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The solution of the linear partial differential equation

\[ \begin{aligned} &\frac{\partial^{2} z}{\partial x^{2}} - 2\frac{\partial^{2} z}{\partial y \partial x} \\ &+ \frac{\partial^{2} z}{\partial y^{2}} = 0 \end{aligned} \]

is :

  • A.\(z = \phi_{1}(x + y) + \phi_{2}(x - y)\)
  • B.\(z = \phi_{1}(x + y) + x\phi_{2}(x - y)\)
  • C.\(z = \phi_{1}(x + y) + x\phi_{2}(x + y)\)
  • D.\(z = \phi_{1}(x + y) + x^{2}\phi_{2}(x + y)\)

Answer: C

The solution is \(z = \phi_{1}(x + y) + x\phi_{2}(x + y)\).

With \(D = \partial/\partial x\) and \(D' = \partial/\partial y\), the equation is \((D^{2} - 2DD' + D'^{2})z = (D - D')^{2}z = 0\). For \((D - mD')^{2}z = 0\) the general solution is \(\phi_{1}(y + mx) + x\phi_{2}(y + mx)\); here \(m = 1\), so the argument is \(x + y\) in both terms.

Check: if \(z = \phi(x + y)\), then \(z_{xx} = z_{xy} = z_{yy} = \phi''\) and \(\phi'' - 2\phi'' + \phi'' = 0\).

Option A has \(x - y\), which belongs to \(D + D'\), a different factor. Option B mixes the two arguments, and option D's \(x^{2}\) would arise only from a cubed factor.

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