How would one go about calculating the fourier transform of the signal? $$ y(t) = x(t-t_0)cos(\omega_0t) $$
2026-03-27 16:00:49.1774627249
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Fourier Transform of a modulated time shifted function
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In summary, you would:
- Apply the Fourier Transform convolution theorem $$\mathcal{F}\left\{x(t-t_0)\cos(\omega_0 t)\right\} = \dfrac{1}{2\pi}\left[\mathcal{F}\left\{x(t-t_0)\right\}*\mathcal{F}\left\{\cos(\omega_0 t)\right\}\right]$$
- Apply the Fourier Transform shift/modulation theorem for $x(t-t_0)$ $$\mathcal{F}\left\{x(t-t_0)\right\} = e^{-it_0 \omega}\mathcal{F}\left\{x(t)\right\}= e^{-it_0 \omega}X(\omega)$$
- Look up the Fourier Transform of $\cos(\omega_0 t)$ in a table $$\mathcal{F}\left\{\cos(\omega_0 t)\right\} = \pi\left[\delta(\omega-\omega_0) + \delta(\omega+\omega_0)\right] $$
- Apply the convolution properties of the Dirac Delta function $$ \dfrac{1}{2\pi} e^{-it_0 \omega}X(\omega) * \pi\left[\delta(\omega-\omega_0) + \delta(\omega+\omega_0)\right] = \dfrac{1}{2}e^{-it_0 (\omega-\omega_0)}X(\omega-\omega_0)+\dfrac{1}{2}e^{-it_0 (\omega+\omega_0)}X(\omega+\omega_0) $$
You end up with a Fourier transform that is the sum of two shifted, scaled, and modulated copies of $\mathcal{F}\{x(t)\}$
I'm not sure if this is the solution, but I'll try to help with that:
$$\int x(t+t_0)cos(w_0t)e^{-i\omega t}dt$$
re express it as follows
$$\tau=t+t_0$$
$$\int x(\tau)cos(w_0(\tau-t_0))e^{-i\omega (\tau+t_0)}d\tau$$
$$e^{-i\omega t_0}\int x(\tau)cos(w_0(\tau-t_0))e^{-i\omega (\tau)}d\tau$$
operating inside the $cos$ you get
$$e^{-i\omega t_0}\int x(\tau)cos(w_0\tau- w_0t_0)e^{-i\omega (\tau)}d\tau$$
where $w0t0$ is a number representing a phase.
Once there you should figure out hot to integrate it in order to obtain the final result.