Why MOT? The Theory That Explains O₂

Valence Bond Theory gave us bonds and shapes, but it stumbled on one stubborn fact: liquid oxygen is attracted to a magnet — it is paramagnetic, meaning it has unpaired electrons. The Lewis structure O=OO=O shows everything paired. Molecular Orbital Theory (MOT), developed by Hund and Mulliken, finally explains this.

Core idea: When atoms combine, their atomic orbitals merge to form new molecular orbitals (MOs) that belong to the whole molecule, not to individual atoms. Electrons then fill these MOs following the same rules as atomic orbitals (Aufbau, Pauli, Hund).

Formation of MOs (LCAO)

Molecular orbitals are formed by the Linear Combination of Atomic Orbitals (LCAO). Two atomic orbitals combine in two ways:

  • Constructive (additive) combination → bonding MO (lower energy, electron density between nuclei). Denoted σ\sigma, π\pi.
  • Destructive (subtractive) combination → antibonding MO (higher energy, a node between nuclei). Denoted σ\sigma^*, π\pi^*.

Key Point: NN atomic orbitals always produce NN molecular orbitals — half bonding, half antibonding. A bonding MO is more stable (lower energy) than the atomic orbitals; an antibonding MO is less stable (higher energy).

[JEE Tip] Bonding MO = electrons help hold the molecule together; antibonding MO (the starred ones) = electrons work against bonding.

Energy Ordering of Molecular Orbitals

Electrons fill MOs from lowest to highest energy. There are two orderings, depending on the molecule.

For O2O_2, F2F_2, Ne2Ne_2 (and heavier):

σ1s<σ1s<σ2s<σ2s<σ2pz<(π2px=π2py)<(π2px=π2py)<σ2pz\sigma 1s < \sigma^* 1s < \sigma 2s < \sigma^* 2s < \sigma 2p_z < (\pi 2p_x = \pi 2p_y) < (\pi^* 2p_x = \pi^* 2p_y) < \sigma^* 2p_z

For Li2Li_2, Be2Be_2, B2B_2, C2C_2, N2N_2 (lighter than O2O_2):

Due to s-p mixing, the σ2pz\sigma 2p_z rises above the two π2p\pi 2p orbitals: σ1s<σ1s<σ2s<σ2s<(π2px=π2py)<σ2pz<(π2px=π2py)<σ2pz\sigma 1s < \sigma^* 1s < \sigma 2s < \sigma^* 2s < (\pi 2p_x = \pi 2p_y) < \sigma 2p_z < (\pi^* 2p_x = \pi^* 2p_y) < \sigma^* 2p_z

Key Point: The ONLY difference is the relative order of σ2pz\sigma 2p_z and the π2p\pi 2p pair. Up to and including N2N_2, the π orbitals fill first; from O2O_2 onward, σ2pz\sigma 2p_z fills first.

[NEET Important] Remember the cutoff: 'till N2N_2, π is below σ2pz; from O2O_2, σ2pz is below π'. This is the single most error-prone point in MOT.

Bond Order, Stability & Magnetism

The most useful number MOT gives us is the bond order.

Definition: Bond order=12(NbNa)\text{Bond order} = \frac{1}{2}\,(N_b - N_a) where NbN_b = number of electrons in bonding MOs and NaN_a = number in antibonding MOs.

What bond order tells us:

  • Bond order > 0 → the molecule/ion exists and is stable. Bond order = 0 → it does not exist (e.g. He2He_2).
  • Higher bond order → shorter bond, greater bond enthalpy, more stable molecule.
  • It can be fractional (e.g. O2+O_2^+ has bond order 2.5).

Magnetic behaviour

  • All electrons paired → diamagnetic (weakly repelled by a magnet).
  • One or more unpaired electrons → paramagnetic (attracted by a magnet); more unpaired electrons → stronger paramagnetism.

Key Point: MOT's triumph — O2O_2 has two unpaired electrons in its π2p\pi^* 2p orbitals, so it is paramagnetic. This is the fact VBT could never explain.

[JEE Tip] Always write the full MO configuration, then read off both bond order and the number of unpaired electrons (for magnetism).

MO Configurations of Key Diatomics

Let's build the important ones. (Core σ1s\sigma 1s, σ1s\sigma^*1s are filled for second-period; we show valence MOs.)

Hydrogen H2H_2 (2 e⁻)

σ1s2\sigma 1s^2. Bond order =12(20)=1= \tfrac{1}{2}(2-0) = 1. Diamagnetic. Stable.

Helium He2He_2 (4 e⁻)

σ1s2σ1s2\sigma 1s^2\,\sigma^*1s^2. Bond order =12(22)=0= \tfrac{1}{2}(2-2) = 0. Does not exist.

Nitrogen N2N_2 (14 e⁻)

KKσ2s2σ2s2π2px2π2py2σ2pz2KK\,\sigma 2s^2\,\sigma^*2s^2\,\pi 2p_x^2\,\pi 2p_y^2\,\sigma 2p_z^2. Nb=8,Na=2N_b=8, N_a=2. Bond order =12(82)=3= \tfrac{1}{2}(8-2) = 3. Diamagnetic.

Oxygen O2O_2 (16 e⁻)

KKσ2s2σ2s2σ2pz2π2px2π2py2π2px1π2py1KK\,\sigma 2s^2\,\sigma^*2s^2\,\sigma 2p_z^2\,\pi 2p_x^2\,\pi 2p_y^2\,\pi^*2p_x^1\,\pi^*2p_y^1. Nb=8,Na=4N_b=8, N_a=4. Bond order =12(84)=2= \tfrac{1}{2}(8-4) = 2. Paramagnetic (2 unpaired in π*).

Fluorine F2F_2 (18 e⁻)

Fills both π\pi^* completely. Bond order =12(86)=1= \tfrac{1}{2}(8-6) = 1. Diamagnetic.

Oxygen-family ions

  • O2+O_2^+ (15 e⁻): bond order 2.52.5, paramagnetic.
  • O2O_2^- (17 e⁻): bond order 1.51.5, paramagnetic.
  • O22O_2^{2-} (18 e⁻): bond order 11, diamagnetic. Stability/bond-length order: O2+>O2>O2>O22O_2^+ > O_2 > O_2^- > O_2^{2-}.

[NEET Important] B2B_2 and O2O_2 are both paramagnetic; C2C_2 and N2N_2 are diamagnetic. These four are exam favourites.

Molecular orbital diagram of paramagnetic O2

Diatomic molecules: bond order and magnetism

Solved Examples

Example 1: Bond order of N₂

Calculate the bond order of N2N_2 (14 electrons).

Solution:

  1. Configuration: bonding electrons Nb=8N_b = 8 (σ2s, π2p×2, σ2pz), antibonding Na=2N_a = 2 (σ*2s).
  2. Formula: bond order =12(NbNa)= \tfrac{1}{2}(N_b - N_a).
  3. Compute: 12(82)=3\tfrac{1}{2}(8 - 2) = 3.

Takeaway: N2N_2 has bond order 3, consistent with its triple bond and high stability.

Example 2: Why O₂ is paramagnetic

Use MOT to explain the paramagnetism of O2O_2.

Solution:

  1. 16 electrons fill up to the π2p\pi^*2p orbitals.
  2. The last two electrons go singly into the two degenerate π2px\pi^*2p_x and π2py\pi^*2p_y orbitals (Hund's rule).
  3. Two unpaired electronsO2O_2 is paramagnetic.

Takeaway: The two unpaired electrons in the antibonding π* orbitals make O2O_2 paramagnetic — MOT's signature success.

Example 3: Existence of He₂

Does the He2He_2 molecule exist? Justify with bond order.

Solution:

  1. 4 electrons: σ1s2σ1s2\sigma 1s^2\,\sigma^*1s^2.
  2. Nb=2,Na=2N_b = 2, N_a = 2.
  3. Bond order =12(22)=0= \tfrac{1}{2}(2-2) = 0.
  4. Conclusion: zero bond order → no net bonding → He2He_2 does not exist.

Takeaway: Bond order 0 means the molecule is not formed.

Example 4: Bond order of O₂⁺

Find the bond order of the dioxygenyl cation O2+O_2^+ (15 electrons).

Solution:

  1. Remove 1 electron from O2O_2's π\pi^* orbital → 15 electrons.
  2. Nb=8,Na=3N_b = 8, N_a = 3.
  3. Bond order =12(83)=2.5= \tfrac{1}{2}(8-3) = 2.5.

Takeaway: Removing an antibonding electron increases bond order; O2+O_2^+ (2.5) is stronger than O2O_2 (2).

Example 5: Comparing O₂, O₂⁺, O₂⁻, O₂²⁻

Arrange these in increasing order of bond length.

Solution:

  1. Bond orders: O2+O_2^+ (2.5), O2O_2 (2.0), O2O_2^- (1.5), O22O_2^{2-} (1.0).
  2. Higher bond order → shorter bond.
  3. Increasing bond length: O2+<O2<O2<O22O_2^+ < O_2 < O_2^- < O_2^{2-}.

Takeaway: Bond length is inversely related to bond order across an isoelectronic-like series.

Example 6: Magnetic nature of B₂

Is B2B_2 (10 electrons) paramagnetic or diamagnetic?

Solution:

  1. For B₂ (lighter than O₂), π2p is below σ2pz.
  2. Configuration:σ2s2σ2s2π2px1π2py1\sigma 2s^2\,\sigma^*2s^2\,\pi 2p_x^1\,\pi 2p_y^1.
  3. The last two electrons go singly into the two degenerate π2p orbitals → 2 unpaired.
  4. Conclusion: B2B_2 is paramagnetic (bond order =12(64)=1= \tfrac{1}{2}(6-4) = 1).

Takeaway: The s-p mixing ordering makes B2B_2 paramagnetic — a classic JEE trap.

Example 7: Bond order of C₂

Calculate the bond order and magnetism of C2C_2 (12 electrons).

Solution:

  1. Ordering (lighter than O₂):σ2s2σ2s2π2px2π2py2\sigma 2s^2\,\sigma^*2s^2\,\pi 2p_x^2\,\pi 2p_y^2.
  2. Nb=6,Na=2N_b = 6, N_a = 2. Bond order =12(62)=2= \tfrac{1}{2}(6-2) = 2.
  3. All electrons paired → diamagnetic.

Takeaway: C2C_2 has bond order 2 and is diamagnetic (both π bonds, no σ2pz electrons).

Example 8: Bond order of F₂

Find the bond order of F2F_2 (18 electrons).

Solution:

  1. Configuration fills both π\pi^* completely: Nb=8,Na=6N_b = 8, N_a = 6.
  2. Bond order =12(86)=1= \tfrac{1}{2}(8-6) = 1.
  3. All paired → diamagnetic.

Takeaway: F2F_2 has a single bond (bond order 1), the weakest among N2N_2, O2O_2, F2F_2.

Example 9: Difference between bonding and antibonding MOs

State two differences between a bonding and an antibonding molecular orbital.

Solution:

  1. Energy: bonding MO is lower in energy than the parent atomic orbitals; antibonding MO is higher.
  2. Electron density: bonding MO has high density between the nuclei; antibonding MO has a node (zero density) between them.
  3. Effect: electrons in bonding MOs stabilise the molecule; in antibonding MOs they destabilise it.

Takeaway: Bonding MOs glue the molecule; antibonding (starred) MOs pull it apart.

Example 10: Why N₂ is more stable than N₂⁺

Compare the bond orders of N2N_2 and N2+N_2^+.

Solution:

  1. N2N_2 (14 e⁻): bond order 3.
  2. N2+N_2^+ (13 e⁻): remove one bonding electron (from σ2pz) → Nb=7,Na=2N_b = 7, N_a = 2 → bond order =12(72)=2.5= \tfrac{1}{2}(7-2) = 2.5.
  3. Conclusion: N2N_2 (3) > N2+N_2^+ (2.5), so N2N_2 is more stable with a shorter bond.

Takeaway: Removing a bonding electron lowers bond order and stability (contrast with O2+O_2^+).

Example 11: Number of unpaired electrons in O₂⁻

How many unpaired electrons are in the superoxide ion O2O_2^- (17 electrons)?

Solution:

  1. Add one electron to O2O_2's π\pi^* orbitals → 17 electrons.
  2. The π* orbitals now hold 3 electrons: one is paired, one remains unpaired.
  3. Conclusion: 1 unpaired electron → paramagnetic; bond order =12(85)=1.5= \tfrac{1}{2}(8-5) = 1.5.

Takeaway: O2O_2^- has bond order 1.5 and one unpaired electron (paramagnetic).

Example 12: Predicting whether Be₂ exists

Use MOT to decide if Be2Be_2 (8 electrons) exists.

Solution:

  1. Configuration: σ1s2σ1s2σ2s2σ2s2\sigma 1s^2\,\sigma^*1s^2\,\sigma 2s^2\,\sigma^*2s^2.
  2. Nb=4,Na=4N_b = 4, N_a = 4.
  3. Bond order =12(44)=0= \tfrac{1}{2}(4-4) = 0.
  4. Conclusion: like He2He_2, Be2Be_2 has zero bond order and does not exist as a stable molecule.

Takeaway: Filled bonding and antibonding pairs cancel → bond order 0 → no stable molecule.