For each Borel set $A$ and $x\in\mathbb{R}^n$, denote Dirac measure centered at $x$ as \begin{equation} \delta_x(A)=\begin{cases} 1 & \mbox{ if } x\in A \\ 0 & \mbox{ otherwise}. \end{cases} \end{equation} Alternatively, we can think $\delta_x$ in the sense of distribution defined by \begin{equation} <\delta_x,\phi> = \phi(x). \end{equation} I want to show that for $c\in\mathbb{R}^n$, $u(x,t):=\delta_{x-ct}$ solves the PDE \begin{equation} u_t+c\cdot Du = 0 \mbox{ in } \mathbb{R}^{n+1} \end{equation} in the sense of distribution.
I tried \begin{equation} <u_t, \phi> = <D_t\delta_{x-ct}, \phi> = -<\delta_{x-ct}, D_t\phi>=-\phi(x-ct)(-c) \end{equation} I am not sure about the last equality because when $c$ is a vector, $<u_t,\phi>$ is a vector? Should it be a scalar instead?
What should I do? Thank you.