Final answer:
To compute either R(ω) or I(ω), you can use the given formula: I(ω) = - 1/π ∫[infinity] to −∞(R(ω'))/(ω - ω') dω'. Start by substituting X(ω) = R(ω) + jI(ω) into the Fourier transform definition. Split the integral into real and imaginary parts, equating R(ω) to the real part and I(ω) to the imaginary part of X(ω).
Step-by-step explanation:
To show that given either R(ω) or I(ω), we can compute the other using the given formulas:
I(ω) = - 1/π ∫[infinity] to −∞(R(ω'))/(ω - ω') dω'.
We can start by substituting X(ω) = R(ω) + jI(ω) into the definition of the Fourier transform:
X(ω) = ∫[infinity] to −∞ x(t)e-jωt dt
Split the integral into two parts:
X(ω) = ∫[infinity] to −∞ R(ω)e-jωt dt + j∫[infinity] to −∞ I(ω)e-jωt dt
Equating the real and imaginary parts:
R(ω) = Re[X(ω)] = 1/π ∫[infinity] to −∞ R(ω')/(ω - ω') dω'
I(ω) = Im[X(ω)] = -1/π ∫[infinity] to −∞ R(ω')/(ω - ω') dω'