A few questions about Green's Functions....

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In summary, the modified Green's function is needed when the solvability condition is not satisfied and it is given by a combination of the standard Green's function and the solution of the corresponding homogeneous problem. It is valid for all x_0 \leq z \leq x_1.
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vancouver_water
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Hi, I am having some trouble understanding exactly when a modified green's function is needed. Here is the general problem:

[tex] Lu = (p(x)u'(x))' + q(x)u(x) = f(x), x_0 \leq x \leq x_1, p(x) > 0,\\
\alpha_0 u(0) + \beta_0 u'(0) = 0, \alpha_1 u(1) + \beta_1 u'(1) = 0[/tex]

In my notes it says if the corresponding homogeneous problem with the same boundary conditions has a non-zero solution [itex] u^*(x) [/itex], then we can construct a standard Green's function, with the solvability condition [itex] \int_{x_0}^{x_1} u^*(x)f(x)dx = 0 [/itex]. Then later in my notes it says if [itex] u^*(x) [/itex] is a non-zero solution, we need to use a modified Green's function. Which one is it?

Another question I have is regarding the formula involving the Wronskian, if we have to linearly independent solutions,

[tex] G(x,z) = -\dfrac{u_1(x)u_2(z)}{p(x)W(x)}, x_0 \leq z \leq x,\\
-\dfrac{u_1(z)u_2(x)}{p(x)W(x)}, x \leq z \leq x_1 [/tex]

When exactly is this solution valid?

Thank you.
 
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The modified Green's function is needed if the corresponding homogeneous problem has a non-zero solution u*(x) and the solvability condition \int_{x_0}^{x_1} u^*(x)f(x)dx \neq 0. The modified Green's function is then given by G(x,z) = -\dfrac{u_1(x)u_2(z)}{p(x)W(x)} - \dfrac{u_1(z)u_2(x)}{p(x)W(x)} + \dfrac{u^*(x)u^*(z)}{p(x)W(x)}, where u_1(x) and u_2(x) are two linearly independent solutions of the homogeneous equation and W(x) is the Wronskian of these two functions. This solution is valid for all x_0 \leq z \leq x_1.
 

1. What are Green's functions?

Green's functions are mathematical tools used in physics and engineering to solve differential equations. They are named after the mathematician George Green, who first introduced them in the 1830s. In simple terms, Green's functions are the solutions to a differential equation with a specific type of boundary conditions.

2. How are Green's functions used?

Green's functions are used in various fields such as quantum mechanics, electromagnetism, and fluid dynamics. They allow us to solve complex differential equations by breaking them down into simpler problems. Green's functions are also used in the study of linear systems, which are systems whose output is proportional to the input.

3. What is the relationship between Green's functions and the Dirac delta function?

The Dirac delta function is often used in conjunction with Green's functions. In fact, Green's functions are sometimes referred to as the "Green's function of the Dirac delta." This is because Green's functions are defined as the solution to a differential equation with a Dirac delta function as the input.

4. Can Green's functions be visualized?

Yes, Green's functions can be visualized using graphs and plots. The shape of the Green's function depends on the specific differential equation and boundary conditions it is solving. In some cases, the Green's function may have a simple, symmetrical shape, while in others it may be more complex and irregular.

5. Are there any limitations to using Green's functions?

Green's functions are primarily used for linear systems, so they may not be suitable for solving nonlinear equations. Additionally, they may not always have a closed-form solution, meaning they cannot be expressed in a simple mathematical formula. In these cases, numerical methods may be used to approximate the Green's function.

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