Green's Function fo a Boundary Value Problem

In summary, we can solve the given boundary value problem by using the self-adjoint operator L[y] = \frac{d^2y}{dx^2}, finding the Green's function, and then using it to solve for the solution y(x) for any given source function f(x).
  • #1
maxtor101
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0

Homework Statement



[tex] L[y] = \frac{d^2y}{dx^2} [/tex]

Show that the Green's function for the boundary value problem with [itex] y(-1) = 0 [/itex] and [itex] y(1) = 0 [/itex] is given by

[itex] G(x,y) = \frac{1}{2}(1-x)(1+y) for
-1\leq y \leq x \leq 1\ [/itex]


[itex] G(x,y) = \frac{1}{2}(1+x)(1-y) for
-1\leq x \leq y \leq 1\ [/itex]


Homework Equations





The Attempt at a Solution




Well in class we had defined [itex] L[y] = (py')' + qy [/itex] as the Strum-Liouville self-adjoint operator

So that gives me:

[itex] L[y] = (py')' + qy = \frac{d^2y}{dx^2} [/itex]


Do I treat this problem like other Strum-Liouville Boundary Problems by writting it as :

[itex] L[y] = (py')' + qy = f(x) [/itex]

Where [itex] f(x) = \frac{d^2y}{dx^2} [/itex]

And continue on as I usually would?

Any help on this would be greatly appreciated!
 
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  • #2


it is important to understand and be able to solve boundary value problems in order to study and analyze various physical phenomena. In this case, we are given a boundary value problem with a self-adjoint operator L[y] = \frac{d^2y}{dx^2} and boundary conditions y(-1) = 0 and y(1) = 0. Our goal is to find the Green's function for this problem, which will help us solve for the solution y(x) for any given source function f(x).

To start, we can rewrite the boundary value problem as:

L[y] = \frac{d^2y}{dx^2} = f(x), with boundary conditions y(-1) = 0 and y(1) = 0.

Next, we can use the definition of the Green's function for a self-adjoint operator L[y] to write:

L[G(x,y)] = \delta(x-y), where \delta(x-y) is the Dirac delta function.

Substituting L[y] = \frac{d^2y}{dx^2} and using the boundary conditions, we get:

\frac{d^2G(x,y)}{dx^2} = \delta(x-y), with boundary conditions G(x,y)|_{x=-1} = 0 and G(x,y)|_{x=1} = 0.

Integrating both sides with respect to x, we get:

\frac{dG(x,y)}{dx} = H(x-y) + C_1, where H(x) is the Heaviside step function and C_1 is a constant of integration.

Integrating again and applying the boundary conditions, we get:

G(x,y) = \frac{1}{2}(1-x)(1+y), for -1\leq y \leq x \leq 1 and

G(x,y) = \frac{1}{2}(1+x)(1-y), for -1\leq x \leq y \leq 1.

Thus, the Green's function for the given boundary value problem is given by:

G(x,y) = \frac{1}{2}(1-x)(1+y), for -1\leq y \leq x \leq 1 and

G(x,y) = \
 

1. What is a Green's function for a boundary value problem?

A Green's function for a boundary value problem is a mathematical function that is used to solve differential equations with given boundary conditions. It represents the influence of the boundary conditions on the solution of the differential equation.

2. How is a Green's function used to solve a boundary value problem?

To solve a boundary value problem using a Green's function, the differential equation is first transformed into an integral equation. The Green's function is then used to solve this integral equation, which gives the solution to the original differential equation.

3. What are the properties of a Green's function for a boundary value problem?

A Green's function for a boundary value problem has several important properties, including symmetry, positivity, and the property that it satisfies the boundary conditions of the problem. It also satisfies a certain differential equation, known as the adjoint equation.

4. Can a Green's function be used for any type of boundary value problem?

No, a Green's function is specific to a particular type of boundary value problem. Different types of boundary conditions and differential equations require different Green's functions. It is important to choose the correct Green's function for the specific boundary value problem at hand.

5. Are there any limitations to using a Green's function for solving boundary value problems?

While Green's functions are a powerful tool for solving boundary value problems, they can be limited by the complexity of the problem. In some cases, it may not be possible to find a closed form expression for the Green's function, making it difficult to use in practice. Additionally, Green's functions may not always exist for certain types of boundary value problems.

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