For adiabatic operation![]() ![]() |
|||
|
(9-13) | ||
where![]() |
|||
|
(9-15) | ||
multiplying by dt, separating variables and integrating between the initial conditions, X = 0 and T =T0, and later conditions X =X and T =T, yields | |||
|
|||
Taking the antilog, we have | |||
![]() |
|||
solving for X yields | |||
![]() |
|||
Then | |||
![]() |
(9-16) | ||
This form is the same as the equation relating X and T derived for flow reactors. Rearranging yields | |||
Temperature |
![]() |
(9-17) |