More practice problems for exam 4
32) Fill in the table using 0.1 M for all initial conditions and 1 s-1 or 1 M-1s-1 or 1 M-2s-1 as appropriate for all rate constants
|
Reaction |
Differential rate equations |
Initial rates (M/s) |
Final concentrations |
|
A --> B |
dA/dt = -k[A] dB/dt = k[A] |
dA/dt = -0.1 M/s dB/dt = 0.1 M/s |
A =0 M B = 0.2 M |
|
A + B -- > C |
dA/dt = -k[A][B] dB/dt = -k[A][B] dC/dt = k[A][B] |
dA/dt = -0.01 M/s dB/dt = -0.01 M/s dC/dt = 0.01 M/s |
A = 0 M B = 0 M C = 0.2 M |
|
A <--> B |
dA/dt = -kf[A] + kb[B] dB/dt = kf[A] - kb[B] |
dA/dt = 0 M/s dB/dt = 0 M/s |
A = 0.1 M B = 0.1 M |
|
A+B <--> C |
dA/dt = -kf[A][B] + kb[C] dB/dt = -kf[A][B] + kb[C] dC/dt = kf[A][B] - kb[C] |
dA/dt = 0.09 M/s dB/dt = 0.09 M/s dC/dt = -0.09 M/s |
A = 0.1708 M B = 0.1708 M C = 0.0292 M |
|
A --> B -->C |
dA/dt = -k1[A] dB/dt = k1[A] - k2[B] dC/dt = k2[B] |
dA/dt = -0.1 M/s dB/dt = 0 M/s dC/dt = 0.1 M/s |
A = 0 M B = 0 M C = 0.3 M |
|
A <--> B+C --> D |
dA/dt = -kf1[A] + kb1[B][C] dB/dt = kf1[A]- kb1[B][C] -k2[B][C] dC/dt = kf1[A]- kb1[B][C] -k2[B][C] dD/dt = k2[B][C] |
dA/dt = -0.09 M/s dB/dt = 0.08 M/s dC/dt = 0.08 M/s dD/dt = 0.01 M/s |
A = 0 M B = 0 M C = 0 M D = 0.3 M |
|
2A +B <-->C-->D |
dA/dt = 2(-kf1[A]2[B] + kb1[C]) dB/dt = -kf1[A]2[B] + kb1[C] dC/dt = kf1[A]2[B] - kb1[C] - k2[C] dD/dt = kf2[C] |
dA/dt = 0.198M/s dB/dt = 0.099 M/s dC/dt =-0.199M/s dD/dt = 0.1 M/s |
A = 0 M B = 0.05 M C = 0 M D = 0.25 M |
|
A+B<-->C<--> D |
dA/dt = -kf1[A][B] + kb1[C] dB/dt = -kf1[A][B] + kb1[C] dC/dt =kf1[A][B]-kb1[C]-kf2[C]+kb2[D] dD/dt = kf2[C] - kb2[D] |
dA/dt = 0.09 M/s dB/dt = 0.09 M/s dC/dt = -0.09 M/s dD/dt = 0 M/s |
A = 0.2109 M B = 0.2109 M C = 0.04451 M D = 0.04451 M |
A = A0 exp(-k t) so 0.5M = (1 M) exp(-k 10s) or k = -ln(0.5) /10 s = 0.0693 s-1
The first thing to recognize is that the equilibrium constant strongly favors the reactant A. Thus, there is never very much B present in the reaction. We can also see that
dC/dt = 5 s-1 [B]. At equilibrium [B]/[A] = 1/50 so [B] = [A]/50 and therefore dC/dt =5 s-1 [A]/50 = 0.1 (s-1) [A] . Now, since there is little [B] present at any time,
dA/dt ~ -dC/dt = -0.1(s-1) [A] or dA/[A] = -0.1 (s-1) dt. This can be integrated to give
lnA = -0.1 (s-1) t + const., were const. is the constant of integration. As shown in the notes, this can be rearranged and evaluated to give A(t) = A0exp(-0.1s-1 t), where A0 is the initial value of A or 1M in this case since there is little B present at any time. Thus, to find how long it takes to get to the point where half the reaction is over (we started with 1 M A),
0.5M = 1Mexp(-0.1 s-1 t) or
t = ln(0.5) / (-0.1 s-1) = 6.935 seconds.
The steady-state approximation is similar except [B]/[A] = kf1/(k2+kb1) = 1/55. Everything else is the same. You end up with t = ln(0.5)/(-0.0909) = 7.63 seconds. The steady state approximation is probably more accurate in this case since it includes the effect of considering the forward reaction from B to C.
At the two temperatures we can write

Now just solve the two equations simultaneously for EA giving 17.71 kJ/mole.
For the first reaction, the equilibrium constant is Keq1 = 10/1 = 10. The second equilibrium constant is Keq2 = 5/.1 = 50. The equilibrium constant for the overall reaction is just the product of these two since

Given the equilibrium constant for the overall reaction, we can calculate the standard reaction free energy as -RTlnKeq = -(8.314)(298)ln(500) = 15.40 kJ/mole.