Finding eigenvalue and eigenfunctions with exponential solutions

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sigmund
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I have this eigenvalue problem:
[itex]\frac{\mbox{d}^2y}{\mbox{d}x^2}+\left(1-\lambda\right)\frac{\mbox{d}y}{\mbox{d}x}-\lambda y = 0 \ , \ x\in[0,1], \ \lambda\in\mathbb{R} [/itex]
[itex]y(0)=0[/itex]
[itex]\frac{\mbox{d}y}{\mbox{d}x}(1)=0[/itex]
Then, I have to show that there exists only one eigenvalue [itex]\lambda[/itex], and find this eigenvalue and write the corresponding eigenfunctions.

Thus far, I have solved the ODE's characteristic equation
[itex]r^2+(1-\lambda)r-\lambda=0[/itex].
This gives me two solutions
[itex]r=-1[/itex] and [itex]r=\lambda[/itex].
Thus the solution to the ODE is
[itex] y=c_1\exp(-x)+c_2\exp(\lambda x) \ , \ x\in\mathbb{R} \ , \ c_1, \ c_2\in\mathbb{R} [/itex].

Can I now conclude that because we only have real solutions to the characteristic equation, only one eigenvalue exists?

Secondly, I am not completely sure how to find the sought eigenvalue. I know how to find the eigenvalue when I have a solution that involves [itex]\sin[/itex] and [itex]\cos[/itex], but here I am not sure how to do it. Could anyone give me a hint?

Thirdly, when I have the eigenvalue there should not be any problems in writing the corresponding eigenfunctions, or is it?

I would appreciate any help. I am not looking for a solution to my homework problem, but any hints to the problem mentioned above are welcome.
 
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You miss text from the problem.In order for that to be a genuine Cauchy problem,you need to specify 2 initial conditions.Besides,you didn't use the one which u have posted...:wink:

Daniel.
 
An "eigenvalue" is a value of &lamba; such that the problem has a non-trivial solution. Have you determined what functions satisfy your other conditions?
(You have y(0)= 0 but then is see only [itex]\frac{dy}{dx}[/itex]. Did you mean [itex]\frac{dy}{dx}(0)= 0[/itex] or [itex]\frac{dy}{dx}(1)= 0[/itex]?)

The problem is a lot easier if it is [itex]\frac{dy}{dx}(0)= 0[/itex]!

Put x= 0 into the formulas for y and dy/dx and you get two equations to solve for c1 and c2. For what values of &lamda; can you NOT solve for specific value of c1 and c2?
 
Has anyone tried to calculate the eigenvalue? My suggestion is [itex]\lambda=-1[/itex]. Can anyone either confirm or refute this?
 
When I use the initial conditions, I get this system of equations:

[tex]c_1+c_2=0[/tex]
[tex]-c_1\exp(-1)+c_2\lambda\exp(\lambda)=0[/tex]

I then guess that [itex]\lambda=-1[/itex], and find out that with this eigenvalue you cannot solve the system for any particular value of [itex]c_1[/itex] and [itex]c_2[/itex].
 
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Yes,indeed,lambda=-1 makes the 2 equations identical.

Now find the eigenfunctions corresponding to [itex]\lambda=-1[/itex]

Daniel.
 
Deleted- DexterCioby beat me to it!
 
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Well, the eigenfunctions corresponding to [itex]\lambda=-1[/itex] must then be

[tex]y=c_1\exp(-x)+c_2\exp(-x)=(c_1+c_2)\exp(-x)=c\exp(-x),~~c_1,\,c_2,\,c\in\mathbb{R}[/tex]
 
After I have talked to the teacher, I have realized that the eigenfunction written in post #11 is wrong. The reason is that when [itex]\lambda=-1[/itex], the characteristic equation has a double root [itex]r=-1[/itex]. Thus, the solution is [itex]y=c_1\exp(-x)+c_2x\exp(-x)[/itex], and NOT [itex]y=c\exp(-x)[/itex] as written earlier. Do you agree dextercioby?
 
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sigmund said:
After I have talked to the teacher, I have realized that the eigenfunction written in post #11 is wrong. The reason is that when [itex]\lambda=-1[/itex], the characteristic equation has a double root [itex]r=-1[/itex]. Thus, the solution is [itex]y=c_1\exp(-x)+c_2x\exp(-x)[/itex], and NOT [itex]y=c\exp(-x)[/itex] as written earlier. Do you agree dextercioby?

I'm confused: To meet the initial condition y(0)=0, [itex]c_1[/itex] has to be zero. But if that's the case, then any value of [itex]c_2[/itex] meets the derivative at the boundary condition specified above and thus we loose uniqueness.
 
Yes, that's the whole point of "eigenvalue". If λ is not an eigenvalue, then the equation Ax= &lamda;x has a unique solution: x= 0. If λ is an eigenvalue, then there exist an infinite number of solutions: the set of eigenvectors corresponding to a given eigenvalue is is a subspace of the original vectdor space.