આ MCQ મોડ્યુલ આના પર આધારિત છે: Vbt Cft
Vbt Cft
આ મૂલ્યાંકન આના પર આધારિત હશે: Vbt Cft
મૂલ્યાંકન બનાવવામાં તેમની સામગ્રી સામેલ કરવા ચિત્રો, PDF અથવા Word દસ્તાવેજ અપલોડ કરો.
Vbt Cft
5.6 Bonding in Coordination Compounds
Werner's theory captured the geometry, but it could not explain why only certain elements form complexes, why coordinate bonds are directional, or why complexes have characteristic colours and magnetic properties. Two complementary theories address these questions at the introductory level: Valence Bond Theory (VBT) and Crystal Field Theory (CFT). Beyond NCERT, ligand field theory and molecular orbital theory go further still.
5.6.1 Valence Bond Theory (VBT)
According to VBT, the metal ion provides a set of empty hybrid orbitals of definite geometry; each ligand donates a lone pair into one of these hybrid orbitals, forming a coordinate (dative) bond. The hybridisation depends on the coordination number and on whether inner-shell (n−1)d orbitals are used.
| CN | Hybridisation | Geometry | Examples |
|---|---|---|---|
| 4 | sp³ | Tetrahedral | [NiCl4]2−, [Ni(CO)4] |
| 4 | dsp² | Square planar | [Ni(CN)4]2−, [Pt(NH3)2Cl2] |
| 5 | sp³d | Trigonal bipyramidal | [Fe(CO)5] |
| 6 | d²sp³ (inner-orbital) | Octahedral | [Co(NH3)6]3+, [Fe(CN)6]3− |
| 6 | sp³d² (outer-orbital) | Octahedral | [CoF6]3−, [FeF6]3− |
Inner vs outer orbital octahedral complexes
For Co3+ (3d6), with strong-field ligands like NH3 the six 3d electrons pair up into the lower three 3d orbitals. The two now-empty 3d orbitals combine with 4s and 4p (giving d²sp³ hybridisation) — an inner-orbital (low-spin) complex with no unpaired electrons → diamagnetic, e.g. [Co(NH3)6]3+.
With weak-field ligands such as F−, electrons stay unpaired in 3d. The metal then uses the outer 4d orbitals: hybridisation sp³d² → outer-orbital (high-spin) complex with four unpaired electrons → paramagnetic, e.g. [CoF6]3−.
Magnetic properties from VBT
Magnetic moment is calculated from the number of unpaired electrons (n) using the spin-only formula:
\[ \mu_{\text{spin-only}} = \sqrt{n(n+2)} \;\; \text{Bohr Magneton (BM)} \]Examples (first transition series):
- n = 1 → μ = √3 ≈ 1.73 BM
- n = 2 → μ = √8 ≈ 2.83 BM
- n = 3 → μ = √15 ≈ 3.87 BM
- n = 4 → μ = √24 ≈ 4.90 BM
- n = 5 → μ = √35 ≈ 5.92 BM
Worked Example 5.7 — Geometry from magnetic moment
The spin-only magnetic moment of [MnBr4]2− is 5.9 BM. Predict the geometry.
μ = 5.9 BM ⇒ √n(n+2) = 5.9 ⇒ n = 5 unpaired electrons.
Square planar dsp² requires pairing of d-electrons (typical n = 1 or 0). Since five electrons remain unpaired, the geometry must be tetrahedral (sp³).
Limitations of VBT
- Built on assumptions; quantitative magnetic moment is not predicted exactly.
- Cannot explain colour of complexes.
- Cannot quantify thermodynamic or kinetic stability.
- Does not always predict whether 4-coordinate complexes are tetrahedral or square planar.
- Does not distinguish between weak- and strong-field ligands.
5.6.2 Crystal Field Theory (CFT)
CFT is purely electrostatic: ligands are treated as point negative charges (or point dipoles for neutral ligands) that perturb the energy of the metal's five d-orbitals. In an isolated ion all five d-orbitals are degenerate. A spherical field would raise them all equally. But a real ligand field is asymmetrical, and the d-orbitals split.
(a) Octahedral splitting — \(\Delta_o\)
In an octahedral complex six ligands lie along the ±x, ±y, ±z axes. The two d-orbitals that point along the axes (\(d_{x^2-y^2}\) and \(d_{z^2}\)) experience strong electrostatic repulsion and are destabilised — these are the eg set. The three orbitals that point between the axes (\(d_{xy}, d_{yz}, d_{xz}\)) are less repelled and are stabilised — these are the t2g set.
The energy gap is \(\Delta_o\) (the crystal-field splitting energy in an octahedral field). The barycentre rule gives:
\[ E(t_{2g}) = -\tfrac{2}{5}\Delta_o, \qquad E(e_g) = +\tfrac{3}{5}\Delta_o \](b) Filling d-orbitals: high spin vs low spin
For d¹, d², d³ ions the electrons occupy t2g singly (Hund's rule). For d4–d7 there are two competing options:
- If \(\Delta_o < P\) (pairing energy) → 4th electron enters eg, giving t2g3eg1 (high-spin, weak-field).
- If \(\Delta_o > P\) → 4th electron pairs in t2g, giving t2g4eg0 (low-spin, strong-field).
(c) Spectrochemical series
Ligands ranked by the magnitude of \(\Delta_o\) they produce form the experimentally derived spectrochemical series:
(weak-field ligands → strong-field ligands)
(d) Tetrahedral splitting — \(\Delta_t\)
In a tetrahedral field the four ligands lie between the axes, so now the t2 orbitals (between axes) are destabilised and the e orbitals (along axes) are stabilised — the reverse of the octahedral pattern. The "g" subscript is dropped (no centre of symmetry):
\[ \Delta_t = \tfrac{4}{9}\,\Delta_o \]Because Δt is much smaller than the pairing energy, tetrahedral complexes are almost always high-spin.
(e) Colour of coordination compounds
If a complex absorbs light of a particular wavelength to promote an electron from t2g → eg (a d–d transition), the colour we see is the complementary colour. For example [Ti(H2O)6]3+ (d1) absorbs blue-green light (≈498 nm) and so appears violet. Removing the ligand field (e.g. by dehydration) destroys the splitting and the substance turns colourless: [Ti(H2O)6]Cl3 is violet but anhydrous TiCl3 is colourless. Anhydrous CuSO4 is white but CuSO4·5H2O is blue.
| Complex | λ absorbed (nm) | Colour absorbed | Colour observed |
|---|---|---|---|
| [CoCl(NH3)5]2+ | 535 | yellow | violet |
| [Co(NH3)5(H2O)]3+ | 500 | blue-green | red |
| [Co(NH3)6]3+ | 475 | blue | yellow-orange |
| [Co(CN)6]3− | 310 | UV (not visible) | pale yellow |
| [Cu(H2O)4]2+ | 600 | red | blue |
| [Ti(H2O)6]3+ | 498 | blue-green | violet |
(f) Limitations of CFT
- Treats ligands as point charges, so anionic ligands ought to give the largest Δ — but they actually sit at the low end of the spectrochemical series.
- Ignores the covalent character of the M–L bond (addressed by ligand field/MO theories).
Setup: A solution of NiCl2 in water gives the green [Ni(H2O)6]2+ ion. Ethane-1,2-diamine (en) is added drop-wise in molar ratios 1:1, 2:1 and 3:1.
Observed: green → pale blue → blue/purple → violet.
Sequence of complexes: [Ni(H2O)6]2+ → [Ni(H2O)4(en)]2+ → [Ni(H2O)2(en)2]2+ → [Ni(en)3]2+. en sits higher than H2O in the spectrochemical series, so each substitution increases Δₒ and shifts the absorbed wavelength to higher energy (shorter λ). The colour we see (the complement) accordingly shifts.
🔧 Interactive: Octahedral Spin-State and Magnetic-Moment Predictor
Pick a metal dn count and a ligand. The simulation predicts the t2g/eg filling, the number of unpaired electrons and the spin-only magnetic moment.
Worked Example 5.8 — Why is [Ni(CN)₄]²⁻ diamagnetic but [NiCl₄]²⁻ paramagnetic?
In [NiCl4]2−, Cl− is a weak-field ligand and cannot pair up the d-electrons. The 3d8 remains as 3d⁶ paired + 2 unpaired. Hybridisation is sp³ → tetrahedral. Two unpaired electrons → paramagnetic (μ ≈ 2.83 BM).
Worked Example 5.9 — Magnetic moment of hexaaqua vs hexacyano Mn²⁺
The hexaqua manganese(II) ion has 5 unpaired electrons but the hexacyano-manganese(III) ion has only one. Explain using CFT.
For Mn3+ (3d4) with the strong-field CN− ligand the question text refers to [Mn(CN)6]3−: Δₒ > P → low-spin t2g4eg0; n = 2 unpaired (although NCERT data often quote 1, depending on Jahn-Teller distortion). The strong field is responsible for the pairing.
🎯 Competency-Based Questions
Q1. The hybridisation of [Ni(CN)4]2− is: L1 Remember
Q2. The number of unpaired electrons in [FeF6]3− is: L3 Apply
Q3. Why is [Cr(NH3)6]3+ paramagnetic but [Ni(CN)4]2− diamagnetic? L4 Analyse
Q4. [Fe(CN)6]4− is yellow but [Fe(H2O)6]2+ is pale green. Account for the difference using CFT. L4 Analyse
Q5. HOT (Create): Sketch a CFT-style splitting diagram for a square-planar complex (derive it conceptually from the octahedral diagram). Where do the four orbitals end up relative to the average? L6 Create
🧠 Assertion–Reason Questions
Choose: (A) Both true, R explains A. (B) Both true, R doesn't explain A. (C) A true, R false. (D) A false, R true.
A: [Ni(CO)4] is diamagnetic but [NiCl4]2− is paramagnetic.
R: CO causes pairing of all 3d electrons of Ni; Cl−, being a weak-field ligand, cannot.
A: Tetrahedral complexes are almost always high-spin.
R: The tetrahedral splitting Δt is only 4/9 of Δo, so it is usually less than the pairing energy.
A: Anhydrous CuSO4 is white but CuSO4·5H2O is blue.
R: Crystal field splitting requires ligands; without ligands no d–d transition is possible.
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