Symmetry & Group Theory
Complete Handwritten-Style Notes · Solved Examples · MCQs · 27 Practice Questions
📋 Table of Contents
- Introduction — Why Symmetry Matters
- Symmetry Elements & Operations
- Point Groups — Assignment Algorithm
- Low & High Symmetry Point Groups
- Properties of Groups & Representations
- Character Tables — Reading & Using Them
- Chirality & Optical Activity
- Molecular Vibrations & IR / Raman Spectroscopy
- Solved Examples
- MCQ Bank (Exam-Style)
- Practice Question Set (27 Qs)
- Exam Tips & Tricks
Why Does Symmetry Matter in Chemistry?
Think of a snowflake — it looks identical after every 60° rotation. That is symmetry in action. In chemistry, when a molecule possesses symmetry, vast amounts of information about its electronic structure, bonding, spectroscopic behaviour, and reactivity become predictable without any calculation.
🔬 What Symmetry Lets Us Do
- Predict the number of IR and Raman active vibrational modes
- Construct molecular orbital (MO) diagrams systematically
- Determine whether a molecule is optically active (chiral)
- Interpret UV-Visible spectra of coordination compounds
- Identify allowed/forbidden electronic transitions
"Before symmetry, you needed pages of mathematics.
After symmetry, a single glance at a character table is enough."
Core Vocabulary — Memorise These First
- Symmetry Element — A geometric entity (axis, plane, centre, or point) about which a symmetry operation is performed.
- Symmetry Operation — The actual physical action (rotation, reflection, inversion) that leaves the molecule looking identical.
- Point Group — The complete set of all symmetry operations for a molecule; they all pass through one common point.
- Character Table — A compact mathematical summary of all irreducible representations of a point group.
The Five Symmetry Elements & Their Operations
Every possible molecular symmetry can be described using just five types of symmetry elements. Understanding each one in detail is the foundation for everything that follows.
| Symbol | Element | Operation | Key Example |
|---|---|---|---|
E |
Identity | Do nothing — all atoms stay in place | Every molecule has E |
Cₙ |
n-fold Rotation Axis | Rotate 360°/n (counterclockwise = positive) | CHCl₃ has C₃; H₂O has C₂ |
σ |
Mirror Plane | Reflect every atom through the plane | H₂O |
i |
Inversion Centre | (x,y,z) → (−x,−y,−z) through the centre | Staggered ethane, SF₆ |
Sₙ |
Improper Rotation Axis | Rotate 360°/n, then reflect ⊥ to that axis | CH₄ has S₄; staggered ethane has S₆ |
① The Identity Operation (E)
Completely trivial in appearance but mathematically essential. Every molecule must contain E, otherwise it cannot form a mathematical group. Think of E as "do nothing and come back to the start."
② Proper Rotation (Cₙ)
- Definition: Rotation by 360°/n around the rotation axis.
- Principal axis: The Cₙ with the largest value of n. Always placed along z by convention.
- Multiple rotations: Cₙᵏ = rotating k times by 360°/n. Note that Cₙⁿ ≡ E always.
- Snowflake magic: One snowflake possesses C₂, C₃, and C₆ axes simultaneously (60°, 120°, and 180° rotations).
⚡ Shortcut: Snowflake Rotation Table
For a regular hexagonal snowflake, rotations and their equivalences:
| Angle | Operation | Equivalence |
|---|---|---|
| 60° | C₆ | — |
| 120° | C₃ | C₆² |
| 180° | C₂ | C₆³ |
| 240° | C₃² | C₆⁴ |
| 300° | C₆⁵ | — |
| 360° | C₆⁶ | ≡ E |
③ Mirror Planes (σ) — Three Flavours
- σₕ (horizontal): Perpendicular to the principal axis Cₙ. The "flat" plane.
- σᵥ (vertical): Contains the principal axis; passes through atoms.
- σd (dihedral): Contains the principal axis but bisects angles between C₂ axes; passes between peripheral atoms.
✅ Quick Memory Aid for σ Labels
h = horizontal = ⊥ to Cₙ
v = vertical = contains Cₙ, through atoms
d = dihedral = contains Cₙ, between atoms
Trick: "h is the hat on top; v goes through the roof; d splits the difference."
④ Inversion Centre (i)
Every atom at position (x, y, z) maps to (−x, −y, −z). The molecule looks identical after this. Molecules like ethane (staggered), benzene, SF₆ have an inversion centre. Tetrahedral molecules like CH₄ do NOT — a common exam trap!
🚫 Common Exam Trap — Inversion
- Has i: Square, rectangle, octahedron, snowflake, staggered ethane, PtCl₄²⁻, SF₆
- No i: Triangle, pentagon, tetrahedron, CH₄, NH₃
- Note: S₂ ≡ i (improper rotation of order 2 is the same as inversion)
- Note: S₁ ≡ σ (improper rotation of order 1 is the same as reflection)
⑤ Improper Rotation (Sₙ) — The Compound Operation
Two-step operation: first rotate 360°/n about the axis, then reflect through the plane perpendicular to that axis. Both steps must be done — Sₙ is not a sum of Cₙ and σ, it is a single operation whose net effect is described by both.
- CH₄ has three S₄ axes — each bisects a pair of opposite edges of the tetrahedron.
- Two consecutive S₄ ≡ C₂:
S₄² = C₂ - Staggered ethane has an S₆ coincident with its C₃ axis.
Assigning Point Groups — The 6-Step Algorithm
The point group of a molecule is determined by a systematic decision tree. Follow these steps in order, and you will never get it wrong.
The D vs C vs S Decision
| Situation | Plane Present? | Point Group | Example |
|---|---|---|---|
| D-set: σₕ exists | σₕ | Dₙₕ | BF₃ (D₃ₕ), benzene (D₆ₕ) |
| D-set: σd exists | σd | Dₙd | Allene (D₂d), staggered ethane (D₃d) |
| D-set: no planes | None | Dₙ | [Co(en)₃]³⁺ (D₃) |
| C-set: σₕ exists | σₕ | Cₙₕ | Trans-N₂F₂ (C₂ₕ) |
| C-set: σᵥ exists | σᵥ | Cₙᵥ | NH₃ (C₃ᵥ), H₂O (C₂ᵥ) |
| C-set: S₂ₙ exists | None | S₂ₙ | 1,3,5,7-F₄ COT (S₄) |
| C-set: nothing else | None | Cₙ | H₂O₂ gauche (C₂) |
Low & High Symmetry Groups — Quick Reference
Low Symmetry Groups
| Group | Symmetry Content | Molecular Example |
|---|---|---|
C₁ | Only E — no symmetry at all | CHFClBr (four different groups on carbon) |
Cₛ | E and one mirror plane σ only | H₂C=CClBr (single plane of the molecule) |
Cᵢ | E and inversion centre i only | HClBrC–CHClBr staggered |
High Symmetry Groups
| Group | Key Features | Example | Total Ops |
|---|---|---|---|
C∞v | Linear, no inversion centre; ∞ C∞ and ∞ σᵥ | HCl, HF, CO, HCN | ∞ |
D∞h | Linear, with inversion centre; adds C₂ ⊥ and σₕ | H₂, N₂, CO₂, C₂H₂ | ∞ |
Td | 4 C₃, 3 C₂, 3 S₄, 6 σd — no C₄ axes | CH₄, CCl₄, NH₄⁺, SiF₄ | 24 |
Oh | All of Td plus 3 C₄, C₂ (=C₄²), i, S₄, S₆, σₕ, σd | SF₆, [PtCl₆]²⁻, cube | 48 |
Ih | 6 C₅, 10 C₃, 15 C₂, i, 6 S₁₀, 10 S₆, 15 σ | B₁₂H₁₂²⁻, C₆₀ (buckminsterfullerene) | 120 |
💡 Distinguishing Td vs Oh — An Exam Favourite
- Td molecules have only C₃ and C₂ — they have S₄ but NO C₄.
- Oh molecules have C₃, C₂, AND C₄ — adding C₄ changes everything.
- Memory rule: "Four-fold symmetry → six-fold coordination → Oh. Three-fold symmetry → four-coordination → Td."
Properties of a Mathematical Group
For a collection of symmetry operations to constitute a group, it must satisfy four rules. Every point group in chemistry obeys all four.
- Closure: The product (combination) of any two operations in the group must also be a member of the group. E.g. in C₂v: σᵥ × C₂ = σᵥ′
- Associativity: A(BC) = (AB)C always holds for symmetry operations.
- Identity: E is present and EA = AE = A for any operation A.
- Inverse: Every operation A has an inverse A⁻¹ such that A × A⁻¹ = E. Mirrors are their own inverse (σ² = E). C₃ and C₃² are inverses of each other.
Matrix Representations of Operations
Each symmetry operation can be expressed as a square transformation matrix acting on coordinates (x, y, z). For the C₂v group, the four transformation matrices are:
C₂v Transformation Matrices
| E | C₂ | σᵥ(xz) | σᵥ′(yz) |
|---|---|---|---|
| [+1, 0, 0 / 0, +1, 0 / 0, 0, +1] | [−1, 0, 0 / 0, −1, 0 / 0, 0, +1] | [+1, 0, 0 / 0, −1, 0 / 0, 0, +1] | [−1, 0, 0 / 0, +1, 0 / 0, 0, +1] |
| χ = 3 | χ = −1 | χ = 1 | χ = 1 |
The character (χ) = trace = sum of diagonal elements of the matrix.
Reducible vs Irreducible Representations
- Reducible representation (Γ): A combination of simpler (irreducible) ones. The 3×3 matrices for C₂v give characters 3, −1, 1, 1 — this Γ reduces to A₁ + B₁ + B₂.
- Irreducible representation: Cannot be broken down further; 1×1 matrices along the diagonal.
- Block diagonalisation is the process of converting reducible matrices to irreducible components.
The Reduction Formula — Most Important Equation
- nᵢ = number of times irreducible representation i appears
- h = order of the group (total number of symmetry operations)
- N(R) = number of operations in the class
- χ(R) = character of the reducible representation under operation R
- χᵢ(R) = character of the irreducible representation i under operation R
- The result must always be a non-negative integer — if you get a fraction, recheck your calculation.
Reading & Using Character Tables
A character table is the DNA of a point group — every symmetry property of the molecule is encoded in it.
Anatomy of the C₂v Character Table
| C₂v | E | C₂ | σᵥ(xz) | σᵥ′(yz) | Linear functions | Quadratic |
|---|---|---|---|---|---|---|
A₁ | 1 | 1 | 1 | 1 | z | x², y², z² |
A₂ | 1 | 1 | −1 | −1 | Rz | xy |
B₁ | 1 | −1 | 1 | −1 | x, Ry | xz |
B₂ | 1 | −1 | −1 | 1 | y, Rx | yz |
Seven Properties of Irreducible Representations (Must Know!)
- Order (h): Total count of all symmetry operations = sum across the top row.
- Classes: Operations with identical characters are grouped; number of classes = number of columns = number of rows (character tables are always square).
- Number of irreps = number of classes.
- Sum of squares of dimensions = h: For C₂v: 1² + 1² + 1² + 1² = 4 = h. ✓
- Sum of squares of characters × N(class) = h for each irrep separately.
- Orthogonality: Σ χᵢ(R)·χⱼ(R) = 0 for i ≠ j (dot product of any two rows = 0).
- Totally symmetric representation (all characters = 1) is always present — it is A₁ (or Ag, A₁g etc.).
Label Decoding — A, B, E, T
| Label | Dimension of irrep | Meaning |
|---|---|---|
A | 1 | Symmetric (χ = +1) w.r.t. principal Cₙ rotation |
B | 1 | Antisymmetric (χ = −1) w.r.t. principal Cₙ rotation |
E | 2 | Doubly degenerate — two modes at same energy |
T | 3 | Triply degenerate (only in cubic/icosahedral groups) |
| Subscript g | — | Symmetric to inversion (gerade) |
| Subscript u | — | Antisymmetric to inversion (ungerade) |
| Subscript 1 | — | Symmetric to perpendicular C₂ (or to σᵥ if no C₂⊥) |
| Subscript 2 | — | Antisymmetric to perpendicular C₂ (or to σᵥ) |
| Prime (′) | — | Symmetric to σₕ |
| Double prime (″) | — | Antisymmetric to σₕ |
Chirality & Optical Activity Through Symmetry
A molecule is chiral (dissymmetric) if it is non-superimposable on its mirror image. The symmetry criterion is simple and powerful:
i.e., NO σ, NO i, NO Sₙ (n ≥ 2)
✅ Chiral Point Groups
A molecule is chiral if it belongs to: C₁, Cₙ (n ≥ 2), Dₙ
Non-chiral (achiral) point groups contain σ, i, or Sₙ: Cₛ, Cᵢ, Cₙₕ, Cₙᵥ, Dₙₕ, Dₙd, Td, Oh, Ih, S₂ₙ
- Optical activity: Chiral molecules rotate plane-polarised light. Dextrorotatory (+) = clockwise; levorotatory (−) = counterclockwise.
- [Ru(en)₃]²⁺ belongs to D₃ — chiral. Its mirror images look like left- and right-handed propellers.
- CBrClFI belongs to C₁ — chiral (four different substituents on carbon).
- A propeller has a C₃ axis but no mirror plane → chiral despite having rotational symmetry.
- Key insight: It is the absence of improper symmetry elements (σ, i, Sₙ) that makes a molecule chiral — not just the absence of all symmetry.
Molecular Vibrations, IR & Raman Activity
Degrees of Freedom
| Molecule Type | Total DOF | Translational | Rotational | Vibrational |
|---|---|---|---|---|
| Linear (N atoms) | 3N | 3 | 2 | 3N − 5 |
| Non-linear (N atoms) | 3N | 3 | 3 | 3N − 6 |
| H₂O (non-linear, N=3) | 9 | 3 | 3 | 3 |
| CO₂ (linear, N=3) | 9 | 3 | 2 | 4 |
| NH₃ (non-linear, N=4) | 12 | 3 | 3 | 6 |
| XeF₄ (non-linear, N=5) | 15 | 3 | 3 | 9 |
Steps to Find Vibrational Modes via Group Theory
- Step 1: Assign x, y, z coordinates to every atom; count 3N total vectors.
- Step 2: For each symmetry operation, find χ(R) for the reducible representation:
— If atom moves position: contribute 0 per atom
— If atom stays: contribute +1 for each unchanged vector direction, −1 for each reversed direction - Step 3: Reduce Γtotal using the reduction formula to get irreducible representations.
- Step 4: Subtract Γtrans and Γrot (from the right column of the character table under x,y,z and Rx,Ry,Rz).
- Step 5: Remaining = Γvib — these are the vibrational modes.
H₂O — Worked Out
H₂O Complete Vibrational Analysis (C₂v)
Γtotal = 3A₁ + A₂ + 3B₁ + 2B₂ (from 9 motion vectors)
Γtrans = A₁ + B₁ + B₂ (matching z, x, y)
Γrot = A₂ + B₁ + B₂ (matching Rz, Ry, Rx)
Γvib = 3A₁ + A₂ + 3B₁ + 2B₂ − (A₁ + A₂ + 2B₁ + 2B₂) = 2A₁ + B₁
✅ 3 modes (= 3N−6 = 9−6 = 3). Both A₁ modes and the B₁ mode are IR active.
IR Activity Rule
Physically: the vibration must cause a change in dipole moment. Translations x, y, z represent motion of the centre of charge — if a vibrational mode transforms like them, it shifts charge.
Raman Activity Rule
Physically: Raman activity requires a change in polarisability of the molecule during the vibration.
⚡ Mutual Exclusion Rule
For molecules with a centre of inversion (i), no mode can be both IR and Raman active. IR-active modes are u (ungerade); Raman-active modes are g (gerade). This is an extremely useful diagnostic: if a molecule shows mutual exclusion in its spectra, it must possess a centre of inversion.
Carbonyl Stretching — The Classic Diagnostic
- cis-ML₂(CO)₂ (C₂v): Γco = A₁ + B₁ → both are IR active → two CO bands in IR.
- trans-ML₂(CO)₂ (D₂h): Γco = Ag + B₃u → Ag is IR inactive, B₃u is active → one CO band in IR.
- fac-M(CO)₃L₃ (C₃v): Γco = A₁ + E → both IR active → two CO bands (E is degenerate).
- Diagnostic rule: Count CO bands in IR to determine geometry of metal carbonyl complexes.
Solved Examples
Exam-Style Multiple Choice Questions
- (A) 2
- (B) 3
- (C) 4
- (D) 6
- (A) HCl
- (B) CO₂
- (C) HCN
- (D) SO₂
- (A) C₂ followed by σᵥ
- (B) σₕ alone
- (C) Inversion (i)
- (D) C₂ alone
- (A) C₃h
- (B) C₃v
- (C) D₃h
- (D) D₃d
- (A) C₁
- (B) Cₛ
- (C) Cᵢ
- (D) C₂
- (A) 10
- (B) 12
- (C) 9
- (D) 15
- (A) A
- (B) B
- (C) E
- (D) T
- (A) A C₂ axis
- (B) A mirror plane
- (C) A centre of inversion
- (D) An S₄ axis
- (A) 1
- (B) 2
- (C) 3
- (D) 4
- (A) Oh
- (B) Td
- (C) D₄h
- (D) Ih
- (A) H₂O
- (B) NH₃
- (C) CHFClBr
- (D) CHCl₃
- (A) Always 1
- (B) Always 0
- (C) The dimension of the representation
- (D) The order of the group
27-Question Practice Set
Based on IIT-JAM, GATE, CSIR-NET, BITSAT, TGT/PGT exam patterns. Answers to selected questions provided.
📌 Selected Answers
- Q1: D₃d — three σd planes (each containing C–C bond and one pair of H atoms from opposite ends)
- Q5: D₄h — yes, inversion centre is present (opposite Cl atoms map onto each other)
- Q6: CO₂ has 4 modes (3N−5): symmetric stretch (IR inactive, Raman active), asymmetric stretch (IR active), 2× bending (IR active, degenerate)
- Q8: nA₁ = (1/6)[6+6+6] = 3; nA₂ = (1/6)[6+6−6] = 1; nE = (1/6)[12−6+0] = 1. So Γ = 3A₁ + A₂ + E
- Q21: h = 48; 10 classes of symmetry operations
- Q23: nT₂ = (1/24)[(3)(4)(1)+(0)(1)(0)+(0)(0)(−1)+(0)(0)(−1)+(6)(2)(1)] = (1/24)[12+0+0+0+12] = 1
- Q24: Staggered D₅d has an S₁₀ axis and inversion centre (i). Eclipsed D₅h has σₕ but no inversion centre.
- Q27: C₂ (gauche N₂H₄) — chiral, as it has only E and C₂ (no σ, no i). Shows optical activity.
Exam Tips, Tricks & High-Yield Points
🎯 High-Frequency Exam Points
- Point group of H₂O = C₂v; NH₃ = C₃v; CH₄ = Td; SF₆ = Oh; CO₂ = D∞h; HCl = C∞v — commit these to memory.
- S₂ ≡ i and S₁ ≡ σ — if you see S₂ in options, it means inversion!
- Mutual exclusion rule: if IR and Raman bands are at the same wavenumber, the molecule has no inversion centre.
- Number of IR-active CO bands: cis = 2; trans = 1. One of the most tested facts in GATE/CSIR-NET.
- Chiral point groups contain ONLY E and proper Cₙ rotations: C₁, Cₙ (n≥2), Dₙ.
- The character under E always equals the dimension of the irrep: A=1, E=2, T=3.
- Reduction formula must give non-negative integers — if you get a fraction, you've made an error.
- The order h of Oh = 48, Td = 24, D₄h = 16, C₂v = 4, C₃v = 6.
- For the principal axis: always use the z direction. The xy plane is perpendicular to z.
🚨 Classic Traps in Competitive Exams
- Trap 1: CHCl₃ looks like it could have Oh symmetry — it does not! It has C₃v (three Cl atoms equivalent, one H on C₃).
- Trap 2: Staggered ethane is D₃d, NOT D₃h. The hydrogen eclipsing in the eclipsed form gives D₃h.
- Trap 3: Allene (D₂d) is NOT the same as ethylene (D₂h). Allene has σd planes, not σₕ.
- Trap 4: "E" in the character table label (E irrep) is completely different from "E" the identity operation. Context matters!
- Trap 5: XeF₄ is square planar (D₄h), not tetrahedral. Xe has lone pairs pushing geometry flat.
- Trap 6: The totally symmetric representation (A₁, Ag, A₁g etc.) is always Raman active.
Quick Recall: How to Tell D vs C Groups
Memory Device: "D has Diagonals, C is Closed"
Look for C₂ axes that stick out perpendicular to the main axis like the spokes of a wheel. If you find them → D group. Count how many: there are always n of them for a Dₙ group. If no spokes → C or S group.
For a D group: σₕ → Dₙh. No σₕ but σd → Dₙd. No planes at all → Dₙ.
For a C group: σₕ → Cₙh. σᵥ → Cₙv. S₂ₙ only → S₂ₙ. Nothing → Cₙ.
Important Tables at a Glance
| Molecule | Point Group | IR-active vibrations | Raman-active | Chiral? |
|---|---|---|---|---|
| H₂O | C₂v | All 3 (2A₁ + B₁) | All 3 | No (σᵥ) |
| CO₂ | D∞h | 2 of 4 (πu, σu) | 1 of 4 (σg+) | No (i) |
| NH₃ | C₃v | All 6 | All 6 | No (σᵥ) |
| CH₄ | Td | T₂ modes only | A₁ + E + T₂ | No (σd) |
| SF₆ | Oh | T₁u only | A₁g + Eg + T₂g | No (i) |
| CHFClBr | C₁ | All modes | All modes | Yes! |
| Benzene | D₆h | Only u modes | Only g modes | No (i, σ) |
| Staggered ethane | D₃d | Only u modes | Only g modes | No (i) |
