Chapter 36: Problem 13
In the discussion of the Lindemann mechanism, it was assumed that the rate of activation by collision with another reactant molecule \(A\) was the same as collision with a nonreactant molecule M such as a buffer gas. What if the rates of activation for these two processes are different? In this case, the mechanism becomes \\[ \begin{array}{l} \mathrm{A}+\mathrm{M} \quad \underbrace{k_{1}}{=} \mathrm{A}^{*}+\mathrm{M} \\\ \mathrm{A}+\mathrm{A} \stackrel{k_{-1}}{=} \mathrm{k}_{-2} \\ \mathrm{A}^{*} \stackrel{\mathrm{k}_{3}}{\longrightarrow} \mathrm{P} \end{array} \\] a. Demonstrate that the rate law expression for this mechanism is \\[ R=\frac{k_{3}\left(k_{1}[\mathrm{A}][\mathrm{M}]+k_{2}[\mathrm{A}]^{2}\right)}{k_{-1}[\mathrm{M}]+k_{-2}[\mathrm{A}]+k_{-3}} \\] b. Does this rate law reduce to the expected form when \([\mathrm{M}]=0 ?\)
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