Level: 4 (Application — novel problems, no hints)
Time: 60 minutes
Total marks: 50
Use R=8.314J K−1mol−1 unless a value is supplied. Assume ideal gas behaviour where relevant.
Question 1 (10 marks)
Two moles of an ideal monatomic gas (Cv,m=23R) at 300K occupy 10.0L. The gas is expanded isothermally to 30.0L.
(a) Calculate q, w, ΔU and ΔH if the expansion is carried out reversibly. (5)
(b) The same initial-to-final change is instead carried out irreversibly against a constant external pressure equal to the final gas pressure. Calculate w and q for this path. (3)
(c) State, with a one-line justification, which quantities in (a) and (b) differ and which are identical, relating this to state vs path functions. (2)
Question 2 (10 marks)
Consider the reaction at 298K and constant pressure:
C2H4(g)+H2(g)→C2H6(g)
(a) Using the bond enthalpies below, estimate ΔHrxn:
C=C 612, C–C 348, C–H 412, H–H 436 (all kJ mol−1). (4)
(b) The value from standard enthalpies of formation is −137kJ mol−1. Account for the discrepancy in one or two sentences. (2)
(c) For this reaction determine ΔUrxn at 298K using the formation-based ΔH. (2)
(d) Predict, without a numerical entropy calculation, the sign of ΔSrxn and hence comment on how ΔG behaves as temperature rises. (2)
Question 3 (10 marks)
Construct a Born–Haber cycle to find the lattice enthalpyΔHL (defined as Na+(g)+Cl−(g)→NaCl(s)) from:
ΔHf∘[NaCl(s)]=−411kJ mol−1
Sublimation of Na =+108
21 bond dissociation of Cl2=+121
Ionisation energy of Na =+496
Electron affinity of Cl =−349 (all kJ mol−1)
(a) Draw/describe the cycle and calculate ΔHL. (6)
(b) A student proposes that replacing Na by K (larger cation) would make ΔHL more exothermic. Evaluate this claim. (2)
(c) State whether the sign of your ΔHL is consistent with a favourable lattice formation and why. (2)
Question 4 (12 marks)
For the reaction N2O4(g)⇌2NO2(g):
ΔH∘=+57.2kJ mol−1,ΔS∘=+175.8J K−1mol−1
(a) Calculate ΔG∘ at 298K and state whether the forward reaction is spontaneous under standard conditions. (3)
(b) Determine the temperature above which the forward reaction becomes spontaneous at standard conditions. (3)
(c) Calculate the equilibrium constant K at 298K. (3)
(d) Estimate K at 400K assuming ΔH∘ and ΔS∘ are temperature-independent, and comment on the direction of shift. (3)
w=−nRTln(V2/V1)=−(2)(8.314)(300)ln3ln3=1.0986, so w=−4988.4×1.0986=−5480J≈−5.48kJ(1)
Isothermal ideal gas ⇒ ΔU=0(1), ΔH=0(1) (both depend only on T).
First law ΔU=q+w=0⇒q=−w=+5.48kJ(1)
Sign logic: gas does work on surroundings (w<0), absorbs equal heat. (1)
(b) Irreversible against Pext=Pfinal
Pfinal=V2nRT=30×10−32×8.314×300=1.663×105Pa(1)w=−PextΔV=−1.663×105(30−10)×10−3=−3326J≈−3.33kJ(1)ΔU=0 (state function, same endpoints) ⇒ q=+3.33kJ(1)
(c)ΔU and ΔH are identical in both (state functions, path-independent). q and w differ (path functions); the reversible path extracts maximum work. (2)
(d)Δng=−1 (2 gas mol → 1) ⇒ ΔSrxn<0. (1) With ΔH<0, ΔS<0: ΔG=ΔH−TΔS becomes less negative as T rises, so reaction becomes less favourable (eventually non-spontaneous) at high T. (1)
(c)ΔG is a state function and additive; a large negative ΔG∘ (ATP hydrolysis) coupled to a positive one makes the sum negative, so the overall process is spontaneous even though one step alone is not. (2)
[ {"claim":"Q1a reversible work ≈ -5480 J","code":"import sympy as sp\nw=-2*8.314*300*sp.log(3)\nresult = abs(float(w)+5480) < 5"}, {"claim":"Q2a bond-energy ΔH = -124 kJ/mol","code":"broken=612+4*412+436\nformed=348+6*412\nresult = (broken-formed)==-124"}, {"claim":"Q3 lattice enthalpy = -787 kJ/mol","code":"dHL=-411-(108+121+496-349)\nresult = dHL==-787"}, {"claim":"Q4b crossover T ≈ 325.4 K","code":"T=57200/175.8\nresult = abs(T-325.4)<0.5"}, {"claim":"Q4c K(298) ≈ 0.143","code":"import sympy as sp\nK=sp.exp(-4812/(8.314*298))\nresult = abs(float(K)-0.143)<0.005"}, {"claim":"Q5b coupled K ≈ 846","code":"import sympy as sp\nK=sp.exp(16700/(8.314*298))\nresult = abs(float(K)-846)<10"}]