00:01
So, here we have x t is equals to cos 2 t plus cos 3 t.
00:12
Now, cos omega naught t can be written as e to the power minus i omega naught e to the power e to the power minus i omega naught t to the power plus i omega naught t plus e to the power minus i omega naught t divided by 2.
00:42
Now, fourier transform of e to the power i omega naught t can be fourier transform of i e to the power i omega naught t is basically equals to 2 pi del of omega minus omega naught.
01:07
Now, fourier transform of e to the power i any value z t would be 2 pi del of w omega omega minus z.
01:26
Then fourier transform of e to the power minus i z t would be 2 pi del of omega plus z.
01:44
That would be a first bracket there.
01:49
So, from this if we just replace the z with our given values that is 2 and 3 we would have fourier transform of e to the power minus i 2 t, i 2 t equals to 2 pi del omega plus 2 and fourier transform of e to the power plus i 2 t would be 2 pi del omega minus 2.
02:28
Similarly, fourier transform of e to the power i 3 t would be equals to 2 pi del of omega minus 3, sorry omega plus 3 and fourier transform of fourier transform of e to the power minus i 3 t would be equals to 2 pi del of omega, omega, omega plus 3 and before one would be omega minus 3.
03:06
That is going to be omega minus 3...