Chemistry Labs

Problem 2

Professor Molina (MIT, Nobel Prize 1995) studied the acid-rain reaction producing HX2SOX4\ce{H2SO4} in the atmosphere and proposed two stoichiometries: Proposal A: HX2O(g)+SOX3(g)→HX2SOX4(g)\ce{H2O(g) + SO3(g) -> H2SO4(g)}; Proposal B: 2 HX2O(g)+SOX3(g)→HX2SOX4(g)+HX2O(g)\ce{2H2O(g) + SO3(g) -> H2SO4(g) + H2O(g)}. (2.1) Using simple collision theory, what reaction orders are expected for A and B? Proposal B is thought to proceed via SOX3+2 HX2O⇌kX−1kX1SOX3 ⋅ 2 HX2O\ce{SO3 + 2H2O <=>[k_1][k_{-1}] SO3.2H2O} (fast) and SOX3 ⋅ 2 HX2O→kX2HX2SOX4+HX2O\ce{SO3.2H2O ->[k_2] H2SO4 + H2O} (slow, k2≪k1,k−1k_2 \ll k_1, k_{-1}). (2.2) Apply the steady-state principle to derive the rate law and order of this mechanism. (2.3) Quantum calculations give overall activation energies EA=+80E_A = +80 kJ mol⁻¹ (A) and EB=−20E_B = -20 kJ mol⁻¹ (B). Write the Arrhenius temperature dependence for each and predict how each rate constant varies with T. (2.4) HX2SOX4\ce{H2SO4} formation is faster in the upper atmosphere (175 K) than at the surface (300 K): which pathway dominates in the upper atmosphere?
Step 2 of 4: Steady-state rate law
d[SOX3 ⋅ 2 HX2O]dt=k1[SOX3][HX2O]2−(k−1+k2)[SOX3 ⋅ 2 HX2O]=0 ⇒ v=k2[SOX3 ⋅ 2 HX2O]=k1k2k−1+k2[SOX3][HX2O]2≈Keqk2[SOX3][HX2O]2\frac{d[\ce{SO3.2H2O}]}{dt} = k_1[\ce{SO3}][\ce{H2O}]^2 - (k_{-1} + k_2)[\ce{SO3.2H2O}] = 0\ \Rightarrow\ v = k_2[\ce{SO3.2H2O}] = \frac{k_1 k_2}{k_{-1} + k_2}[\ce{SO3}][\ce{H2O}]^2 \approx K_{eq}k_2[\ce{SO3}][\ce{H2O}]^2
Analysis

Setting the complex's net rate of formation to zero gives [SOX3 ⋅ 2 HX2O]=k1[SOX3][HX2O]2/(k−1+k2)[\ce{SO3.2H2O}] = k_1[\ce{SO3}][\ce{H2O}]^2/(k_{-1}+k_2). Since k2≪k−1k_2 \ll k_{-1}, the pre-equilibrium is essentially undisturbed and the overall rate is third order with effective constant Keqk2K_{eq}k_2.