KINETICS OF BRANCHED CHAIN REACTION

One general gaseous reaction in which A is the reactant, R is a reactive chain carrier, P is the product, and α is the number of chain carriers produced by one carrier in the propagation step so that we can write it as,

\[\displaystyle A\underset{{}}{\overset{{\mathop{K}_{1}}}{\longrightarrow}}R(\text{chain Initiation})\]
\[\displaystyle R+A\underset{{}}{\overset{{\mathop{K}_{2}}}{\longrightarrow}}P+2R(\text{chain Propagation})\]
\[\displaystyle R\underset{{}}{\overset{{\mathop{K}_{3}}}{\longrightarrow}}destruction(\text{termination})\]

The chain carrier is destroyed by collision with other molecules or collision against the walls of the vessels. The rate of formation of chain carrier is given by,

\[\displaystyle \frac{{d\left[ R \right]}}{{dt}}={{k}_{1}}\left[ A \right]-{{k}_{2}}\left[ R \right]\left[ A \right]+\alpha {{k}_{2}}\left[ R \right]\left[ A \right]-{{k}_{3}}\left[ R \right]---(1)\]

The steady-state approximation for the chain carrier, i.e.

\[\displaystyle \frac{{d\left[ R \right]}}{{dt}}=0,\]
\[\displaystyle \left[ R \right]=\frac{{{{k}_{1}}\left[ A \right]}}{{{{k}_{2}}\left[ A \right]\left( {1-\alpha } \right)+{{k}_{3}}}}----(2)\]

Here, k3 = constant for considered equal to the sum of two terms, kw for the wall reaction and kg for the gas phase reaction, so, equation (2) we can write as,

\[\displaystyle \left[ R \right]=\frac{{{{k}_{1}}\left[ A \right]}}{{{{k}_{2}}\left[ A \right]\left( {1-\alpha } \right)+{{k}_{w}}+{{k}_{g}}}}----(3)\]

According to equation (3), consider the following cases;

Case:1: when α =1

Each propagation step of the reaction results in the formation of a product molecule with the regeneration of only one chain carrier, a reaction known as non- branched or stationary chain reaction.

In these reactions, the radical concentration α ratio of its formation rate to the decomposition rate.

An example of this reaction is the Pyrolysis of several organic compounds.

Case:2: when α>1

More than on-chain carriers are produced in the propagation sequences of the reaction called non-stationary chains or Branched chains reaction.

Case:3: when α>>1

Many chain carriers are produced in the propagation sequence; the concentration carrier [R] is almost infinite. The reaction rate also becomes almost infinite, resulting in explosions called isothermal explosions.

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Bhoomika Sheladiya

BSc. (CHEMISTRY) 2014- Gujarat University
MSc. (PHYSICAL CHEMISTRY) 2016 - School of Science, Gujarat University

Junior Research Fellow (JRF)- 2019
AD_HOC Assistant Professor-(July 2016 to November 2021)

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