Can I combine the wave and heat equations? I have this equation 
$$\frac{\partial^2u}{\partial x^2} = 2\frac{\partial u}{\partial t} + \frac{
\partial^2u}{\partial t^2}$$
Is it possible for me to use both the wave and heat equations to solve this equation? I understand both, I just wanted to see if it was possible. 
 A: No, one cannot obtain a solution of this PDE by adding a solution of heat equation to a solution of the wave equation. (With linear PDE, we can combine solutions of the same equation to make new ones; but your situation is different).
Your PDE is known as damped wave equation and is solved here. It does inherit some features from the heat and wave equation. 


*

*oscillation is possible (as in wave equation)

*with homogeneous boundary conditions, solution dissipates to zero (as in heat equation)


It is instructive to generalize to $u_{tt}+cu_t = u_{xx}$ and consider varying $c$. As $c$ increases, the diffusion aspect begins to dominate in that some low-frequency harmonics get overdamped (they don't oscillate at all, simply return to zero). At the same time, higher frequencies are still able to oscillate. 
A: Let $u=e^{-t}v$ ,
Then $\dfrac{\partial u}{\partial t}=e^{-t}\dfrac{\partial v}{\partial t}-e^{-t}v$
$\dfrac{\partial^2u}{\partial t^2}=e^{-t}\dfrac{\partial^2v}{\partial t^2}-e^{-t}\dfrac{\partial v}{\partial t}-e^{-t}\dfrac{\partial v}{\partial t}+e^{-t}v=e^{-t}\dfrac{\partial^2v}{\partial t^2}-2e^{-t}\dfrac{\partial v}{\partial t}+e^{-t}v$
$\dfrac{\partial u}{\partial x}=e^{-t}\dfrac{\partial v}{\partial x}$
$\dfrac{\partial^2u}{\partial x^2}=e^{-t}\dfrac{\partial^2v}{\partial x^2}$
$\therefore e^{-t}\dfrac{\partial^2v}{\partial x^2}=2e^{-t}\dfrac{\partial v}{\partial t}-2e^{-t}v+e^{-t}\dfrac{\partial^2v}{\partial t^2}-2e^{-t}\dfrac{\partial v}{\partial t}+e^{-t}v$
$\dfrac{\partial^2v}{\partial t^2}=v+\dfrac{\partial^2v}{\partial x^2}$
Similar to Solve initial value problem for $u_{tt} - u_{xx} - u = 0$ using characteristics
Consider $v(x,a)=f(x)$ and $v_t(x,a)=g(x)$ ,
Let $v(x,t)=\sum\limits_{n=0}^\infty\dfrac{(t-a)^n}{n!}\dfrac{\partial^nv(x,a)}{\partial t^n}$ ,
Then $v(x,t)=\sum\limits_{n=0}^\infty\dfrac{(t-a)^{2n}}{(2n)!}\dfrac{\partial^{2n}v(x,a)}{\partial t^{2n}}+\sum\limits_{n=0}^\infty\dfrac{(t-a)^{2n+1}}{(2n+1)!}\dfrac{\partial^{2n+1}v(x,a)}{\partial t^{2n+1}}$
$\dfrac{\partial^4v}{\partial t^4}=\dfrac{\partial^2v}{\partial t^2}+\dfrac{\partial^4v}{\partial x^2\partial t^2}=v+\dfrac{\partial^2v}{\partial x^2}+\dfrac{\partial^2v}{\partial x^2}+\dfrac{\partial^4v}{\partial x^4}=v+2\dfrac{\partial^2v}{\partial x^2}+\dfrac{\partial^4v}{\partial x^4}$
Similarly, $\dfrac{\partial^{2n}v}{\partial t^{2n}}=\sum\limits_{k=0}^nC_k^n\dfrac{\partial^{2k}v}{\partial x^{2k}}$
$\dfrac{\partial^3v}{\partial t^3}=\dfrac{\partial v}{\partial t}+\dfrac{\partial^3v}{\partial x^2\partial t}$
$\dfrac{\partial^5v}{\partial t^5}=\dfrac{\partial^3v}{\partial t^3}+\dfrac{\partial^5v}{\partial x^2\partial t^3}=\dfrac{\partial v}{\partial t}+\dfrac{\partial^3v}{\partial x^2\partial t}+\dfrac{\partial^3v}{\partial x^2\partial t}+\dfrac{\partial^5v}{\partial x^4\partial t}=\dfrac{\partial v}{\partial t}+2\dfrac{\partial^3v}{\partial x^2\partial t}+\dfrac{\partial^5v}{\partial x^4\partial t}$
Similarly, $\dfrac{\partial^{2n+1}v}{\partial t^{2n+1}}=\sum\limits_{k=0}^nC_k^n\dfrac{\partial^{2k+1}v}{\partial x^{2k}\partial t}$
$\therefore v(x,t)=\sum\limits_{n=0}^\infty\sum\limits_{k=0}^n\dfrac{C_k^nf^{(2k)}(x)(t-a)^{2n}}{(2n)!}+\sum\limits_{n=0}^\infty\sum\limits_{k=0}^n\dfrac{C_k^ng^{(2k)}(x)(t-a)^{2n+1}}{(2n+1)!}$
Hence $u(x,t)=e^{-t}\sum\limits_{n=0}^\infty\sum\limits_{k=0}^n\dfrac{C_k^nf^{(2k)}(x)(t-a)^{2n}}{(2n)!}+e^{-t}\sum\limits_{n=0}^\infty\sum\limits_{k=0}^n\dfrac{C_k^ng^{(2k)}(x)(t-a)^{2n+1}}{(2n+1)!}$
