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Structure of Matter · Bonding and properties

Ionic Bonding and Born–Haber Cycles

Table salt on your kitchen counter is not made of little "NaCl molecules" floating around. It is an enormous three-dimensional lattice of $\mathrm{Na^+}$ and $\mathrm{Cl^-}$ ions held together by electrostatic attraction. That lattice is so stable that nobody can simply boil it into separate gaseous ions and measure the energy. So how much energy does it take to pull a mole of salt apart into ions? A clever thermodynamic detour, the Born–Haber cycle, answers it.

An Ionic Crystal Is Not a Molecule

Two-dimensional sketch of a rock salt lattice with cations and anions alternating in regular positions Rock salt lattice: each ion is surrounded by opposite charges

Properties of ionic solids

Ionic solids are brittle: a blow shifts a layer so that like charges line up and repel, and the crystal cracks. They have high melting points because many strong electrostatic attractions must be overcome. They do not conduct as solids because the ions are locked in place, but they conduct when molten or dissolved because the ions can move.

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Sodium chloride, $\mathrm{NaCl}$, crystallizes forming a three-dimensional rock salt structure (two interpenetrating ionic sublattices), whereas hydrogen chloride,…

Sodium chloride, $\mathrm{NaCl}$, crystallizes forming a three-dimensional rock salt structure (two interpenetrating ionic sublattices), whereas hydrogen chloride, $\mathrm{HCl}$, forms discrete diatomic molecules in the gas phase at room temperature. Justify, on the basis of the type of bonding and structure, why it makes no physical sense to speak of a "$\mathrm{NaCl}$ molecule" in the solid state, stating how the empirical formula of this ionic compound is defined.

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Lattice Energy: Charge and Ionic Radius

NaCl melts at $801\,^\circ\text{C}$, NaF at $996\,^\circ\text{C}$, and MgO at $2852\,^\circ\text{C}$. What microscopic factors make it so much harder to pull apart the ions of one crystal than another?

Picture two ions approaching each other. Far apart, they barely attract. As they get closer, the potential energy drops. At very short distance, electron clouds repel and the energy shoots up. The minimum of the curve gives the equilibrium distance (the bond length) and its depth is the energy released.

Potential energy of an ion pair versus internuclear distance, with a minimum at the bond length bond length minimum = energy released internuclear distance potential energy Comparison of how charge and internuclear distance change the electrostatic attraction between ions according to Coulomb's law small, highly charged ions strong attraction large ions weaker attraction
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Consider the lithium halides $\mathrm{LiF}$ and $\mathrm{LiI}$. Both compounds crystallize with the same ionic lattice geometry ($\mathrm{NaCl}$ type). Given that the…

Consider the lithium halides $\mathrm{LiF}$ and $\mathrm{LiI}$. Both compounds crystallize with the same ionic lattice geometry ($\mathrm{NaCl}$ type). Given that the ionic radii are $r(\mathrm{F^-}) = 133\,\mathrm{pm}$ and $r(\mathrm{I^-}) = 220\,\mathrm{pm}$, and considering the Born–Landé equation or Coulomb's law for the lattice energy (taken here as the exothermic process of formation of the lattice from gaseous ions, $\Delta H_{\mathrm{ret}} < 0$): a) Deduce, with justification, which of the two solids has the lattice enthalpy of greater magnitude $(|\Delta H_{\mathrm{ret}}|)$. b) Justify which of the two compounds will have the higher melting point.

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Potassium bromide, $\mathrm{KBr(s)}$, dissociates completely into its gaseous ions according to the endothermic process:…

Potassium bromide, $\mathrm{KBr(s)}$, dissociates completely into its gaseous ions according to the endothermic process: $\mathrm{KBr(s)} \to \mathrm{K^+(g)} + \mathrm{Br^-(g)}$. For this process, the lattice dissociation enthalpy is $\Delta H_{\mathrm{ret,dis}} = +689\,\mathrm{kJ\times mol^{-1}}$. Determine the standard lattice enthalpy of formation of the lattice, $\Delta H_{\mathrm{ret}}$, corresponding to the reaction $\mathrm{K^+(g)} + \mathrm{Br^-(g)} \to \mathrm{KBr(s)}$, and briefly explain the meaning of the thermodynamic sign obtained.

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The ionic compounds magnesium fluoride, $\mathrm{MgF_2}$, and calcium fluoride, $\mathrm{CaF_2}$, are compared. Both have an identical cation/anion charge ratio (+2/−1).…

The ionic compounds magnesium fluoride, $\mathrm{MgF_2}$, and calcium fluoride, $\mathrm{CaF_2}$, are compared. Both have an identical cation/anion charge ratio (+2/−1). Ionic radii data: $r(\mathrm{Mg^{2+}}) = 72\,\mathrm{pm}$, $r(\mathrm{Ca^{2+}}) = 100\,\mathrm{pm}$, and $r(\mathrm{F^-}) = 133\,\mathrm{pm}$. Experimentally, the magnitudes of the lattice enthalpies of formation $(\Delta H_{\mathrm{ret}} < 0)$ for both solids are $\approx 2957\,\mathrm{kJ\times mol^{-1}}$ and $\approx 2630\,\mathrm{kJ\times mol^{-1}}$. a) Assign, with justification, each lattice enthalpy value to its corresponding compound using arguments of electrostatic attraction. b) If $\mathrm{MgF_2}$ is now compared with magnesium oxide, $\mathrm{MgO}$ (where $r(\mathrm{O^{2-}}) = 140\,\mathrm{pm}$ and its $|\Delta H_{\mathrm{ret}}|$ is approximately $3791\,\mathrm{kJ\times mol^{-1}}$), explain the role of the greater charge of the oxide anion in the electrostatic attraction. State why a rigorous quantitative comparison also requires considering the stoichiometry and the structure of the lattices.

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The Born–Haber Cycle

We can easily measure the enthalpy of formation of NaCl and the ionization energy of sodium. But no instrument can vaporize a solid crystal straight into isolated gaseous ions. How do we find an energy we cannot measure directly?

Enthalpy level diagram of the Born–Haber cycle for sodium chloride connecting the elements, gaseous ions, and the crystal lattice H Na(s) + ½Cl₂(g) Na(g) + ½Cl₂(g) Na⁺(g) + e⁻ + ½Cl₂(g) Na⁺(g) + e⁻ + Cl(g) Na⁺(g) + Cl⁻(g) NaCl(s) sublimation ionization dissociation electron affinity lattice energy formation

Ions with More Than One Charge

Energy level diagram comparing the exothermic first electron affinity and the endothermic second electron affinity of oxygen O(g) EA₁ < 0 O⁻(g) EA₂ > 0 O²⁻(g)

Partial Covalent Character: Fajans' Rules

Sketch of a cation polarizing the electron cloud of an anion, producing partial covalent character Ag⁺ polarizing distorted anion
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Back to the start: Pulling a mole of table salt apart into gaseous ions takes about $+787\ \text{kJ}$. That is a huge energy cost, which is why NaCl is a stable crystalline solid and not a gas of free molecules.

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