Modeling — Question 9

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Question 9

In a closed, well-mixed vessel of constant volume, the reversible reaction A⇌2B\mathrm A\rightleftharpoons 2\mathrm B has forward reaction rate kfak_fa and reverse reaction rate krb2k_rb^2 in mol/(L⋅\cdotmin), where a,ba,b are concentrations in mol/L. Here kf=1k_f=1 min−1^{-1} and kr=1k_r=1 L/(mol⋅\cdotmin). Initially a=1a=1, b=0b=0 mol/L. There are no other reactions. Use numerical concentration values in these units.

Tasks

  1. Derive the concentration equations from the stoichiometric coefficients. Identify a conserved weighted concentration and explain why a+ba+b is not conserved.

  2. Reduce to a scalar equation for bb and identify its physically allowed interval. Show this interval is invariant.

  3. Find the unique physical equilibrium and prove the stated initial response approaches it monotonically in bb.

  4. Solve explicitly for b(t)b(t) by separation, then recover a(t)a(t). Explain why the second algebraic root of the equilibrium equation is inadmissible and why the physical equilibrium is not reached at finite time.

Original worksheet page 1: question and worked solution for 5-12-009
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Question 9 – Solution

Strategy. Each forward reaction consumes one A and creates two B; the resulting weighted conservation law reduces the nonlinear system.

Step 1: Respect the reaction stoichiometry. A net forward reaction rate a−b2a-b^2 gives a′=−a+b2,b′=2a−2b2\boxed{a'=-a+b^2,\qquad b'=2a-2b^2} in the chosen numerical units. Hence (2a+b)′=0(2a+b)'=0 and 2a+b=2\boxed{2a+b=2} mol/L. The sum a+ba+b has derivative a−b2a-b^2 and is not conserved: the reaction changes the number of molecules, while preserving the weighted building-block total.

Step 2: Reduce within the physical domain. With a=1−b/2a=1-b/2, the scalar equation is b′=2−b−2b2\boxed{b'=2-b-2b^2}, with 0≤b≤20\le b\le 2 required by a,b≥0a,b\ge 0. At b=0b=0 the derivative is 2>02>0, and at b=2b=2 it is −8<0-8<0. Uniqueness and inward boundary directions make the interval invariant. The concentrations cannot be extended to negative values merely because an algebraic equation has another root.

Step 3: Identify the attracting physical equilibrium. Let d=17d=\sqrt{17} and r±=(−1±d)/4r_\pm=(-1\pm d)/4. Then b′=−2(b−r+)(b−r−)b'=-2(b-r_+)(b-r_-), with r−<0<r+<2r_-<0<r_+<2. The only physical equilibrium is b*=r+,a*=1−r+/2.\boxed{b_*=r_+,\qquad a_*=1-r_+/2.} For 0≤b<r+0\le b<r_+, b′>0b'>0. Uniqueness prevents crossing the equilibrium, so the solution from zero increases and stays below r+r_+. Its limit must be a zero of the scalar right side; otherwise its positive derivative would remain bounded away from zero. Thus it tends to r+r_+.

Step 4: Separate and impose the initial concentration. Since 2(r+−r−)=d2(r_+-r_-)=d, integration gives log⁡|b−r+b−r−|=−dt+log⁡|r+r−|.\log\left|\frac{b-r_+}{b-r_-}\right|=-dt+ \log\left|\frac{r_+}{r_-}\right|. The ratio is negative on the physical branch starting at zero. Solving gives b(t)=r+(1−e−dt)1−(r+/r−)e−dt,a(t)=1−b(t)2.\boxed{b(t)=\frac{r_+(1-e^{-dt})}{1-(r_+/r_-)e^{-dt}},\qquad a(t)=1-\frac{b(t)}2.} The denominator exceeds 11 at finite times because r+/r−<0r_+/r_-<0. The formulas give (a,b)=(1,0)(a,b)=(1,0) initially and the stated equilibrium as t→∞t\to\infty. For every finite tt, b<r+b<r_+, so arrival is asymptotic.

Original worksheet page 2: question and worked solution for 5-12-009

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