Chemical Bonding and Molecular Structure
⚑ Panic box
VSEPR repulsion: lp–lp > lp–bp > bp–bp; more lone pairs usually compress bond angles.
Bond order: Lewis count = shared pairs; MO value = $\tfrac12(N_b-N_a)$.
Resonance: the molecule is one hybrid, not a structure switching between canonical forms.
Multiple bond: one $\sigma$ bond plus additional $\pi$ bond(s), except the unusual MO description of $\mathrm{C_2}$.
MO magnetism: unpaired electrons → paramagnetic; all paired → diamagnetic.
1. Lewis structures and the octet idea
- Chemical bond — attraction holding atoms or ions together; bonding lowers a system’s energy.
- Valence electrons — outer-shell electrons available for bonding; Lewis-symbol dots count them.
- Octet rule — atoms commonly gain, lose or share electrons to reach eight outer-shell electrons; H aims for a duplet.
- Ionic bond — electrostatic attraction between oppositely charged ions; electron transfer creates the ions.
- Covalent bond — shared electron pair(s) between atoms; one pair = single, two = double, three = triple bond.
- Lone pair — valence-electron pair not shared in a bond.
- Electrovalence — number of unit charges on an ion.
Lewis structure routine
- Add all atoms’ valence electrons; add one per negative charge, subtract one per positive charge.
- Choose the skeletal arrangement; usually put the least electronegative atom centrally (never H).
- Join atoms with single bonds; complete terminal atoms’ shells, then the central atom’s.
- If the central atom lacks an octet, make multiple bonds where possible; check total electrons and charge.
Octet-rule exceptions
| Case | Recognise it | Examples |
|---|---|---|
| Incomplete octet | Central atom has fewer than 8 electrons | $\mathrm{BeH_2, BCl_3, BF_3}$ |
| Odd-electron species | Total electron count is odd | $\mathrm{NO, NO_2}$ |
| Expanded octet | Central atom has more than 8 electrons | $\mathrm{PF_5, SF_6, H_2SO_4}$ |
Useful for many molecules, especially second-period atoms; it does not predict shape or relative molecular stability, and noble gases can form compounds.
Formal charge — bookkeeping charge on an atom in a Lewis structure:
$$\mathrm{FC}=V-L-\tfrac12B$$
$V$ = free-atom valence electrons; $L$ = nonbonding electrons; $B$ = bonding electrons. Formal charge is not necessarily the atom’s real charge; among alternatives, a structure with smaller formal charges is generally favoured.
2. Ionic bonding and bond parameters
Ionic formation: $\mathrm{M(g)\rightarrow M^+(g)+e^-}$ (ionisation; endothermic) · $\mathrm{X(g)+e^-\rightarrow X^-(g)}$ (electron gain; may release or absorb energy) · gaseous ions assemble into a crystal lattice.
- Favourable ion formation — relatively low ionisation enthalpy for the cation-former and strongly negative electron-gain enthalpy for the anion-former.
- Lattice enthalpy — energy needed to separate one mole of ionic solid into gaseous ions; lattice formation releases this energy.
- Ionic-solid stability — lattice formation can outweigh the energy cost of forming gaseous ions; octets alone do not decide stability.
| Parameter | Meaning / relation | Recall point |
|---|---|---|
| Bond length | Equilibrium internuclear distance; for a covalent $\mathrm{AB}$ bond, $R=r_A+r_B$ | Higher bond order generally means shorter bond |
| Covalent radius | Half the bond length between identical bonded atoms | Bonded situation |
| van der Waals radius | Half the separation of identical nonbonded atoms in a solid | Nonbonded situation; larger than covalent radius |
| Bond angle | Angle between bonding orbitals around a central atom | Helps identify molecular shape |
| Bond enthalpy | Energy to break one mole of a specified bond type in gaseous molecules | Larger value → stronger bond |
| Mean bond enthalpy | Total dissociation enthalpy divided by number of bonds broken | Used for polyatomic molecules; successive bonds may differ |
| Bond order (Lewis) | Number of bonds between two atoms | Single = 1, double = 2, triple = 3 |
Trend: bond order ↑ → bond enthalpy ↑ and bond length ↓. In polyatomic molecules, the same bond can have different dissociation enthalpies in different chemical environments.
3. Resonance, polarity and dipole moment
Resonance — several valid Lewis canonical forms with the same nuclear arrangement contribute to one real resonance hybrid.
- Use when one Lewis structure cannot match the observed bonding (e.g. equal bonds in $\mathrm{O_3}$ or $\mathrm{CO_3^{2-}}$).
- Hybrid energy is lower than that of any individual canonical form; bond character is averaged.
- Canonical forms are not separate real structures and are not in equilibrium with one another.
Bond polarity — equal sharing between identical atoms gives a nonpolar covalent bond; unequal sharing toward the more electronegative atom gives a polar covalent bond.
$$\mu=Qr$$
$Q$ = charge magnitude; $r$ = separation of charge centres. Dipole moment is a vector; $1\ \mathrm{D}=3.33564\times10^{-30}\ \mathrm{C,m}$. Molecular dipole = vector sum of bond dipoles (and the lone-pair contribution).
| Molecule pattern | Net dipole |
|---|---|
| Symmetric bonds cancel (e.g. $\mathrm{BeF_2, BF_3, CCl_4}$) | $0$ |
| Bent or pyramidal arrangement (e.g. $\mathrm{H_2O, NH_3}$) | Usually nonzero |
| $\mathrm{NH_3}$ vs $\mathrm{NF_3}$ | $\mathrm{NH_3}$ larger: lone-pair contribution reinforces N–H bond resultants; in $\mathrm{NF_3}$ it opposes N–F resultants |
Fajans’ rules: greater covalent character when the cation is smaller, the cation charge is higher, or the anion is larger. For same-size, same-charge cations, a transition-metal-type $(n-1)d^nns^0$ configuration polarises more than a noble-gas configuration.
4. VSEPR shapes
VSEPR rule — valence-shell electron pairs spread out to minimise repulsion; multiple bonds count as one electron domain (a “super pair”).
$$\mathrm{lp-lp>lp-bp>bp-bp}$$
| Electron domains around central atom | Electron-pair arrangement | Example with no lone pair |
|---|---|---|
| 2 | Linear, $180^\circ$ | $\mathrm{BeCl_2}$ |
| 3 | Trigonal planar, $120^\circ$ | $\mathrm{BF_3}$ |
| 4 | Tetrahedral, $109.5^\circ$ | $\mathrm{CH_4}$ |
| 5 | Trigonal bipyramidal | $\mathrm{PCl_5}$ |
| 6 | Octahedral | $\mathrm{SF_6}$ |
| Central-atom domains | Molecular shape | Example / angle |
|---|---|---|
| 3 bonding + 1 lone pair | Trigonal pyramidal | $\mathrm{NH_3}$, $107^\circ$ |
| 2 bonding + 2 lone pairs | Bent | $\mathrm{H_2O}$, $104.5^\circ$ |
| 2 bonding + 1 lone pair | Bent | $\mathrm{SO_2}$, about $119.5^\circ$ |
| 4 bonding + 1 lone pair | See-saw | Lone pair prefers equatorial position |
| 3 bonding + 2 lone pairs | T-shaped | Lone pairs prefer equatorial positions |
Lone pairs occupy more space than bonding pairs → bond angles shrink from ideal values. In trigonal bipyramidal arrangements, equatorial lone-pair placement reduces repulsions; axial bonds experience more repulsion and are longer/weaker than equatorial bonds.
5. Valence-bond theory, overlap and hybridisation
Valence-bond picture — covalent bonding forms when half-filled atomic orbitals overlap and opposite-spin electrons pair. As atoms approach, attraction lowers potential energy until the equilibrium distance; closer approach then raises energy sharply. Greater effective overlap generally gives a stronger bond.
| Bond type | Orbital overlap | Key feature |
|---|---|---|
| $\sigma$ | Head-on along internuclear axis; $s-s$, $s-p$ or $p-p$ | Greater overlap; stronger than $\pi$ |
| $\pi$ | Sideways overlap of parallel $p$ orbitals | Electron clouds above and below the internuclear axis |
A double bond contains $1\sigma+1\pi$; a triple bond contains $1\sigma+2\pi$. In phase/sign diagrams, $+$ and $-$ mark wave-function phase, not charge; effective overlap requires suitable phase and orientation.
Hybridisation — mixing valence orbitals of similar energy to make equivalent, directionally arranged hybrid orbitals. Number of hybrids = number of orbitals mixed; promotion is not always required, and filled orbitals may participate.
| Hybridisation | Orbitals mixed → hybrids | Arrangement / angle | Chapter examples |
|---|---|---|---|
| $sp$ | $s+p\rightarrow2$ | Linear, $180^\circ$ | $\mathrm{BeCl_2}$; carbon in $\mathrm{C_2H_2}$ |
| $sp^2$ | $s+2p\rightarrow3$ | Trigonal planar, $120^\circ$ | $\mathrm{BCl_3}$; carbon in $\mathrm{C_2H_4}$ |
| $sp^3$ | $s+3p\rightarrow4$ | Tetrahedral, $109.5^\circ$ | $\mathrm{CH_4}$; also $\mathrm{NH_3,H_2O}$ |
| $sp^3d$ | $s+3p+d\rightarrow5$ | Trigonal bipyramidal | $\mathrm{PCl_5}$ |
| $sp^3d^2$ | $s+3p+2d\rightarrow6$ | Octahedral | $\mathrm{SF_6}$ |
| $dsp^2$ | $d+s+2p\rightarrow4$ | Square planar | $[\mathrm{Ni(CN)_4}]^{2-}$ |
$sp^3$ examples: $\mathrm{CH_4}$ has four bonding hybrids; $\mathrm{NH_3}$ has three bonds + one lone pair; $\mathrm{H_2O}$ has two bonds + two lone pairs. In $\mathrm{C_2H_4}$, each C–C double bond is $1\sigma+1\pi$; in $\mathrm{C_2H_2}$, the C–C triple bond is $1\sigma+2\pi$.
6. Molecular-orbital theory
MO formation (LCAO): atomic orbitals combine when their energies are similar, symmetry matches about the molecular axis, and overlap is effective. Combining $n$ atomic orbitals gives $n$ molecular orbitals.
$$\psi_{\mathrm{bonding}}=\psi_A+\psi_B \qquad \psi_{\mathrm{antibonding}}=\psi_A-\psi_B$$
| Molecular orbital | Electron density / energy | Effect |
|---|---|---|
| Bonding | Density between nuclei; lower energy | Stabilises molecule |
| Antibonding ($*$) | Node between nuclei; higher energy | Destabilises molecule |
| $\sigma$ MO | Symmetric around bond axis | Includes end-on combinations |
| $\pi$ MO | Not symmetric around bond axis | Side-on $p$ combinations; density above/below axis |
Fill MOs by increasing energy, following Aufbau, Pauli and Hund rules. For second-period homonuclear molecules:
- $\mathrm{B_2,C_2,N_2}$: $\sigma_{1s}<\sigma^{1s}<\sigma{2s}<\sigma^{2s}<\pi{2p_x}=\pi_{2p_y}<\sigma_{2p_z}<\pi^_{2p_x}=\pi^{2p_y}<\sigma^*{2p_z}$
- $\mathrm{O_2,F_2}$: same order through $\sigma^{2s}$, then $\sigma{2p_z}<\pi_{2p_x}=\pi_{2p_y}<\pi^{2p_x}=\pi^*{2p_y}<\sigma^*_{2p_z}$
$$\mathrm{MO\ bond\ order}=\tfrac12(N_b-N_a)$$
$N_b$ = bonding-MO electrons; $N_a$ = antibonding-MO electrons. Positive bond order → stable; zero or negative → unstable. Larger bond order generally means shorter, stronger bonding. Unpaired MO electrons → paramagnetic; all paired → diamagnetic.
| Species | Bond order | Stability / magnetism |
|---|---|---|
| $\mathrm{H_2}$ | 1 | Stable; diamagnetic |
| $\mathrm{He_2}$ | 0 | Unstable |
| $\mathrm{Li_2}$ | 1 | Stable; diamagnetic |
| $\mathrm{Be_2}$ | 0 | Unstable |
| $\mathrm{C_2}$ | 2 | Stable; diamagnetic; two $\pi$ bonds in the MO account |
| $\mathrm{O_2}$ | 2 | Stable; paramagnetic, two unpaired electrons |
7. Hydrogen bonding
Hydrogen bond — attraction between H attached to a strongly electronegative atom (F, O or N) and an electronegative atom on another site. The bonded H becomes partially positive; the electronegative atom is partially negative. Weaker than a covalent bond.
| Type | Where it forms | Examples |
|---|---|---|
| Intermolecular | Between molecules | HF, alcohols, water |
| Intramolecular | Within one molecule | $o$-nitrophenol |
Hydrogen bonding is strongest in solids and weakest in gases; it substantially affects structure and properties.
8. Traps
Octet rule applies to every atom→ Check incomplete, odd-electron and expanded-octet cases.Formal charge is the atom’s actual charge→ It is Lewis-structure bookkeeping; the ion’s net charge belongs to the whole ion.Canonical resonance forms are structures the molecule switches between→ The actual molecule is one resonance hybrid.Polar bonds guarantee a polar molecule→ Molecular geometry can make bond-dipole vectors cancel.All electron-pair repulsions are equal→ $\mathrm{lp-lp>lp-bp>bp-bp}$; account for lone pairs before assigning shape.A double bond is two $\sigma$ bonds→ It is $1\sigma+1\pi$; a triple bond is $1\sigma+2\pi$.More antibonding electrons increase stability→ Use $\tfrac12(N_b-N_a)$; zero bond order means unstable in this model.$\mathrm{O_2}$ is diamagnetic because it has a double bond→ MO theory leaves two unpaired electrons, so it is paramagnetic.