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Determine the Green's function for the boundary value problem y+y=0y'' + y = 0 with...
Jul 2, 2024
Determine the Green's function for the boundary value problem y+y=0y'' + y = 0 with y(0)=0y(0) = 0 and y(pi)=0y(pi) = 0.
Solution by Steps
step 1
To determine the Green's function for the boundary value problem y+y=0y'' + y = 0 with y(0)=0y(0) = 0 and y(π)=0y(\pi) = 0, we first solve the homogeneous equation y+y=0y'' + y = 0
step 2
The general solution to the homogeneous equation y+y=0y'' + y = 0 is y(x)=Asin(x)+Bcos(x)y(x) = A \sin(x) + B \cos(x)
step 3
Apply the boundary conditions to find AA and BB. For y(0)=0y(0) = 0, we have Asin(0)+Bcos(0)=0    B=0A \sin(0) + B \cos(0) = 0 \implies B = 0
step 4
With B=0B = 0, the solution simplifies to y(x)=Asin(x)y(x) = A \sin(x). Apply the second boundary condition y(π)=0y(\pi) = 0: Asin(π)=0    A=0A \sin(\pi) = 0 \implies A = 0
step 5
Since both AA and BB are zero, the homogeneous solution is y(x)=0y(x) = 0. Now, we construct the Green's function G(x,ξ)G(x, \xi) for the inhomogeneous problem
step 6
The Green's function G(x,ξ)G(x, \xi) must satisfy G(x,ξ)+G(x,ξ)=δ(xξ)G''(x, \xi) + G(x, \xi) = \delta(x - \xi) with boundary conditions G(0,ξ)=0G(0, \xi) = 0 and G(π,ξ)=0G(\pi, \xi) = 0
step 7
For xξx \neq \xi, the Green's function satisfies the homogeneous equation G(x,ξ)+G(x,ξ)=0G''(x, \xi) + G(x, \xi) = 0. Thus, G(x,ξ)G(x, \xi) can be written as G(x,ξ)={A(ξ)sin(x)+B(ξ)cos(x)amp;for xlt;ξC(ξ)sin(x)+D(ξ)cos(x)amp;for xgt;ξG(x, \xi) = \begin{cases} A(\xi) \sin(x) + B(\xi) \cos(x) & \text{for } x < \xi \\ C(\xi) \sin(x) + D(\xi) \cos(x) & \text{for } x > \xi \end{cases}
step 8
Apply the boundary conditions: G(0,ξ)=0    B(ξ)=0G(0, \xi) = 0 \implies B(\xi) = 0 and G(π,ξ)=0    C(ξ)sin(π)+D(ξ)cos(π)=0    D(ξ)=0G(\pi, \xi) = 0 \implies C(\xi) \sin(\pi) + D(\xi) \cos(\pi) = 0 \implies D(\xi) = 0
step 9
The Green's function simplifies to G(x,ξ)={A(ξ)sin(x)amp;for xlt;ξC(ξ)sin(x)amp;for xgt;ξG(x, \xi) = \begin{cases} A(\xi) \sin(x) & \text{for } x < \xi \\ C(\xi) \sin(x) & \text{for } x > \xi \end{cases}
step 10
Ensure continuity at x=ξx = \xi: A(ξ)sin(ξ)=C(ξ)sin(ξ)    A(ξ)=C(ξ)A(\xi) \sin(\xi) = C(\xi) \sin(\xi) \implies A(\xi) = C(\xi)
step 11
To satisfy the jump condition at x=ξx = \xi, we integrate the differential equation around ξ\xi: ξϵξ+ϵ(G(x,ξ)+G(x,ξ))dx=ξϵξ+ϵδ(xξ)dx    [G(x,ξ)]ξϵξ+ϵ=1\int_{\xi-\epsilon}^{\xi+\epsilon} (G''(x, \xi) + G(x, \xi)) \, dx = \int_{\xi-\epsilon}^{\xi+\epsilon} \delta(x - \xi) \, dx \implies [G'(x, \xi)]_{\xi-\epsilon}^{\xi+\epsilon} = 1
step 12
This gives G(ξ+,ξ)G(ξ,ξ)=1G'(\xi^+, \xi) - G'(\xi^-, \xi) = 1. For x < \xi, G(x,ξ)=A(ξ)sin(x)G(x, \xi) = A(\xi) \sin(x), so G(x,ξ)=A(ξ)cos(x)G'(x, \xi) = A(\xi) \cos(x). For x > \xi, G(x,ξ)=A(ξ)sin(x)G(x, \xi) = A(\xi) \sin(x), so G(x,ξ)=A(ξ)cos(x)G'(x, \xi) = A(\xi) \cos(x)
step 13
At x=ξx = \xi, G(ξ+,ξ)=A(ξ)cos(ξ)G'(\xi^+, \xi) = A(\xi) \cos(\xi) and G(ξ,ξ)=A(ξ)cos(ξ)G'(\xi^-, \xi) = A(\xi) \cos(\xi). Thus, A(ξ)cos(ξ)A(ξ)cos(ξ)=1    A(ξ)=1cos(ξ)A(\xi) \cos(\xi) - A(\xi) \cos(\xi) = 1 \implies A(\xi) = \frac{1}{\cos(\xi)}
step 14
The Green's function is G(x,ξ)={sin(x)cos(ξ)amp;for xlt;ξsin(x)cos(ξ)amp;for xgt;ξG(x, \xi) = \begin{cases} \frac{\sin(x)}{\cos(\xi)} &amp; \text{for } x &lt; \xi \\ \frac{\sin(x)}{\cos(\xi)} &amp; \text{for } x &gt; \xi \end{cases}
Answer
The Green's function for the boundary value problem y+y=0y'' + y = 0 with y(0)=0y(0) = 0 and y(π)=0y(\pi) = 0 is G(x,ξ)={sin(x)cos(ξ)amp;for xlt;ξsin(x)cos(ξ)amp;for xgt;ξG(x, \xi) = \begin{cases} \frac{\sin(x)}{\cos(\xi)} &amp; \text{for } x &lt; \xi \\ \frac{\sin(x)}{\cos(\xi)} &amp; \text{for } x &gt; \xi \end{cases}.
Key Concept
Green's function for boundary value problems
Explanation
The Green's function is a fundamental solution used to solve inhomogeneous differential equations subject to boundary conditions. It represents the response of the system at a point xx due to a unit impulse applied at another point ξ\xi.
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