Lecture 4 Chapter 4 Internal energy and enthalpy changes associate with the chemical reactions H = qp; H = Hf-Hi; Cp = dH/dT (slope of curve) • A) phase transitions: solid liquid liquid solid liquid gas gas liquids solid gas gas solid melting; fusion (fusH) freezing vaporization (vapH ) condensation sublimation (subH ) deposition Solid liquid gas Water fusH = 6.01 kJ vapH = 40.7 kJ Methane fusH = 0.94 kJ vapH = 8.2 kJ Standard molar enthalpy Hm H Transition under standard conditions : 1 Hforward Hreverse mol of pure substance at 1 bar (s )-> 1 mol of pure substance (l) at 1 Hforward = - Hreverse bar Standard state of substance – pure substance at 1 bar (temperature and physical state has to be specified) gas liquid solid subH = fusH + vapH At constant T Enthalpy of ionization Ionization: H(g) H+(g) + e- (g) ionH = 1312 kJ energy (heat) that must be supplied to ionize 1 mol of H (g) at 1bar The standard enthalpy of sublimation for Mg (s) is 148 kJ mol-1 at 295 K. How much energy (heat; at constant T and P) must be supplied to 1 mol of magnesium metal to produce Mg2+ and electrons H = subH + H (first ion)+ H (second ion) H = 2337 kJ Mg 2+(g) + e- (g) 1451 kJ Mg +(g) + e- (g) H 738 kJ 148kJ Electron gain: H+(g) + e- (g) H(g) Standard enthalpy of electron gain egH = -ionH Mg (g) Mg (s) Note: The enthalpy for first ionization is smaller than enthalpy for second ionization • Bond enthalpies - Energy (heat) to be supply to dissociate a covalent bond Potential energy curve for diatomic molecule U N2 -> 2 N H = 945 kJ mol-1 r - Value depends on molecules H-O-H (g) -> H-O (g) + H (g) H = 499 kJ mol-1 H-O (g) -> O (g) + H (g) H = 428kJ mol-1 Accurate determination is complicated since it has to be done for each specific molecules Mean bond enthalpies HB - mean bond enthalpy based on several similar compounds Bond dissociation enthalpy – precisely measured value Bond energy R – equilibrium distance H = 436.3 kJ mol-1 U = 432 kJ mol-1 H = U + pV Bond energy Bond enthalpy (work term (1 mol -> 2 mols) and molecule has rotational and vibration energy Resonance energy Molecules with conjugated double bonds are more stable, the difference in stability is called resonance energy fH (benzene,g) = 82.93 kJ as measured fH (benzene) = 241 kJ based on bound enthalpies Molecules with conjugated double bounds are more stable than those with single/double bound only • Problem: Estimate the enthalpy of combustion for methane using the bond enthalpy values Chemical Change and Reaction enthalpy CH2=CH2 + H2 CH3 –CH3 H = -137 kJ heat due to the cleavage/formation of covalent bond A) Combustion CH4(g) + 2O2 (g) CO2 (g)+ 2H2O (l ) cH = -890 kJ standard enthalpy of combustion – change in standard enthalpy per mol of combustible substance ; measured using bomb calorimetry B) Standard enthalpy of formation rH = fH (products) - fH (reactants) - stoch. coeffic. fH - standard molar enthalpy of formation – enthalpy change when 1 mol of a compound is formed from its constituent element at 1 bar and 298 K. C (s, graphite) + O2 (g) CO2 (g) H 395 kJ mol-1 rH = 1xfH (CO2) – [1xfH (C, graphite) + 1xfH (O2)] fH (CO2) = 395 kJ fH (C, graphite) = 0 fH (O2) = 0 By convention, fH are assigned to be zero for elements in their most stable allotropic form rH = 395 kJ mol-1 – (0 kJ mol-1 + 0 kJ mol-1) = 395 kJ mol-1 fH (C, diamond) = 1.90 kJ mol-1 fH (O3) = 147. 7 kJ mol-1 For compounds that can be synthesized from their elements, the reaction enthalpy can be determined directly. Problem: calculated the value of rH for reacting 1 g of solid glycylclycine with oxygen to form solid urea, CO2 and liquid water at 1 atm and 25 oC using tabulated enthalpy of formation. Indirect methods for determination of reaction enthalpy - Most of the compound can not be synthesized from their elements, thus the enthalpy of formation can not be measured directly Hess law: when reactant are converted into products, the change in enthalpy is the same whether the reaction takes place in one step or multiple steps Find the value of fH for carbon monoxide formation C + 1/2O2 CO 1) C (graphite) + O2 CO2 2 CO(g) + 1/2 O2 CO2 rH = -393.5 kJ mol-1 rH = -283 kJ mol-1 rH (C+ ½ O2) + rH (CO+ ½ O2) = rH (C+O2) CO + ½ O2 rH = -283 kJ mol-1 C + O2 rH CO2 = -393.5 kJ mol-1 rH (C+ ½ O2) + -283 kJ mol-1 = -393.5 kJ mol-1 rH (C+ ½ O2) = -110.5 kJ mol-1. • Temperature dependence of enthalpy of reaction rH = fH (products) - fH (reactants) ( rH/ T)P = [H (products) /T]P - [H (reactants )/T]P = Cp (products) - Cp (reactants) = Cp different in the heat capacities of products and reactants ∆𝐻 𝑇2 𝑇2 Thus: 𝑑∆𝐻 = ∆𝐻 𝑇1 ∆𝐶𝑝 𝑑𝑇 𝑇1 ∆𝐻 𝑇2 − ∆𝐻 𝑇1 = ∆𝐶𝑝(𝑇2 − 𝑇1) H(T2) = H(T1) + Cp (T2-T1) Kirchhoff’s law Problem: The standard enthalpy change for the reaction formation of ozone is 285.4 kJ mol-1 at 295 K. Calculate the value at 380 K. Assume that heat capacities are temperature dependent. • The energy change for the reaction (U) U = H - (PV) At constant pressure: U = H - PV For solids and liquids, V is small and thus U ~ H For gases (using perfect gas approximation) and at constant temperature U = H - RTn where n corresponds to n(products) - n(reactants) • calorimetry - Constant volume calorimetry Bomb container + water are isolated from surrounding => no heat exchange adiabatic process Steel container – constant volume Considering bomb – system and water bath surrounding U = U(system) + U (surrounding) = 0 and U(system) = - U(surrounding) Cv – determined independently T is measured And U = is then calculated H =U +RTn U(system) = qv –p V U = qv = -Cv (T2-T1) Cv is heat capacity of the bomb calorimeter • Differential scanning calorimetry Sample and the reference are slowly heated electrically in such matter that the T of sample and reference reminds the same. H = CpdT Protein denaturation: For 2 state unfolding: N U Tm corresponds to the temperature when 50 % protein is in folded state H = 200 kJ mol-1 to 800 kJ mol-1 Homework 4 • Homework: 2.27; 2.28; 2.29; 2.30; 3.32 (3.35); 3.31 (3.34); 3.29 (3.32) 3.26 (3.29), 3.27 (3.30) 3.25 (3.28); 3.22 (3.26); 3.10 (3.14); 3.11 (3.15); 3.17 (3.21)
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