ok, so ignore the first post please
the equation is
[tex]\frac { d^2 \theta }{d x'^2 } = -y *exp(\theta)[/tex] eq. 1
first off, this is a steady state model. meaning, we consider the pre-explosion temperature to be small in comparison with the absolute temperature of the walls:[tex]\frac {\Delta T}{T} << 1[/tex]
2nd, the reaction rate only depends on the deperature in accordance with exp(-E/RT)
3rd we regad the thermal conductivity of the walls as being infinitely large.
x' = x/r is the nondimensionalization of x, r is the half length (i.e radius for cylinder), not the derivative, for -L < x < L we have -1 < x' < 1. x' drops unit (i.e m, cm, ..)
theta is the nondimensionalization of temperature [tex]\theta = \frac {E}{RT^2_a} *(T - T_a)[/tex]
y (although i used a different variable) is known as the frank kamenetskii parameter
[tex]y = \frac {Q}{d}*\frac {E}{R*T^2_a}*r^2*z* exp(\frac {-E}{RT_a})[/tex]
E: activation energy
T_a: ambient temperature
Q: heat released
z: frequency of particle collision
r: radius or half width (depending on geometry)
R: gas constant
d: thermal conductivity
all uniform except Q, i think..
the book solves the differential equation 1, analytically, for a function [tex]\theta = f(y,x')[/tex] in case of high activation energy E. RT<<E
the book gives the following result.
[tex]exp(\theta) = \frac {a}{cosh^2(b \frac{+}{-} \sqrt \frac{a*y}{2} * x')}[/tex]
im just trying to figure out what steps I need to take in order to arrive at the last solution.