Chemical Energetics I – Rapid Review Introduction Thermochemistry: study of heat changes accompanying chemical/physical processes. System: part of universe examined; surroundings: everything else. Heat flows from higher T T T to lower T T T until equilibrium. Enthalpy H H H : energy content at constant pressure (KE + PE); only changes Δ H \Delta H Δ H measurable. Sign convention: Δ H < 0 \Delta H<0 Δ H < 0 exothermic, Δ H > 0 \Delta H>0 Δ H > 0 endothermic. Standard conditions: P = 1 bar , T = 298 K , [ ] = 1 mol dm − 3 P=1\,\text{bar},\;T=298\,\text{K},\;[\;]=1\,\text{mol dm}^{-3} P = 1 bar , T = 298 K , [ ] = 1 mol dm − 3 ; denote by ∘ ^{\circ} ∘ . Key Standard Enthalpy Changes Δ H r ∘ \Delta H_{r}^{\circ} Δ H r ∘ : reaction (stoichiometric amounts).Δ H f ∘ \Delta H_{f}^{\circ} Δ H f ∘ : formation (1 mol compound from elements, standard states).Δ H c ∘ \Delta H_{c}^{\circ} Δ H c ∘ : combustion (complete burn of 1 mol substance).Δ H < e m > n e u t ∘ \Delta H<em>{neut}^{\circ} Δ H < e m > n e u t ∘ : neutralisation (forming 1 mol H < / e m > 2 O \text{H}</em>2\text{O} H < / e m > 2 O ).Δ H a t ∘ \Delta H_{at}^{\circ} Δ H a t ∘ : atomisation (gaseous atoms from element/compound).Bond energy BE \text{BE} BE : average energy to break 1 mol covalent bonds (gaseous). Ionic terms:
• Ionisation energy IE \text{IE} IE (endothermic).
• Electron affinity EA \text{EA} EA (1st usually exo, 2nd endo).
• Lattice energy LE \text{LE} LE (gaseous ions → \rightarrow → solid; exothermic).
• Δ H < e m > h y d ∘ \Delta H<em>{hyd}^{\circ} Δ H < e m > h y d ∘ : hydration of gaseous ion (exo).
• Δ H < / e m > s o l ∘ \Delta H</em>{sol}^{\circ} Δ H < / e m > so l ∘ : solution of ionic solid. Experimental Determination Calorimetry uses Q = m c Δ T Q = mc\Delta T Q = m c Δ T (or Q = C Δ T Q=C\Delta T Q = C Δ T ). Δ H = − Q n \Delta H = -\dfrac{Q}{n} Δ H = − n Q for exothermic, + Q n +\dfrac{Q}{n} + n Q for endothermic; n n n = moles as defined.Assumptions: negligible heat losses, density ≈ \approx ≈ 1 g cm − 3 1\,\text{g cm}^{-3} 1 g cm − 3 , c ≈ 4.18 J g − 1 K − 1 c\approx4.18\,\text{J g}^{-1}\text{K}^{-1} c ≈ 4.18 J g − 1 K − 1 . Temperature correction via extrapolated T < e m > m a x / T < / e m > m i n T<em>{max}/T</em>{min} T < e m > ma x / T < / e m > min to account for losses. Combustion calorimetry: heat water; adjust for efficiency. Bond‐Energy Calculations For gaseous reactions: Δ H ∘ = ∑ BE(bonds broken) − ∑ BE(bonds formed) \Delta H^{\circ}=\sum \text{BE(bonds broken)}-\sum \text{BE(bonds formed)} Δ H ∘ = ∑ BE(bonds broken) − ∑ BE(bonds formed) . For diatomic gas X < e m > 2 X<em>2 X < e m > 2 : BE ( X − X ) = 2 Δ H < / e m > a t ∘ ( X < e m > 2 ) \text{BE}(X-X)=2\,\Delta H</em>{at}^{\circ}(X<em>2) BE ( X − X ) = 2 Δ H < / e m > a t ∘ ( X < e m > 2 ) (only if X < / e m > 2 X</em>2 X < / e m > 2 is gaseous at 298 K). Factors Affecting Ionic Energetics Lattice energy magnitude ∝ q + q − r + + r − \propto \dfrac{q^{+}q^{-}}{r^{+}+r^{-}} ∝ r + + r − q + q − .
• Higher charge, smaller radii ⇒ \Rightarrow ⇒ more exothermic LE \text{LE} LE . Hydration energy ∣ Δ H h y d ∘ ∣ ↑ \left|\Delta H_{hyd}^{\circ}\right| \uparrow Δ H h y d ∘ ↑ with higher charge density. Δ H < e m > s o l ∘ = Δ H < / e m > h y d ∘ ( cation ) + Δ H < e m > h y d ∘ ( anion ) − LE \Delta H<em>{sol}^{\circ}=\Delta H</em>{hyd}^{\circ}(\text{cation})+\Delta H<em>{hyd}^{\circ}(\text{anion})-\text{LE} Δ H < e m > so l ∘ = Δ H < / e m > h y d ∘ ( cation ) + Δ H < e m > h y d ∘ ( anion ) − LE .
• Negative Δ H < / e m > s o l ∘ \Delta H</em>{sol}^{\circ} Δ H < / e m > so l ∘ favours solubility.Enthalpy change independent of path: sum round any cycle = 0 =0 = 0 . Useful identities:
• Δ H < e m > r ∘ = ∑ Δ H < / e m > f ∘ ( products ) − ∑ Δ H < e m > f ∘ ( reactants ) \Delta H<em>{r}^{\circ}=\sum \Delta H</em>{f}^{\circ}(\text{products})-\sum \Delta H<em>{f}^{\circ}(\text{reactants}) Δ H < e m > r ∘ = ∑ Δ H < / e m > f ∘ ( products ) − ∑ Δ H < e m > f ∘ ( reactants )
• Δ H < / e m > r ∘ = ∑ Δ H < e m > c ∘ ( reactants ) − ∑ Δ H < / e m > c ∘ ( products ) \Delta H</em>{r}^{\circ}=\sum \Delta H<em>{c}^{\circ}(\text{reactants})-\sum \Delta H</em>{c}^{\circ}(\text{products}) Δ H < / e m > r ∘ = ∑ Δ H < e m > c ∘ ( reactants ) − ∑ Δ H < / e m > c ∘ ( products )
• Δ H < e m > s o l ∘ = [ Δ H < / e m > h y d ∘ ( ions ) ] − LE \Delta H<em>{sol}^{\circ}=\big[\Delta H</em>{hyd}^{\circ}(\text{ions})\big]-\text{LE} Δ H < e m > so l ∘ = [ Δ H < / e m > h y d ∘ ( ions ) ] − LE Apply via energy cycles, energy-level diagrams, algebraic manipulation. Atomise elements: Δ H < e m > a t ∘ ( M ) + 1 2 Δ H < / e m > a t ∘ ( X 2 ) \Delta H<em>{at}^{\circ}(M)+\tfrac12\Delta H</em>{at}^{\circ}(X_2) Δ H < e m > a t ∘ ( M ) + 2 1 Δ H < / e m > a t ∘ ( X 2 ) . Ionise metal: IEs \text{IEs} IEs . Add electrons to non-metal: EAs \text{EAs} EAs . Lattice formation: LE \text{LE} LE . Overall: Δ H < e m > f ∘ = ∑ Δ H < / e m > a t ∘ + ∑ IE + ∑ EA + LE \Delta H<em>{f}^{\circ}=\sum \Delta H</em>{at}^{\circ}+\sum \text{IE}+\sum \text{EA}+\text{LE} Δ H < e m > f ∘ = ∑ Δ H < / e m > a t ∘ + ∑ IE + ∑ EA + LE . Quick Reference Equations Heat: Q = m c Δ T Q=mc\Delta T Q = m c Δ T . Reaction enthalpy (gaseous, bonds): Δ H = Σ B E < e m > b r e a k − Σ B E < / e m > f o r m \Delta H=\Sigma BE<em>{break}-\Sigma BE</em>{form} Δ H = Σ BE < e m > b re ak − Σ BE < / e m > f or m . Solution: Δ H < e m > s o l ∘ = Δ H < / e m > h y d ∘ ( + ) + Δ H h y d ∘ ( − ) − LE \Delta H<em>{sol}^{\circ}=\Delta H</em>{hyd}^{\circ}(+) + \Delta H_{hyd}^{\circ}(-) - \text{LE} Δ H < e m > so l ∘ = Δ H < / e m > h y d ∘ ( + ) + Δ H h y d ∘ ( − ) − LE . Lattice trends: more exothermic with ↑ q \uparrow q ↑ q , ↓ r \downarrow r ↓ r . Stability Indicators Negative Δ H < e m > f ∘ \Delta H<em>{f}^{\circ} Δ H < e m > f ∘ or more exothermic LE \text{LE} LE /Δ H < / e m > h y d \Delta H</em>{hyd} Δ H < / e m > h y d ⇒ \Rightarrow ⇒ higher thermodynamic stability. Less negative or positive Δ H f ∘ \Delta H_{f}^{\circ} Δ H f ∘ implies relative instability toward elemental decomposition.