Part 1 · Chapter 3

Chemical Bonding & Molecular Structure

Why atoms join and what shape the result takes — from Lewis dots and VSEPR to hybridization and molecular orbitals

Fundamentals of Chemistry Prof. Mithun Mondal Reading time ≈ 46 min
i What you'll learn
  • Why atoms bond — the octet rule, Lewis structures and formal charge.
  • The difference between the ionic and covalent bond, and where Fajans' rules blur the line.
  • Bond parameters — length, angle, enthalpy and order — and how resonance averages them.
  • Predicting molecular shape with VSEPR, and explaining it with hybridization.
  • Molecular orbital theory: bonding and antibonding levels, bond order and magnetism.
  • Dipole moment, polarity, and the special role of the hydrogen bond.
Section 3-1

Why Atoms Bond

Atoms bond because the joined arrangement is lower in energy than the separated atoms. The Kössel–Lewis view captured this as the octet rule: atoms gain, lose or share electrons to reach the stable eight-electron configuration of a noble gas (a duplet for hydrogen).

A Lewis (electron-dot) structure shows valence electrons as dots, a shared pair as a line. Formal charge tells us which of several valid structures is most plausible:

Formal charge
\(\text{FC}=(\text{valence } e^-)-(\text{lone-pair } e^-)-\tfrac{1}{2}(\text{bonding } e^-)\)

The best Lewis structure has formal charges closest to zero and any negative charge on the most electronegative atom. The octet rule has exceptions — incomplete octets \((\ce{BF3})\), expanded octets \((\ce{SF6})\) and odd-electron species \((\ce{NO})\).

Section 3-2

The Ionic Bond

When a metal of low ionization energy meets a non-metal of high electron affinity, an electron transfers outright. The resulting cation and anion are held by electrostatic attraction in a giant crystal lattice. The energy released as gaseous ions assemble into one mole of solid is the lattice energy — the true measure of ionic-bond strength.

A transfer of electrons
\[ \ce{Na ->[-e^-] Na+},\qquad \ce{Cl ->[+e^-] Cl-},\qquad \ce{Na+ + Cl- -> NaCl} \]
Lattice energy rises with larger charges and smaller ions, following the Coulomb form \(U\propto \dfrac{q_+q_-}{r_++r_-}\).
No bond is purely ionic. Fajans' rules say a small, highly charged cation polarizes a large anion, dragging electron density back and adding covalent character — which is why \(\ce{AlCl3}\) is far more covalent than \(\ce{NaCl}\).
Section 3-3

The Covalent Bond

When two atoms of similar electronegativity meet, neither wins the tug-of-war, so they share electron pairs. One shared pair is a single bond, two a double, three a triple. Where a single Lewis structure cannot capture the real molecule, two or more contributing structures are drawn and the molecule is a resonance hybrid of them.

Resonance in the carbonate ion

The three \(\ce{C-O}\) bonds of \(\ce{CO3^2-}\) are identical, intermediate between single and double. No one Lewis structure shows this; the true ion is the average — the resonance hybrid — and is more stable than any single contributor (resonance energy).

Section 3-4

Bond Parameters

Every covalent bond carries measurable quantities. Bond length is the equilibrium internuclear distance; bond angle is the angle between two bonds at an atom; bond enthalpy is the energy to break one mole of bonds in the gas phase; bond order is the number of bonds between two atoms.

BondOrderLength (pm)Enthalpy (kJ mol⁻¹)
\(\ce{C-C}\)1154348
\(\ce{C=C}\)2134614
\(\ce{C#C}\)3120839
The trend that never fails. Higher bond order means a shorter and stronger bond. Length and strength move in opposite directions.
Section 3-5

VSEPR & the Shape of Molecules

Valence-shell electron-pair repulsion theory predicts geometry from one idea: electron pairs around the central atom arrange themselves to be as far apart as possible. Lone pairs repel more strongly than bonding pairs, so they compress the remaining bond angles.

linear · 180°
2 pairs — \(\ce{BeCl2}\)
trigonal · 120°
3 pairs — \(\ce{BF3}\)
tetrahedral · 109.5°
4 pairs — \(\ce{CH4}\)
Bond + lone pairsElectron geometryExample shape
2 + 0Linear\(\ce{CO2}\) — linear
3 + 0Trigonal planar\(\ce{BF3}\) — trigonal planar
4 + 0Tetrahedral\(\ce{CH4}\) — tetrahedral
3 + 1Tetrahedral\(\ce{NH3}\) — pyramidal (107°)
2 + 2Tetrahedral\(\ce{H2O}\) — bent (104.5°)
5 + 0Trigonal bipyramidal\(\ce{PCl5}\)
6 + 0Octahedral\(\ce{SF6}\)
Section 3-6

Valence Bond Theory

VSEPR predicts shape but says nothing about how bonds form. Valence bond theory says a covalent bond is the overlap of two half-filled atomic orbitals; the greater the overlap, the stronger the bond.

σ : head-on along the axis π : sideways above & below
A σ bond overlaps end-to-end; a π bond overlaps side-to-side
Single, double, triple. A single bond is one σ; a double bond is one σ + one π; a triple bond is one σ + two π. The σ forms first and is the stronger; π bonds add to bond order but restrict rotation.
Section 3-7

Hybridization

Pure atomic orbitals cannot explain the equal bonds and observed angles of methane. The fix is hybridization: atomic orbitals of similar energy mix to form an equal number of identical hybrid orbitals pointing toward the bonded atoms. The number of hybrids equals the steric number (σ bonds + lone pairs).

HybridizationSteric numberGeometryExample
\(sp\)2Linear\(\ce{BeCl2},\ \ce{C2H2}\)
\(sp^2\)3Trigonal planar\(\ce{BF3},\ \ce{C2H4}\)
\(sp^3\)4Tetrahedral\(\ce{CH4},\ \ce{NH3},\ \ce{H2O}\)
\(sp^3d\)5Trigonal bipyramidal\(\ce{PCl5}\)
\(sp^3d^2\)6Octahedral\(\ce{SF6}\)
🧩
A fast count
\(\text{Steric number}=(\text{number of }\sigma\text{ bonds})+(\text{number of lone pairs on the central atom})\)

Steric number 2, 3, 4, 5, 6 maps directly to \(sp,\ sp^2,\ sp^3,\ sp^3d,\ sp^3d^2\). Only σ bonds and lone pairs count — π bonds do not change the hybridization.

Section 3-8

Molecular Orbital Theory

Where VBT keeps electrons on individual atoms, molecular orbital theory lets atomic orbitals combine into molecular orbitals spread over the whole molecule. Two atomic orbitals make two MOs: a lower-energy bonding orbital and a higher-energy antibonding orbital \((\ast)\).

AO AO σ* antibonding σ bonding ↑↓ bond order = ½(Nb − Na)
Two atomic orbitals split into a bonding and an antibonding MO
📊
Bond order from MOT
\(\text{Bond order}=\tfrac{1}{2}\,(N_b-N_a)\)

where \(N_b\) and \(N_a\) are electrons in bonding and antibonding MOs. A positive bond order means a stable molecule; unpaired electrons make it paramagnetic. This is MOT's triumph — it correctly predicts that \(\ce{O2}\) is paramagnetic, which Lewis structures cannot.

Section 3-9

Polarity & Dipole Moment

When bonded atoms differ in electronegativity, the bond is polar — one end slightly negative, the other slightly positive. The dipole moment measures this separation, and being a vector, it depends on shape as much as on the bonds.

Dipole moment
\[ \mu = q\times d \qquad (\text{measured in debye, } 1\ \text{D}=3.34\times10^{-30}\ \text{C m}) \]
A molecule is non-polar if its bond dipoles cancel by symmetry.
! Shape can cancel polarity

\(\ce{CO2}\) has two polar \(\ce{C=O}\) bonds yet \(\mu=0\) — being linear, the dipoles oppose and cancel. Bent \(\ce{H2O}\), with the same idea of polar bonds, does not cancel and is strongly polar. Geometry decides.

Section 3-10

The Hydrogen Bond

When hydrogen is bonded to a small, highly electronegative atom \((\ce{N},\ \ce{O},\ \ce{F})\), the bare proton attracts a lone pair on a neighbouring electronegative atom. This hydrogen bond is far weaker than a covalent bond but strong among intermolecular forces.

Small bonds, large effects. Hydrogen bonding explains water's high boiling point, ice being less dense than liquid water, and the double helix of DNA. It comes in intermolecular (between molecules, raising boiling point) and intramolecular (within a molecule, as in \(o\)-nitrophenol) varieties.
Worked Examples

Putting It to Work

1 Formal charge in ozone

Problem. In one resonance form of ozone \(\ce{O3}\), the central oxygen has one lone pair, one single bond and one double bond. Find its formal charge.

Solution. Valence \(=6\), lone-pair electrons \(=2\), bonding electrons \(=6\):

Working
\[ \text{FC}=6-2-\tfrac{1}{2}(6)=+1 \]
2 Predicting a shape with VSEPR

Problem. Predict the shape and bond angle of \(\ce{NH3}\).

Solution. Nitrogen has 3 bonding pairs and 1 lone pair — steric number 4, so the electron geometry is tetrahedral. The lone pair pushes the bonds together:

Working
\[ \text{shape = trigonal pyramidal},\qquad \angle\ce{HNH}\approx107^{\circ} \]
3 Hybridization of a central atom

Problem. Find the hybridization of carbon in ethyne \(\ce{C2H2}\).

Solution. Each carbon forms 2 σ bonds (one to \(\ce{H}\), one to \(\ce{C}\)) and has no lone pair — steric number 2:

Working
\[ \text{steric number}=2\ \Rightarrow\ sp\ \text{hybridized, linear} \]

The remaining two p orbitals on each carbon form the two π bonds of the triple bond.

4 Bond order and magnetism of O₂

Problem. Using MOT, find the bond order of \(\ce{O2}\) (16 electrons) and state whether it is paramagnetic.

Solution. Filling the MOs gives \(N_b=10,\ N_a=6\):

Working
\[ \text{Bond order}=\tfrac{1}{2}(10-6)=2 \]

The two \(\pi^\ast\) orbitals each hold one electron, so \(\ce{O2}\) has two unpaired electrons — it is paramagnetic.

5 Polar bonds, non-polar molecule

Problem. Both \(\ce{CO2}\) and \(\ce{H2O}\) contain polar bonds. Why is one non-polar and the other polar?

Solution. \(\ce{CO2}\) is linear, so its two equal bond dipoles point in opposite directions and sum to zero — \(\mu=0\). \(\ce{H2O}\) is bent \((104.5^{\circ})\), so its bond dipoles add to a net moment \((\mu=1.85\ \text{D})\). Geometry, not the bonds alone, decides molecular polarity.

6 Comparing bond orders

Problem. Arrange \(\ce{O2},\ \ce{O2+},\ \ce{O2-}\) in order of increasing bond length.

Solution. Removing an antibonding electron raises bond order; adding one lowers it:

Working
\[ \ce{O2+}\,(2.5)>\ce{O2}\,(2.0)>\ce{O2-}\,(1.5) \]

Higher bond order means shorter bond, so increasing length is \(\ce{O2+}<\ce{O2}<\ce{O2-}\).

Review

Chapter Summary

Why atoms bond

To lower energy and reach an octet; formal charge picks the best Lewis structure.

Bond types

Ionic = transfer (lattice energy); covalent = sharing; Fajans' rules blend the two.

Parameters

Higher bond order → shorter, stronger bond; resonance averages them.

Shape

VSEPR from electron-pair repulsion; hybridization from steric number.

MOT

\(\text{B.O.}=\tfrac12(N_b-N_a)\); unpaired electrons → paramagnetic.

Polarity

\(\mu=q\times d\); symmetric shapes cancel dipoles; H-bonding shifts properties.

Practice

Problems

Draw the Lewis structure first, count σ bonds and lone pairs, then read off shape and hybridization. Difficulty rises down the list.

  1. Draw the Lewis structure of \(\ce{CO2}\) and assign formal charges.
  2. Predict the shapes and bond angles of \(\ce{BF3},\ \ce{H2O}\) and \(\ce{SF6}\).
  3. State the hybridization of the central atom in \(\ce{PCl5},\ \ce{SO2}\) and \(\ce{XeF4}\).
  4. Explain why the bond angle in \(\ce{H2O}\,(104.5^{\circ})\) is smaller than in \(\ce{NH3}\,(107^{\circ})\).
  5. How many σ and π bonds are present in \(\ce{C2H4}\) and in \(\ce{HCN}\)?
  6. Using Fajans' rules, arrange \(\ce{NaCl},\ \ce{MgCl2},\ \ce{AlCl3}\) in order of increasing covalent character.
  7. Calculate the bond order of \(\ce{N2}\) and \(\ce{N2+}\) and predict which has the stronger bond.
  8. Why is \(\ce{O2}\) paramagnetic while \(\ce{N2}\) is diamagnetic? Use MOT.
  9. Account for the order of boiling points \(\ce{HF}>\ce{HCl}\) despite \(\ce{HCl}\) having the larger molar mass.
  10. Predict whether \(\ce{NH3}\) or \(\ce{NF3}\) has the larger dipole moment, and justify it.
  11. Compare the bond orders of \(\ce{O2},\ \ce{O2^2-}\) and \(\ce{O2+}\), and order their bond strengths.
  12. The dipole moment of \(\ce{HCl}\) is \(1.03\ \text{D}\) and the bond length is \(127\ \text{pm}\). Estimate its percent ionic character.
Tip: almost every structure question yields to one routine — draw the Lewis structure, total the σ bonds and lone pairs on the central atom to get the steric number, and that number alone gives you the hybridization, the electron geometry and (after subtracting lone pairs) the molecular shape. Reach for MOT only when magnetism or fractional bond orders are involved.