Machine-translated by Google. Questions are authored in English.
Top

Discussion

Let \(u_{1}\) and \(u_{2}\) be solutions of the equation :

\(\Delta u = 0\) in D
\(\dfrac{\partial u}{\partial n} = g(s)\) on \(\partial D\)

where \(D = \{(x, y) \in \mathbf{R}^{2} / \frac{x^{2}}{4} + \frac{y^{2}}{9} \le 1\}\) is an ellipse with boundary \(\partial D = \{(x, y) \in \mathbf{R}^{2} /\) \(\frac{x^{2}}{4} + \frac{y^{2}}{9} = 1\}\). If \(u_{1}(0, \frac{1}{2}) - u_{2}(0, \frac{1}{2}) = 1\). Then :

  • A.\(u_{1}\) and \(u_{2}\) are dependent solutions
  • B.\(u_{1} \equiv u_{2} + 1\) in D
  • C.\(u_{1} - u_{2}\) changes sign in D
  • D.\(u_{1} \equiv u_{2}\) in D

Answer: B

The answer is \(u_{1} \equiv u_{2} + 1\) in D.

Let \(w = u_{1} - u_{2}\). Then \(\Delta w = 0\) in D and \(\partial w / \partial n = 0\) on the boundary. Green's identity gives

\[ \begin{aligned} \int_{D} |\nabla w|^{2} &= \int_{\partial D} w \frac{\partial w}{\partial n} - \int_{D} w\, \Delta w \\ &= 0 \end{aligned} \]

so \(\nabla w = 0\) and \(w\) is constant: solutions of the Neumann problem are unique up to an additive constant. The given value \(w(0, \frac{1}{2}) = 1\) fixes the constant as 1.

So \(u_{1} - u_{2}\) does not change sign (C), the two are not identical (D), and they are not 'dependent' in any multiplicative sense (A).

No comment is present. Be the first to comment.
Loading…

Post your comment

Please log in or register to post a comment.