Syllabus topics (official RTMNU)
(A) MO theory
- LCAO approximation, wave equation for molecular orbitals.
- Difference between bonding and antibonding MO in terms of energy and electron density distribution curves, order of energy levels in MO.
- Molecular Orbital diagrams for homonuclear diatomic molecules of elements(with Z= 1 to 9) Concepts of nonbonding MO in HF molecule.
- Coulson’s MO diagram of CO and NO diatomic molecule.
(B) Noble gases
- Chemical properties of the noble gases, Chemistry of Xenon and Krypton, Preparation, properties and structures of xenon fluorides (XeF2, XeF4 and XeF6), structure and bonding in XeOF2, XeOF4 and XeO2F2.
(A) Molecular orbital (MO) theory
LCAO approximation and wave equation for MOs
- In a molecule, electrons occupy molecular orbitals spread over all the nuclei.
- MOs are formed by Linear Combination of Atomic Orbitals: ψMO = cAψA ± cBψB.
- Addition gives the bonding MO: ψb = ψA + ψB; subtraction gives the antibonding MO: ψa = ψA − ψB.
- Electron density: ψb² = ψA² + ψB² + 2ψAψB (extra density between nuclei); ψa² = ψA² + ψB² − 2ψAψB (less density, a node between nuclei).
- Conditions for combination: AOs of comparable energy, same symmetry about the bond axis, and good overlap.
- n atomic orbitals give n molecular orbitals.
Bonding vs antibonding MO
| Bonding MO | Antibonding MO |
|---|---|
| Constructive overlap (in-phase) | Destructive overlap (out of phase) |
| Lower energy than the AOs; stabilises | Higher energy than the AOs; destabilises |
| High electron density between nuclei | Nodal plane between nuclei; density pushed outside |
| Written σ, π | Written σ*, π* |
Electron density curve (density on y-axis, internuclear axis on x-axis): for the bonding MO the curve stays high between the two nuclei; for the antibonding MO it drops to zero at the midpoint.
Order of energy levels
- Up to N₂ (s–p mixing is strong): σ1s < σ*1s < σ2s < σ*2s < (π2px = π2py) < σ2pz < (π*2px = π*2py) < σ*2pz.
- For O₂ and F₂: σ2pz lies below π2px = π2py.
- Bond order = ½(Nb − Na). Unpaired electrons → paramagnetic.
Homonuclear diatomic molecules (Z = 1 to 9)
| Molecule | Electrons | Bond order | Magnetism |
|---|---|---|---|
| H₂ | 2 | 1 | diamagnetic |
| He₂ | 4 | 0 (does not exist) | — |
| Li₂ | 6 | 1 | diamagnetic |
| Be₂ | 8 | 0 (unstable) | — |
| B₂ | 10 | 1 | paramagnetic (2 unpaired in π2p) |
| C₂ | 12 | 2 | diamagnetic |
| N₂ | 14 | 3 | diamagnetic |
| O₂ | 16 | 2 | paramagnetic (2 unpaired in π*2p) |
| F₂ | 18 | 1 | diamagnetic |
O₂ configuration (valence): σ2s² σ*2s² σ2pz² π2px² π2py² π*2px¹ π*2py¹. MO theory explains paramagnetism of O₂, which VBT cannot.
Non-bonding MO in HF
- H 1s combines only with F 2pz (same symmetry along the bond axis, similar energy) to give σ and σ* MOs.
- F 2s (too low in energy) and F 2px, 2py (wrong symmetry) do not combine: they stay as non-bonding MOs, holding F’s three lone pairs.
- 8 valence electrons: 2 in σ, 6 in non-bonding MOs; bond order 1. σ MO lies closer to F, so the bond is polar (Hδ+–Fδ−).
Coulson’s MO diagram of CO and NO
- Heteronuclear: O is more electronegative, so its AOs are drawn lower in energy than those of C or N. The diagram is unsymmetrical.
- CO: 10 valence electrons, isoelectronic with N₂. Bond order = 3; diamagnetic. The highest filled MO (a σ orbital) is mainly on carbon, so CO donates its lone pair through carbon to metals (metal carbonyls).
- NO: 11 valence electrons; the extra electron goes into a π* MO. Bond order = (8 − 3)/2 = 2.5; paramagnetic (1 unpaired electron). Losing it gives NO⁺, bond order 3, shorter bond.
(B) Noble gases
Chemical properties
- Monatomic with stable ns²np⁶ configuration, very high ionisation energy and nearly zero electron affinity, so they are very unreactive.
- 1962: Bartlett made O₂⁺[PtF₆]⁻; noting that the IE of Xe (1170 kJ mol⁻¹) is close to that of O₂ (1175 kJ mol⁻¹), he made Xe⁺[PtF₆]⁻, the first noble gas compound.
- Only Kr, Xe and Rn form true compounds, mainly with the most electronegative elements F and O. Xe and Kr also form clathrates (trapped in ice or quinol cages).
Xenon fluorides: preparation
- Xe + F₂ (2 : 1 excess Xe), 400 °C, nickel vessel → XeF₂
- Xe + 2F₂ (1 : 5), 400 °C, about 6 atm → XeF₄
- Xe + 3F₂ (1 : 20), about 300 °C, 50–60 atm → XeF₆
Properties
- Colourless crystalline solids; strong fluorinating and oxidising agents.
- Hydrolysis: 2XeF₂ + 2H₂O → 2Xe + 4HF + O₂; 6XeF₄ + 12H₂O → 4Xe + 2XeO₃ + 24HF + 3O₂; XeF₆ + 3H₂O → XeO₃ + 6HF.
- Partial hydrolysis of XeF₆: XeF₆ + H₂O → XeOF₄ + 2HF; XeF₆ + 2H₂O → XeO₂F₂ + 4HF.
- Fluoride donors/acceptors: XeF₂ + PF₅ → [XeF]⁺[PF₆]⁻; XeF₆ + MF → M⁺[XeF₇]⁻ (M = Na, K, Rb, Cs).
Structures (VSEPR)
| Compound | Bond pairs + lone pairs | Hybridisation | Shape |
|---|---|---|---|
| XeF₂ | 2 + 3 | sp³d | Linear (lone pairs equatorial) |
| XeF₄ | 4 + 2 | sp³d² | Square planar |
| XeF₆ | 6 + 1 | sp³d³ | Distorted octahedral |
| XeOF₂ | 3 σ + 2 lone pairs (one Xe=O π bond) | sp³d | T-shaped |
| XeOF₄ | 5 σ + 1 lone pair (one Xe=O π bond) | sp³d² | Square pyramidal |
| XeO₂F₂ | 4 σ + 1 lone pair (two Xe=O π bonds) | sp³d | See-saw (F axial, O and lone pair equatorial) |
In the oxyfluorides the Xe=O π bonds are formed by d-orbitals of Xe (pπ–dπ) and do not change the shape.
Krypton
- KrF₂ is the main krypton compound: made by electric discharge through Kr and F₂ at very low temperature. Linear, sp³d, like XeF₂.
- Unstable at room temperature; a very powerful fluorinating agent. KrF₂ + SbF₅ → [KrF]⁺[SbF₆]⁻.
Likely exam questions
Long answer
- Explain the LCAO approximation. Draw the MO diagram of O₂ and N₂ and explain their bond order and magnetic nature.
- How are XeF₂, XeF₄ and XeF₆ prepared? Discuss their structures on the basis of hybridisation.
Short answer
- Distinguish between bonding and antibonding molecular orbitals.
- Explain the concept of non-bonding MO with reference to HF.
- Give the structures of XeOF₂, XeOF₄ and XeO₂F₂.