Solve this PDE using the characteristic form
$\begin{equation} \frac{\partial w}{\partial t} +x\frac{\partial w}{\partial x}=1 \\ w(x,0)=f(x) \end{equation}$
My attempt Let's go to rewrite the PDE.
$\frac{\partial w}{\partial t} +x\frac{\partial w}{\partial x}-1=0$
For other way We know $w(t)=w(x(t),t)$
Then by chain rule
$\frac{\partial w}{\partial t}=\frac{\partial w}{\partial x}\times \frac{\partial x}{\partial t} + \frac{\partial w}{\partial t}$
This implies
$\begin{equation} \frac{\partial x}{\partial t}=x \\ \frac{\partial w}{\partial t}=0 \end{equation}$
Then:
$x=e^{t+x_0}$
This implies
$w(x,t)=c=w(x_0,0)=f(x_0)=f(ln(x)-t)$
Is correct this?
By the principle of superposition, a single solution to $$ \frac{\partial w}{\partial t} + x \frac{\partial w}{\partial x} = 1$$
Combined with the general solution to
$$ \frac{\partial w}{\partial t} + x \frac{\partial w}{\partial x} = 0 $$ Will form the general solution of:
$$ \frac{\partial w}{\partial t} + x \frac{\partial w}{\partial x} = 1$$
So we now focus our attention to:
$$ \frac{\partial w}{\partial t} + x \frac{\partial w}{\partial x} = 0$$
As you noted correctly for any differentiable function $f$ we have that $f(\ln(x) - t)$ is a $w$ that obeys the above equation.
So what remains is to find a single solution to:
$$ \Omega[w] = \frac{\partial w}{\partial t} + x \frac{\partial w}{\partial x} = 1$$
We can use a power-series approach. Let $w_0 = t$. then $\Omega[w_0] = 1$ [We got lucky with our first guess, but if it weren't so we would continue adding terms to create a series solution] so we have that:
$$w(x,t) = t + f(\ln(x) - t)$$
Is the general solution.
Note:
To support $w(x,0) = h(x)$ as an initial value problem for some $h(x)$ given ahead of time you have that:
$$ f(\ln (x)) = h(x) \rightarrow f(x) = h(e^x) \rightarrow w(x,t) = t+ h(e^{-ln(x)-t}) \rightarrow t + h(xe^{-t}) $$