When this reaction takes place in a perfectly mixed batch reactor, the mass balance is given by the following equation:

,

where , and are the final reaction time and the time variable, , for and , and are the activation energy and pre-exponential factor, is the ratio of the activation energies, and is the dimensionless temperature.

This mass balance can be integrated to give:

with .

The value of the optimum temperature or can be found for given values of , , and from: at . After the optimum value of is found, the actual optimal temperature is given by: ; the reaction is assumed to be exothermic (i.e., ). This assumption is important for the Demonstration to perform correctly because only for exothermic reactions can one find an optimum temperature. Indeed, high values increase the rate constant but lower the equilibrium conversion. Thus, one must reconcile between competing thermodynamic and kinetic considerations by choosing an appropriate optimal temperature. High is better in the beginning where equilibrium limitations are not important and low is better later when one approaches equilibrium.

The Demonstration plots the optimal dimensionless temperature, , and the corresponding final conversion, , versus parameter for user-set values of the ratio of the activation energies, .