Table of contents | |
Introduction | |
Parallel Reactions | |
Consecutive Reactions | |
Consecutive Reactions With an Equilibrium | |
Steady-State Approximations | |
Lindemann Mechanism | |
Equilibrium Approximations |
A major goal in chemical kinetics is to determine the sequence of elementary reactions, or the reaction mechanism, that comprise complex reactions. For example, Sherwood Rowland and Mario Molina won the Nobel Prize in Chemistry in 1995 for proposing the elementary reactions involving chlorine radicals that contribute to the overall reaction of O3 → O2 in the troposphere. In the following sections, we will derive rate laws for complex reaction mechanisms, including reversible, parallel and consecutive reactions.
Consider the reaction in which chemical species A undergoes one of two irreversible first order reactions to form either species B or species C:
The overall reaction rate for the consumption of A can be written as:
Integrating [A] with respect to t, we obtain the following equation:
Plugging this expression into the equation for
Integrating [B] with respect to t, we obtain:
At t = 0, [B] = 0. Therefore,
Likewise,
The ratio of [B] to [C] is simply:
An important parallel reaction in industry occurs in the production of ethylene oxide, a reagent in many chemical processes and also a major component in explosives. Ethylene oxide is formed through the partial oxidation of ethylene:
However, ethylene can also undergo a combustion reaction:
To select for the first reaction, the oxidation of ethylene takes place in the presence of a silver catalyst, which significantly increases k1 compared to k2. Figure 9.4.1 displays the concentration profiles for species A, B, and C in a parallel reaction in which k1 > k2.
Consider the following series of first-order irreversible reactions, where species A reacts to form an intermediate species, I, which then reacts to form the product, P:
We can write the reaction rates of species A, I and P as follows:
As before, integrating [A] with respect to t leads to:
The concentration of species I can be written as
Then, solving for [P], we find that:
Figure 9.4.2 displays the concentration profiles for species A, I, and P in a consecutive reaction in which k1 = k2. As can be seen from the figure, the concentration of species I reaches a maximum at some time, tmax. Oftentimes, species I is the desired product. Returning to the oxidation of ethylene into ethylene oxide, it is important to note another reaction in which ethylene oxide can decompose into carbon dioxide and water through the following reaction
Thus, to maximize the concentration of ethylene oxide, the oxidation of ethylene is only allowed proceed to partial completion before the reaction is stopped.
Finally, in the limiting case when k2 ≫ k1, we can write the concentration of P as
Thus, when k2 ≫ k1, the reaction can be approximated as A → P and the apparent rate law follows 1st order kinetics.
Consider the reactions
We can write the reaction rates as:
The exact solutions of these is straightforward, in principle, but rather involved, so we will just state the exact solutions, which are
where
Consider the following consecutive reaction in which the first step is reversible:
We can write the reaction rates as:
These equations can be solved explicitly in terms of [A], [I], and [P], but the math becomes very complicated quickly. If, however, k2 + k−1 ≫ k1 (in other words, the rate of consumption of I is much faster than the rate of production of I ), we can make the approximation that the concentration of the intermediate species, I, is small and constant with time:
Equation 21.22 can now be written as
where [I]ss is a constant represents the steady state concentration of intermediate species, [I]. Solving for [I]ss,
We can then write the rate equation for species A as
Integrating,
Equation 21.28 is the same equation we would obtain for apparent 1st order kinetics of the following reaction:
where
Figure 9.4.3 displays the concentration profiles for species, A, I, and P with the condition that k2 + k−1 ≫ k1. These types of reaction kinetics appear when the intermediate species, I, is highly reactive.
Consider the isomerization of methylisonitrile gas, CH3NC, to acetonitrile gas, CH3CN:
If the isomerization is a unimolecular elementary reaction, we should expect to see 1st order rate kinetics. Experimentally, however, 1st order rate kinetics are only observed at high pressures. At low pressures, the reaction kinetics follow a 2nd order rate law:
To explain this observation, J.A. Christiansen and F.A. Lindemann proposed that gas molecules first need to be energized via intermolecular collisions before undergoing an isomerization reaction. The reaction mechanism can be expressed as the following two elementary reactions
where M can be a reactant molecule, a product molecule or another inert molecule present in the reactor. Assuming that the concentration of A∗ is small, or k1 ≪ k2 + k−1, we can use a steady-state approximation to solve for the concentration profile of species B with time:
Solving for [A∗],
The reaction rates of species A and B can be written as
where
At high pressures, we can expect collisions to occur frequently, such that k−1[M] ≫ k2. Equation 21.33 then becomes
which follows 1st order rate kinetics.
At low pressures, we can expect collisions to occurs infrequently, such that k−1[M] ≪ k2. In this scenario, equation 21.33 becomes
which follows second order rate kinetics, consistent with experimental observations.
Consider again the following consecutive reaction in which the first step is reversible:
Now let us consider the situation in which k2 ≪ k1 and k−1. In other words, the conversion of I to P is slow and is the rate-limiting step. In this situation, we can assume that [A] and [I] are in equilibrium with each other. As we derived before for a reversible reaction in equilibrium,
or, in terms of [I],
These conditions also result from the exact solution when we set k2 ≈ 0. When this is done, we have the approximate expressions from the exact solution:
and the approximate solutions become
In the long-time limit, when equilibrium is reached and transient behavior has decayed away, we find
Plugging the above equation into the expression for d[P]/dt,
The reaction can thus be approximated as a 1st order reaction
with
Figure 9.4.4 displays the concentration profiles for species, A, I, and P with the condition that k2 ≪ k1 = k−1. When k1 = k−1, we expect [A] = [I]. As can be seen from the figure, after a short initial startup time, the concentrations of species A and I are approximately equal during the reaction.
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