Solving a 2nd Order Differential Equation with Exponential Terms

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The discussion revolves around solving a second-order differential equation with exponential terms, specifically the equation d²θ/dx'² = -y * exp(θ). Participants explore the transformation of variables and the implications of treating y as a constant during integration. The conversation highlights the confusion regarding the transition from ordinary to partial derivatives and the interpretation of the Frank-Kamenetskii parameter. Participants also discuss the integration process and how to express the solution in a form consistent with textbook results, particularly addressing the constants and the presence of both positive and negative signs in the solution. The thread concludes with a collaborative effort to clarify the solution's form and constants.
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Homework Statement



\frac { d^2 \theta }{d x'^2 } = -y *exp(\theta) eq. 1

mayb be integrated to yield

exp(\theta) = \frac {a}{cosh^2(b \frac{+}{-} \sqrt \frac{a*y}{2} * x')}

\theta = f(y,x')

Homework Equations


The Attempt at a Solution



the exponent is throwing me off, but i probably have to use the following properties

\frac { d^2 \theta }{d x'^2 } + \sqrt{y}*exp(/theta) = 0


g = [1/2 (e^k^x + e^-^k^x)]^2 = cosh^2(kx)

the problem is the exp(theta), do I have to replace the variable with something like

g = ln(theta)

then find

\frac { d^2 g }{d x'^2 }

to get

\frac { d^2 g }{d x'^2 } + \sqrt{y}*g = 0

then apply

m^2 + k^2 = 0?

thanks
 
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I'm confused. In the other thread you started, you have
\frac { \partial^2 \theta }{\partial x'^2 } = -y *exp(\theta)
and in this one you have it as a 2nd-order ODE.
Since theta is a function of y and x', you really need partial derivatives, not ordinary derivatives. If theta were a function of a single variable, say x', then you could talk about d(theta)/dx' and d^2(theta)/dx'^2.

Having said that, how do you go from equation 1 to this equation? IOW, how did y in the first equation become sqrt(y) in this equation?
\frac { d^2 \theta }{d x'^2 } + \sqrt{y}*exp(\theta) = 0
 
sorry, at first it was a partial derivative but then I realized that theta is only dependent on the spatial variable x', like you said. Since this is a steady state problem (conditions for the problem approaching a steady state are given by the rate of reaction, it reduces to a ODE

Anyway,

I found more info on how to solve the equation

x' = \int \frac{d \theta}{\sqrt{-2*\int -y*exp(\theta) d \theta}}

then i get

x' = \int \frac {d\theta}{\sqrt{2*y*exp(\theta) + 2*y*c}}and now I am trying to figure out the above integral.
 
Last edited:
Factor 2y out of the terms in the radical and bring them out of the radical and out of the integral so that you have exp(theta) + c in the radical. I would then see if a substitution would work.
 
ok so following ur suggestion i did

x' = \frac {1}{\sqrt{2y}} * \int \frac {d\theta}{\sqrt{\int exp(\theta)d\theta}}

x' = \frac {1}{\sqrt{2y}} * \int \frac {d\theta}{\sqrt{ exp(\theta)+c}}

then i use the identity for int 1/sqrt(theta^2 + a^2) that is

x' = \frac {1}{\sqrt{2y}} * ln | exp(\theta/2) + \sqrt{exp(\theta) + c} | + a

but when i try to solve for theta, i don't know how to reduce the exp to fit the form of the solution the book gives for exp(theta)
 
Not sure if this will help, but the integral formula you used can be expressed another way.
\int \frac{dx}{\sqrt{x^2 + a^2}}~=~sinh^{-1}(x/a) + C

One thing I've been bothered by is treating y as if it were a constant in the integration with respect to theta. You have theta = f(y, x'), and in the other thread you said that y = x/x'.
 
hey mike, thanks so much for your hlep. yes that identity definitely helps.

please try to ignore the other post

y here is known as the frank-kamenetskii parameter

y = \frac {E}{RT^2_a} \frac {Q}{h} *r^2*z*exp(-E/RT_a)

now, the r^2 in the y comes from x' = x/r

this is the substitution to drop the units of x, where r can be the half width or radius of a cylinder.

specifically, by the chain rule

\Delta x' = r^2 \Delta

Quoting the book, In the simplest problems, the boundary condition is \theta = 0 at the surface, and the critical condition reduces to y = const = y_c_r_i_t since neither in the equation nor in the boundary condions are there any parameters other than y.

So i think its ok to factor out y, no?
 
Last edited:
That's Mark...
You have \Delta x' = r^2 \Delta
Don't you mean this?
\Delta x' = \Delta r^2
Based on what you said about y, sounds like you can move it out of the integral.
 
sorry, mark :)

I still don't get the same answer as in the book

I did

x' = \frac {1}{\sqrt{2y}} * sech^-^1 (\frac {exp(\frac {\theta}{2})}{\sqrt{c}}) + a

when I solve for exp(\theta) i get

exp(\theta) = c* sech^2(\sqrt{2y}*x' + a)

then

exp(\theta) = \frac {2c}{cosh^2 (\sqrt {2y}*x' + a)}

the only problem now are the constants, the book has

exp(\theta) = \frac {a}{cosh^2 ( \sqrt {\frac {ay}{2}}*x' \frac {+}{-} b)}

im confused why they have +/- and why it is sqrt(ay)/2
 
Last edited:
  • #11
exp(\theta) = \frac {2c}{cosh^2 (\sqrt {2y}*x' + a)}

the only problem now are the constants, the book has

exp(\theta) = \frac {a}{cosh^2 ( \sqrt {\frac {ay}{2}}*x' \frac {+}{-} b)}

im confused why they have +/- and why it is sqrt(ay/2)
 
  • #12
Got me, so that looks like something you'll have to puzzle out...
 
  • #13
alrighty

well, thanks again for getting me this close. great help :)
 

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