How to integrate \frac{(1+\Phi)+\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}?

In summary: So\int \frac{(1+\Phi)+\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}dx=2ln[\frac{(1+\Phi)-\Phi e^{-x}}{\Phi e^{-x}}]Is it right?I am not sure, but it looks correct to me. Great job!
  • #1
Petar Mali
290
0
I have a problem with this equation

[tex]\frac{d^2\Omega(\alpha)}{d\alpha^2}+\frac{(1+\Phi)+\Phi e^{-\alpha}}{(1+\Phi)-\Phi e^{-\alpha}}\frac{d\Omega(\alpha)}{d\alpha}-S(S+1)\Omega(\alpha)=0[/tex]

Boundary conditions are

[tex]\Omega(0)=1[/tex]

[tex][\Pi^S_{p=-S}(p-\frac{d}{d\alpha})]\Omega(\alpha)|_{\alpha=0}=0[/tex]

How to to transform part before first derivative [tex]\frac{(1+\Phi)+\Phi e^{-\alpha}}{(1+\Phi)-\Phi e^{-\alpha}}[/tex]?
 
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  • #2
[tex]\Phi[/tex] and [tex]S[/tex] are constants! Thanks for your answer!
 
  • #3
The general solution to the equation (maple obtained) is

[tex]\Omega(x)= \frac{e^{-x/2}}{-\Phi-1+\Phi e^{-x}}(C_{1}e^{x(S+1/2)}+C_{2}e^{-x(S+1/2)})[/tex]

The first boundary condition puts the constraint

[tex]C_{1}+C_{2}=-1[/tex]

while the second one says

[tex]\Pi_{p=-S}^{p=S} [p-[(1+2S)C_{2}+S-\Phi]] =0[/tex]

which is a product with a finite number of terms. I assume S is an integer or half integer A solution is obtained by cancelling any factor of the product. You get a solution for any C2 satisfying

[tex](1+2S)C_{2}+S-\Phi=p, -S\le p \le S [/tex]

All this needs some checking
 
Last edited:
  • #4
Ok! But how to get solution without use of any computer programme? How to solve this with pencil and paper? What is the idea?
 
  • #5
Well, first thing I thought was eliminating the term in the first derivative by a standart trick. If

[tex] u''(x)+A(x)u'(x)-S(S+1)u(x)=0[/tex]then it turns out that [tex]u(x)=exp(-\frac{1}{2}\int{A(x')dx'})v(x)[/tex] transforms the equation into

[tex] v''+[-S(S+1)-A^2/4-A'/2]v=0[/tex]

In this case, we have

[tex] \int{A(x)dx}=-2ln[\frac{exp(-x/2)}{-1-\Phi+\Phi exp(-x)}][/tex]

And the resulting equation for v(x) is

[tex]v''(x)-(S+1/2)^{2}v(x)=0[/tex]

resulting in the solution above. This equation has several lucky "coincidences", but the procedure to eliminate the first derivative term is standard, and very useful for non-homogeneous oscilators
 
  • #6
gato_ said:
Well, first thing I thought was eliminating the term in the first derivative by a standart trick. If

[tex] u''(x)+A(x)u'(x)-S(S+1)u(x)=0[/tex]


then it turns out that [tex]u(x)=exp(-\frac{1}{2}\int{A(x')dx'})v(x)[/tex] transforms the equation into

[tex] v''+[-S(S+1)-A^2/4-A'/2]v=0[/tex]

Are you sure about this?

I get equation

[tex]v''+[-S(S+1)+\frac{A^2}{4}-\frac{A}{2}-\frac{A'}{2}]v=0[/tex]
 
  • #7
gato_ said:
Well, first thing I thought was eliminating the term in the first derivative by a standart trick. If

[tex] u''(x)+A(x)u'(x)-S(S+1)u(x)=0[/tex]


then it turns out that [tex]u(x)=exp(-\frac{1}{2}\int{A(x')dx'})v(x)[/tex] transforms the equation into

[tex] v''+[-S(S+1)-A^2/4-A'/2]v=0[/tex]

In this case, we have

[tex] \int{A(x)dx}=-2ln[\frac{exp(-x/2)}{-1-\Phi+\Phi exp(-x)}][/tex]

And the resulting equation for v(x) is

[tex]v''(x)-(S+1/2)^{2}v(x)=0[/tex]

resulting in the solution above. This equation has several lucky "coincidences", but the procedure to eliminate the first derivative term is standard, and very useful for non-homogeneous oscilators

How you get this form [tex]v''(x)-(S+1/2)^{2}v(x)=0[/tex] from [tex] v''+[-S(S+1)-A^2/4-A'/2]v=0[/tex]?
 
  • #8
By substituting A
 
  • #9
[tex]A(x)=\frac{(1+\Phi)+\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}[/tex]

[tex]A'(x)=[\frac{(1+\Phi)+\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}]'[/tex]

[tex]A'(x)=\frac{-\Phi e^{-x}[(1+\Phi)-\Phi e^{-x}]-[(1+\Phi)+\Phi e^{-x}]\Phi e^{-x}}{[(1+\Phi)-\Phi e^{-x}]^2}=\frac{-2\Phi e^{-x}(1+\Phi)}{[(1+\Phi)-\Phi e^{-x}]^2}[/tex]

[tex]\frac{-A'(x)}{2}=\frac{\Phi e^{-x}(1+\Phi)}{[(1+\Phi)-\Phi e^{-x}]^2}[/tex]

[tex]\frac{-A^2}{4}=-\frac{\frac{(1+\Phi)^2}{4}+\frac{1}{2}(1+\Phi)\Phi e^{-x}+\frac{1}{4}\Phi^2 e^{-2x}}{[(1+\Phi)-\Phi e^{-x}]^2}[/tex]

[tex]\frac{-A^2}{4}-\frac{A'(x)}{2}=-\frac{\frac{(1+\Phi)^2}{4}-\frac{1}{2}(1+\Phi)\Phi e^{-x}+\frac{1}{4}\Phi^2 e^{-2x}}{[(1+\Phi)-\Phi e^{-x}]^2}=-\frac{1}{4}[/tex]

[tex]\upsilon''(x)-(S+\frac{1}{2})^2\upsilon(x)=0[/tex]


Thanks!
 
  • #10
You are welcome
 
  • #11
gato_ said:
In this case, we have

[tex] \int{A(x)dx}=-2ln[\frac{exp(-x/2)}{-1-\Phi+\Phi exp(-x)}][/tex]

I got

[tex]\int \frac{(1+\Phi)+\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}dx=2ln[\frac{(1+\Phi)-\Phi e^{-x}}{\Phi e^{-x}}][/tex]


I have done this integral like

[tex]\int \frac{(1+\Phi)+\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}dx=\int\frac{1+\Phi}{(1+\Phi)-\Phi e^{-x}}dx+\int\frac{\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}dx[/tex]

and got

[tex]\int\frac{1+\Phi}{(1+\Phi)-\Phi e^{-x}}dx=ln[\frac{(1+\Phi)-\Phi e^{-x}}{\Phi e^{-x}}][/tex]

and

[tex]\int\frac{\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}dx=ln[{(1+\Phi)-\Phi e^{-x}}][/tex]
 

FAQ: How to integrate \frac{(1+\Phi)+\Phi e^{-x}}{(1+\Phi)-\Phi e^{-x}}?

What is a differential equation?

A differential equation is a mathematical equation that describes the relationship between a function and its derivatives. It involves both the function and its derivatives, and it is used to model various physical phenomena in science and engineering.

What is the difference between an ordinary and a partial differential equation?

An ordinary differential equation involves only one independent variable, while a partial differential equation involves multiple independent variables. Ordinary differential equations are often used to model systems that change over time, while partial differential equations are used to model systems that vary in space and time.

What are the applications of differential equations?

Differential equations have numerous applications in science and engineering, including modeling population growth, predicting weather patterns, and analyzing electrical circuits. They are also used in economics, biology, and other fields to study complex systems.

What are some common methods for solving differential equations?

Some common methods for solving differential equations include separation of variables, integrating factors, and power series solutions. Other methods include using Laplace transforms, numerical methods, and computer simulations.

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Differential equations are important in science because they allow us to mathematically describe and understand the behavior of complex systems. They provide a powerful tool for prediction and analysis, and they are used in a wide range of fields to solve real-world problems.

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