Definition
Describes the intrinsic angular momentum (spin) of the electron.
Allowed Values
$$m_s = +\frac{1}{2} \text{ or } -\frac{1}{2}$$- $+\frac{1}{2}$: spin up (↑)
- $-\frac{1}{2}$: spin down (↓)
Spin Angular Momentum
$$S = \sqrt{s(s+1)} \cdot \frac{h}{2\pi} = \sqrt{\frac{3}{4}} \cdot \frac{h}{2\pi}$$Summary Table
| Quantum Number | Symbol | Values | Determines |
|---|---|---|---|
| Principal | n | 1, 2, 3, … | Shell, size, energy |
| Azimuthal | l | 0 to (n-1) | Subshell, shape |
| Magnetic | mₗ | -l to +l | Orbital orientation |
| Spin | mₛ | ±½ | Electron spin |
Counting Electrons
Maximum Electrons
- In an orbital: 2 (opposite spins)
- In a subshell: 2(2l + 1)
- In a shell: 2n²
| Shell | Subshells | Total orbitals | Max electrons |
|---|---|---|---|
| K (n=1) | 1s | 1 | 2 |
| L (n=2) | 2s, 2p | 1+3=4 | 8 |
| M (n=3) | 3s, 3p, 3d | 1+3+5=9 | 18 |
| N (n=4) | 4s, 4p, 4d, 4f | 1+3+5+7=16 | 32 |
Quantum Number Problems
Example 1: Valid Set
Problem: Which set is valid? (n, l, mₗ, mₛ) a) (2, 2, 0, +½) b) (3, 2, -2, -½) c) (2, 1, 2, +½)
Solution:
- a) Invalid: l cannot equal n (l must be < n)
- b) Valid: n=3, l=2 (d subshell), mₗ=-2 (allowed for l=2), mₛ=-½ (correct)
- c) Invalid: mₗ=2 not allowed when l=1 (range is -1 to +1)
Example 2: Electron Count
Problem: How many electrons in an atom can have n=3, l=2?
Solution: n=3, l=2 → 3d subshell Number of orbitals = 2(2)+1 = 5 Maximum electrons = 5 × 2 = 10
Example 3: Possible Sets
Problem: How many possible sets of quantum numbers exist for n=2?
Solution: For n=2: l = 0, 1
| l | mₗ | mₛ | Total |
|---|---|---|---|
| 0 | 0 | ±½ | 2 |
| 1 | -1, 0, +1 | ±½ each | 6 |
Total = 8 (which equals 2n² = 2×4 = 8, correct!)
Key Points for JEE
- l is always less than n
- mₗ ranges from -l to +l
- Each orbital holds maximum 2 electrons
- No two electrons can have all four quantum numbers same (Pauli)
- Number of orbitals in a subshell = 2l + 1
- Number of orbitals in a shell = n²
Practice Problems
Write all possible sets of quantum numbers for 3p electrons.
An electron has quantum numbers n=4, l=2. What are the possible values of mₗ?
How many orbitals in an atom can have n=4 and mₗ=0?