Assume that $f$ is infinitely differentiable. Let $\delta$ be the (Dirac) delta functional.
I know that $f\delta = f(0)\delta$, but I'm not sure how to derive the equation $f\delta′=f(0)\delta′−f′(0)\delta$.
Assume that $f$ is infinitely differentiable. Let $\delta$ be the (Dirac) delta functional.
I know that $f\delta = f(0)\delta$, but I'm not sure how to derive the equation $f\delta′=f(0)\delta′−f′(0)\delta$.
On
You're missing an $f$ in the left hand side.
Compute $(f\delta)'$ in two different ways.
On one hand $(f\delta)' = f'\delta + f\delta' = f'(0)\delta + f\delta'$.
On the other hand $(f\delta)' = (f(0)\delta)' = f(0)\delta'$.
Hence $f\delta' = f(0)\delta' - f'(0)\delta$.
On
(I suppose that with $\delta$ you mean the Dirac function.) Just evaluate $(f(t)\delta(t))'$ in two ways.
First, use Leibniz' rule: $$ (f(t)\delta(t))'=f(t)\delta'(t)+f'(t)\delta(t)=f(t)\delta'(t)+f'(0)\delta(t). $$ We also have $$ (f(t)\delta(t))'=(f(0)\delta(t))'=f(0)\delta'(t). $$
Since the two expressions must be equal, we have $$ f(t)\delta'(t)=f(0)\delta'(t)-f'(0)\delta(t). $$
I'm assuming you mean the delta function(al) $\delta(x)$.
If so, you should use formal integration by parts. $$\int g\times (f\delta') =\int -(fg)'\delta = \int -(f'(0)g(x)+g'(x)f(0))\delta = -f'(0) \int g\delta-f(0)\int g'\delta$$
Integrating the last term by parts and stripping off the $\int g\times$ gives the result.