So I have to get the Fourier Transform of $\sin(2 \pi f_0 t)$ using differentiation and $$\mathcal{F} \{ \cos(2 \pi f_0 t\} = \frac{1}{2} (\delta (f+f_0) + \delta(f-f_0)) $$
Differentiation gives me $$\frac{d}{dt} \cos(2 \pi f_0 t\ ) = (-2\pi f_0) \sin(2 \pi f_0 t) $$
My "Solution" gives me this:
$$(j2\pi f) \mathcal{F}\{ \cos(2 \pi f_0 t\ ) \} = (-2\pi f_0) \mathcal{F} \{\sin(2 \pi f_0 t)\}$$
I do not understand what is happening here. I know that the Diff g'(x) of a Function g(x) when it is Fourier transformed gives me this: $\mathcal{F}\{g^{(n)}(t) \} = (j2\pi f)^n \cdot \hat g(f)$
But here both sides have have their Fourier transform taken. How does this work ?
You have an identity: $$\frac{d}{dt} \cos(2 \pi f_0 t\ ) = (-2\pi f_0) \sin(2 \pi f_0 t)$$
Then you take the Fourier transform of both sides to get another identity: $$\mathcal{F}\{\frac{d}{dt} \cos(2 \pi f_0 t\ )\} = \mathcal{F}\{(-2\pi f_0) \sin(2 \pi f_0 t)\}$$
Then you use a Fourier transform identity to rewrite the derivative in the left hand side: $$j 2\pi f \, \mathcal{F}\{ \cos(2 \pi f_0 t\ )\} = \mathcal{F}\{(-2\pi f_0) \sin(2 \pi f_0 t)\}$$