CSIR-NET Chemical Bonding Theories Compared — VBT, MOT, CFT and LFT
A large family of CSIR-NET inorganic questions is not really asking you to calculate anything. It is asking which theory accounts for a given observation — and, just as often, which theory cannot. If you know that valence bond theory has nothing to say about colour, or that crystal field theory cannot explain why neutral CO sits at the strong-field end of the spectrochemical series, you can eliminate two options before doing any work. This article puts the four theories side by side, works the numbers each one actually produces, and states plainly where each one breaks.
The four theories in one table
| Theory | Core picture | Explains well | Fails at |
|---|---|---|---|
| Valence bond theory (VBT) | Hybridised metal orbitals overlap with filled ligand orbitals; the bond is a localised electron pair | Geometry, hybridisation, magnetic moment (inner vs outer orbital complexes) | Colour, spectra, the magnitude of splitting, temperature dependence of magnetism |
| Molecular orbital theory (MOT) | Atomic orbitals combine into delocalised molecular orbitals over the whole species | Bond order, paramagnetism of O2, bonding in odd-electron species, spectra | Requires more work; simple diagrams assume symmetry that real molecules may not have |
| Crystal field theory (CFT) | Ligands are point negative charges; the d orbitals split purely electrostatically | Splitting patterns, high/low spin, CFSE, colour, Jahn–Teller distortion | Spectrochemical order, nephelauxetic effect, π-bonding, charge-transfer bands |
| Ligand field theory (LFT) | CFT corrected by real orbital overlap — an MO treatment of the complex | Everything CFT does, plus the spectrochemical series, backbonding, covalency | Heaviest to apply by hand; needs symmetry labels and interaction diagrams |
Valence bond theory — what it still gets right
VBT survives in NET papers because it answers one question quickly: is the complex inner-orbital (using (n−1)d orbitals) or outer-orbital (using nd orbitals)? That single choice fixes the hybridisation and the number of unpaired electrons.
Worked example 1 — two cobalt(III) complexes. Co is Z = 27, so Co3+ is [Ar]3d6: six d electrons.
[Co(NH3)6]3+: ammonia forces pairing, so the six d electrons occupy three 3d orbitals as three pairs. Two 3d orbitals are freed, giving d2sp3 hybridisation — an inner-orbital octahedral complex with zero unpaired electrons, diamagnetic.
[CoF6]3−: fluoride does not force pairing, so the 3d level keeps four unpaired electrons (t2g4eg2 in field language). The metal must use 4d orbitals: sp3d2, an outer-orbital complex with four unpaired electrons.
Spin-only moment for the second: μ = √(n(n+2)) = √(4 × 6) = √24 = 4.90 BM. (Check the arithmetic: 4 × 6 = 24, and 4.92 = 24.01, so √24 = 4.899 ≈ 4.90.)
Notice what VBT never told us: both complexes are coloured, and their colours differ. VBT has no orbital-energy gap in it, so it cannot produce an absorption wavelength at all. That is the standard "which theory fails" answer.
Molecular orbital theory — bond order is the deliverable
For second-row diatomics the filling order depends on s–p mixing, and this is the single most common slip in NET answers:
- B2, C2, N2 (Z ≤ 7): s–p mixing is strong, so the π2p pair lies below σ2pz.
- O2, F2, Ne2 (Z > 7): mixing is weak, so σ2pz lies below the π2p pair.
Worked example 2 — O2, N2 and NO.
O2 has 8 + 8 = 16 electrons. Filling σ1s2 σ*1s2 σ2s2 σ*2s2 σ2pz2 π2px2 π2py2 π*2px1 π*2py1 uses all 16. Bonding electrons = 2 + 2 + 2 + 2 + 2 = 10; antibonding = 2 + 2 + 1 + 1 = 6. Bond order = (10 − 6)/2 = 2, with two unpaired electrons — O2 is paramagnetic. No Lewis structure predicts this; MOT does it in one line.
N2 has 14 electrons; the π orbitals fill before σ2p. Bonding = 10, antibonding = 4, bond order = (10 − 4)/2 = 3, diamagnetic.
NO has 7 + 8 = 15 electrons — one more than N2, and it goes into a π* orbital. Bonding = 10, antibonding = 5, bond order = (10 − 5)/2 = 2.5. Removing that electron gives NO+ with bond order 3, which is why NO+ has a shorter, stronger bond than NO — a favourite two-species comparison.
Crystal field theory — where the arithmetic lives
CFT replaces the ligands by point charges. In an octahedral field the five d orbitals split into a lower t2g set (three orbitals, −0.4Δo each) and an upper eg set (two orbitals, +0.6Δo each). The centre of gravity is preserved: 3(−0.4) + 2(+0.6) = −1.2 + 1.2 = 0.
Here P is the mean pairing energy. Low spin is favoured when Δo > P; high spin when Δo < P.
Worked example 3 — d6 iron(II), both spin states.
[Fe(H2O)6]2+, high spin: t2g4eg2. CFSE = (−0.4 × 4) + (0.6 × 2) = −1.6 + 1.2 = −0.4 Δo, with 4 unpaired electrons, μ = √(4 × 6) = 4.90 BM.
[Fe(CN)6]4−, low spin: t2g6eg0. CFSE = (−0.4 × 6) + (0.6 × 0) = −2.4 Δo, diamagnetic. Relative to the free ion the low-spin case has formed two extra pairs, so the honest comparison is −2.4Δo + 2P against −0.4Δo; low spin wins only when 2Δo > 2P, i.e. Δo > P.
Tetrahedral fields invert the pattern — the e set (two orbitals) lies below the t2 set (three orbitals) — and the splitting is smaller, Δt ≈ (4/9)Δo. That single factor is why tetrahedral complexes of the first transition series are almost always high spin.
Worked example 4 — CFSE of a tetrahedral d3 ion.
Filling is e2t21; the e orbitals are at −0.6Δt
and t2 at +0.4Δt.
CFSE = (−0.6 × 2) + (0.4 × 1) = −1.2 + 0.4 = −0.8 Δt.
Expressed in octahedral units this is −0.8 × (4/9)Δo = −0.356Δo,
much less stabilisation than the octahedral d3 value of
(−0.4 × 3) = −1.2Δo. This is exactly why d3 ions such as
Cr3+ so strongly prefer octahedral geometry.
Where CFT breaks, and what LFT adds
CFT treats ligands as bare negative charges. If that were true, the spectrochemical series should follow charge and size. It does not. The observed order runs roughly
Neutral CO outranks the anions, and iodide — the largest, softest anion — sits at the weak end. A point-charge model cannot produce this. Ligand field theory can, because it treats the metal–ligand interaction as real orbital overlap:
- π-donor ligands (halides, OH−) have filled p orbitals that interact with the metal t2g set and push it up, shrinking Δo — weak field.
- Pure σ-donors (NH3, en) leave t2g essentially non-bonding — intermediate field.
- π-acceptor ligands (CN−, CO, NO) have empty π* orbitals that accept t2g electron density and pull it down, enlarging Δo — strong field. This is backbonding, and it is invisible to CFT.
LFT also accounts for the nephelauxetic effect: the Racah parameter B measured in a complex is smaller than in the free ion, because the d electrons are spread onto the ligands. A purely electrostatic model has no mechanism for that at all, so the nephelauxetic ratio β = Bcomplex/Bfree ion being less than 1 is direct evidence of covalency. Charge-transfer bands — intense LMCT and MLCT absorptions such as the deep colour of MnO4−, where the metal is d0 and can have no d–d transition at all — are the other standard proof.
Choosing the right theory in the exam
| The question asks about… | Reach for |
|---|---|
| Shape, hybridisation, inner/outer orbital | VBT |
| Bond order, bond length or strength trend in a diatomic | MOT |
| Paramagnetism of O2, stability of O2+/O2− | MOT |
| High spin vs low spin, μspin-only, CFSE, Jahn–Teller | CFT |
| Colour of a dn complex, Δo from λmax | CFT (Tanabe–Sugano for detail) |
| Spectrochemical order, backbonding, ν(CO) shifts, nephelauxetic effect | LFT / MO treatment |
| Intense colour of a d0 or d10 species | Charge transfer — LFT, never d–d |
Mistakes that cost marks
- Using the wrong MO order. Putting σ2p below π2p for N2 gives the right bond order by luck but the wrong HOMO, and every photoelectron-spectrum question then fails. Remember the switch happens after nitrogen.
- Counting d electrons from the neutral atom. The d count belongs to the ion. Co3+ is d6, not d7; Fe3+ is d5, not d6. Strip the 4s electrons first, then the required number of 3d.
- Comparing CFSE without pairing energy. −2.4Δo looks better than −0.4Δo until you add the 2P cost of the extra pairs. Only the full comparison decides the spin state.
- Explaining colour with VBT. VBT contains no energy gap; any answer that uses it to justify an absorption band is wrong on principle.
- Assuming Δt = (4/9)Δo is exact. It is a point-charge estimate for identical metal, ligands and bond length. Treat it as a working approximation and say so.
- Calling a strong-field ligand a strong base. CN− and CO sit at the top of the spectrochemical series for π-acceptor reasons, not Brønsted basicity — CO is a very poor base.
Where this appears in the paper
| Exam | Typical use of these theories |
|---|---|
| CSIR-NET Chemical Sciences | Part B and Part C inorganic: spin state, μ, CFSE ordering, spectrochemical reasoning, "which theory explains" items |
| GATE Chemistry | Bond order of diatomics and ions, magnetic moments, MO energy ordering |
| IIT-JAM / CUET-PG | Hybridisation and geometry, high vs low spin, basic MO diagrams |
| MSc coursework | Full LFT treatment, Tanabe–Sugano diagrams, nephelauxetic series |
Part A, Part B and Part C are the three sections of the CSIR-NET paper; for the current marking scheme, number of questions and negative-marking rules, always read the official notification for your session rather than any coaching summary, including this one.
The arithmetic here is short but unforgiving. CFSE sums, spin-only moments and bond orders are all a handful of multiplications, and the marks are lost to slips rather than to theory. Work each one on paper and then recompute it independently — the suite's scientific calculator is enough for that. There is no dedicated bonding-theory tool in the suite, so this button honestly opens the suite itself rather than pretending a matching calculator exists.
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