Solution of a PDE Solve $\displaystyle \frac{\partial^2 z}{\partial x^2}+z=0$, given that when $x=0$, $z=e^y$ and $\displaystyle \frac{\partial z}{\partial x}=1$.
My Attempt: Integrating w.r.t x twice (keeping y constant)
$\displaystyle \frac{\partial z}{\partial x}+xz=f(y)$
$\displaystyle z+\frac{x^2}{2}z=xf(y)+g(y)$
The problem has a hint given : start with $\displaystyle z=f(y)\sin x+g(y)\cos x$. Uisng this obviously helps.
But if I go the standard way, I get stuck.. Am I missing something here or do I just memorise this hint and hope for the best.
 A: Notice that you cannot integrate the way you did since $z$ is the dependent variable of your problem and therefore cannot be treated as a simple constant, just like you did in the $xz$ term.
You may want to try solutions of the form (since the PDE does not depend on $y$):
$$z(x,y) = C e^{qx},$$ which after substituting back into the PDE yields:
$$q^2 + 1 = 0, $$ and therefore we have $q = \pm i$, so the set of solutions is hence described by:
$$z(x,y) = C_1(y) \sin{x} + C_2(y) \cos{x},$$ where $C_{1,2}$ are arbitrary functions of $y$, which remains to be fixed by some boundary conditions. I'm sure you can now solve for $C_1$ and $C_2$ with the given information.
Hope this helps.
Edit: notice that I just treated $y$ as a constant, because the PDE is independent from $y$, and can be solved like a classical ODE with constant coefficients. I said nothing regarding $C$, but it naturally becomes $y$-dependent through the boundary conditions. Also notice that this is not the general approach to solve PDEs but it's heavily faster in this cases. 
Cheers!
A: If you know how to solve higher order linear ODE, then you can just note that the PDE you have contains only derivatives with respect to $x$, so it is essentially a linear homogeneous ODE, with auxiliary equation $m^2 + 1 = 0 \Rightarrow m = \pm i$, for which the solution is $c_1\cos(x) + c_2\sin(x)$. As we actually have a PDE (with the only other independent variable being $y$), $c_1$ and $c_2$ should be functions of $y$ rather than pure constants.
If you want a "from scratch" solution, here goes...
Let $\partial_x = \dfrac{\partial}{\partial x}$. Then the given PDE is $\partial_x^2z + z = 0$, or $(\partial_x^2 + 1)z = 0$. This can be written as $(\partial_x + i)(\partial_x - i)z = 0$ (the validity of this factorization of the operator can be verified by actually carrying out the differentiations and verifying that this becomes the original equation - you will see that it is only a convenient notation). Thus we have to solve
$$(\partial_x + i)(\partial_x - i)z = 0$$
Let $(\partial_x - i)z = w$. Then the equation becomes
$(\partial_x + i)w = 0\Rightarrow\\
\partial_x w = -iw \Rightarrow\\
\dfrac{1}{w} \partial_xw = -i \Rightarrow\\
\partial_x (\log w) = -i \Rightarrow\\
\log w = -ix + C(y) \Rightarrow\\
w = c_1(y) e^{-ix} \qquad (\text{where we have written $e^{C(y)}$ as $c_1(y)$})
$
Now, as $(\partial_x - i)z = w$, we have
$
\partial_x z - iz = c_1(y)e^{-ix} = c_1 e^{-ix} \Rightarrow\\
\dfrac{\partial z}{\partial x} - iz = c_1 e^{-ix}
$
This is a first order linear equation that can be solved using the integrating factor $e^{\int (-i)\, dx} = e^{-ix}$. Therefore:
$z\times \text{IF} = \displaystyle \int \text{RHS}\times \text{IF} \,dx \Rightarrow\\
z e^{-ix} = \displaystyle \int c_1 e^{-2ix} \,dx \Rightarrow\\
z e^{-ix} = c_1 \dfrac{e^{-2ix}}{-2i} + c_2 a = C_1 e^{-2ix} + C_2 \Rightarrow\\
z = C_1 e^{-ix} + C_2 e^{ix} \Rightarrow\\
z = C_1(\cos x - i \sin x) + C_2(\cos x + i \sin x) \Rightarrow\\
z = (C_1 + C_2) \cos x - i(C_1 - C_2) \sin x \Rightarrow\\
z = A \cos x + B \sin x
$
Now as the equation is actually a PDE, $A$ and $B$ are functions of $y$, say $A = f(y)$ and $B = g(y)$. Thus
$$\boxed{z = f(y)\cos x + g(y) \sin x}$$
