The Critical Temperature

The Semenov theory provides an easy method for calculating the critical temperature Tcritical. As can be seen from figure 2, the critical temperature occurs when the heat loss line [Greek letter phi with a -] is at a tangent to the heat gain curve [Greek letter phi with a +]. This means that the values of [Greek letter phi with a -] and [Greek letter phi with a +] must be equal. This gives a way of calculation Tcritical this is shown below.

[Beginning of derivation for the critical temperature]

At the critical temperature the gradients will also be equal. Therefore differentiating the above equation with respect to temperature results in the following equation.

[Differential of equation above]

At the critical temperature for both the above equations to be true then the following must also be true.

[Resultant of the above 2 equations]

For a large value of the activation energy EA, the value of Tc and the value of Ta become very close and the following result can be stated.

[Result of Tc and Ta been close at a large activation energy]

This equation can now be rearranged to give the approximate equation for Tc

[Equation 4 - Approximate value for the critical temperature]
Equation 4 - Approximate value equation for the critical temperature

(All variables in this equation are defined in equation 1 and equation 2

The above equation is a good approximation for the calculation of the critical temperature and can be used in most cases. However in some cases it may be better to get a more exact value of the critical temperature. To do this, instead of assuming a large activation energy as before, we rearrange the equation into a quadratic form. This is shown below.

[Previous Equation]
[Quadratic form of the above equation]

Using the quadratic roots equation the following derivation can be formed

[Rearrangment of above equation into quadratic roots equation]

This leads to the following 2 roots

[Root 1]
[Root 2]

The first root is not likely to occur because it results in very high values for the critical temperature, which will not be physically possible, generally. Therefore that root can be discarded. The second root, however, does provide a value for critical temperature, and it will give a far more accurate result than equation 4.

Examples and questions for both the approximate equation and the more exact value are presented at after the Frank-Kamenetskii section.


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