How Does Green's Identity Prove Solutions in Poisson's Equation?

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In summary: This theorem states that if u and v are two solutions of \bigtriangledown^2 u = p(x) u \ \ x \in \mathcal{R} \ \ \bigtriangledown \cdot n = g(x) \ \x \in \partial \mathcal{R}, then u - v is also a solution of the Poisson equation with zero boundary conditions. From part (i), we know that u ≡ 0 on \mathcal{R}. Therefore, u - v ≡ 0 on \mathcal{R}, which implies that u ≡ v on \mathcal{R}. Thus, u is unique. In summary, to show that u ≡ 0 on \
  • #1
OliviaB
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I think this is Poisson's Equation (and inhomogenous). I think I need to use Green's Identity.

Let [itex] \mathcal{R} [/itex] be a bounded region in [itex]\mathbb{R}^3[/itex], and suppose [itex] p(x) > 0 [/itex] on [itex] \mathcal{R}[/itex].

(i) If [itex]u[/itex] is a solution of

[itex]\bigtriangledown^2 u = p(x) u \ \ x \in \mathcal{R} \ \ \bigtriangledown \cdot n = 0 \ \x \in \partial \mathcal{R}[/itex]

show that [itex]u \equiv 0[/itex] on [itex]\mathcal{R}[/itex]

(ii) If [itex]u[/itex] is a solution of

[itex]\bigtriangledown^2 u = p(x) u \ \ x \in \mathcal{R} \ \ \bigtriangledown \cdot n = g(x) \ \x \in \partial \mathcal{R}[/itex]

show that [itex]u[/itex] is unique (It can be assumed that part (i) is true).

I don't know how to start this...
 
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Solution: (i) To show that u ≡ 0 on \mathcal{R}, we can use Green's Identity. Green's identity states that for any two functions u and v, \int_\mathcal{R} \bigtriangledown u \cdot \bigtriangledown v \, dx = \int_\mathcal{R} u \bigtriangledown^2 v \, dx - \oint_{\partial R} v \bigtriangledown u \cdot n \, ds Letting u = 1 and v = u, we have \int_\mathcal{R} \bigtriangledown u \cdot \bigtriangledown u \, dx = \int_\mathcal{R} u \bigtriangledown^2 u \, dx - \oint_{\partial R} u \bigtriangledown u \cdot n \, ds Substituting in the equation \bigtriangledown^2 u = p(x) u we have \int_\mathcal{R} \bigtriangledown u \cdot \bigtriangledown u \, dx = \int_\mathcal{R} u^2 p(x) \, dx - \oint_{\partial R} u \bigtriangledown u \cdot n \, ds Since \bigtriangledown \cdot n = 0, the second term is zero. As u > 0 on \mathcal{R}, this implies that \int_\mathcal{R} \bigtriangledown u \cdot \bigtriangledown u \, dx = \int_\mathcal{R} u^2 p(x) \, dx However, as \bigtriangledown u = 0, the left hand side is also zero. This implies that \int_\mathcal{R} u^2 p(x) \, dx = 0, which implies that u ≡ 0 on \mathcal{R}.(ii) To show that u is unique, we can use the uniqueness theorem for the Poisson equation.
 

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