1st order reversible reaction

A 1st order reversible reaction of the type A\rightleftharpoons B is composed of the reactions:

A\rightarrow B\; \; \; \; \; \; \; v_1=k_1[A]

B\rightarrow A\; \; \; \; \; \; \; v_2=k_2[B]

The rate law is:

\frac{d[A]}{dt}=-k_1[A]+k_2[B]

Substitute [B] = [A0] – [A], where [A0] is the initial concentration of A, in the above equation and rearranging, we have.

\frac{d[A]}{dt}=-(k_1+k_2)[A]+k_2[A_0]\; \; \; \; \; \; \; \; 16

Let

x=(k_1+k_2)[A]-k_2[A_0]\; \; \; \; \; \; \; \; 17

Eq16 becomes \frac{d[A]}{dt}=-x. Differentiating eq17 with respect to [A], we have d[A]=\frac{dx}{k_1+k_2}, and differentiating this expression with respect to time, we have \frac{d[A]}{dt}=\frac{1}{k_1+k_2}\frac{dx}{dt}, which is equivalent to

-x=\frac{1}{k_1+k_2}\frac{dx}{dt}\; \; \Rightarrow \; \; -(k_1+k_2)dt=\frac{dx}{x}

Let x = x0 when t =0 and integrate the above expression. We have

-(k_1+k_2)t=lnx-lnx_0\; \; \; \; \; \; \; \; 18

Substitute eq17 in eq18, noting that the 2nd term on RHS of eq18 refers to concentrations at t = 0, where [A] = [A0], 

-(k_1+k_2)t=ln\frac{(k_1+k_2)[A]-k_2[A_0]}{(k_1+k_2)[A_0]-k_2[A_0]}

which rearranges to

[A]=\frac{k_2+k_1e^{-(k_1+k_2)t}}{k_1+k_2}[A_0]\; \; \; \; \; \; \; \; 19

When t = 0, eq19 becomes [A] = [A0]. As t → ∞,

[A_\infty ]=[A_{eqm}]=\frac{k_2}{k_1+k_2}[A_0]

Since [B_{eqm}]=[A_0]-[A_\infty ] ,

[B_{eqm}]=[A_0]-\frac{k_2}{k_1+k_2}[A_0]=[A_0]\frac{k_1}{k_1+k_2}

Therefore, the equilibrium constant for the reaction is:

K=\frac{[B_{eqm}]}{[A_{eqm}]}=\frac{k_1}{k_2}

This is the link between chemical kinetics and thermodynamics.

 

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