sam.green
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Hello,
I am working through Signals and Systems Demystified, but I am at an impasse.
I would like to take the inverse Fourier transform of
[tex] H(f)=\begin{cases}<br /> -j&\text{if } f > 0\\<br /> j&\text{if } f<0\end{cases}[/tex]
So
[tex] h(t) = \int_{-\infty}^{0} je^{j2\pi f t}df + \int_{0}^{\infty} -je^{j2\pi ft}df <br /> = \int_{-\infty}^{0} je^{j2\pi f t}df + \int_{-\infty}^{0} je^{j2\pi f t}df <br /> = 2\int_{-\infty}^{0} je^{j2\pi f t}df <br /> = \frac{j2e^{j2\pi ft}}{j2\pi t}|_{-\infty}^{0}[/tex]
So
[tex] h(t) = \frac{1}{\pi t} - \lim_{f \rightarrow -\infty} \frac{e^{j2\pi ft}}{\pi t}[/tex]
The book says that [tex]h(t) = \frac{1}{\pi t}[/tex] is the answer, but I don't understand how. Isn't [tex]\lim_{f \rightarrow -\infty} \frac{e^{j2\pi ft}}{\pi t}[/tex] periodic and nonconverging?
I am working through Signals and Systems Demystified, but I am at an impasse.
I would like to take the inverse Fourier transform of
[tex] H(f)=\begin{cases}<br /> -j&\text{if } f > 0\\<br /> j&\text{if } f<0\end{cases}[/tex]
So
[tex] h(t) = \int_{-\infty}^{0} je^{j2\pi f t}df + \int_{0}^{\infty} -je^{j2\pi ft}df <br /> = \int_{-\infty}^{0} je^{j2\pi f t}df + \int_{-\infty}^{0} je^{j2\pi f t}df <br /> = 2\int_{-\infty}^{0} je^{j2\pi f t}df <br /> = \frac{j2e^{j2\pi ft}}{j2\pi t}|_{-\infty}^{0}[/tex]
So
[tex] h(t) = \frac{1}{\pi t} - \lim_{f \rightarrow -\infty} \frac{e^{j2\pi ft}}{\pi t}[/tex]
The book says that [tex]h(t) = \frac{1}{\pi t}[/tex] is the answer, but I don't understand how. Isn't [tex]\lim_{f \rightarrow -\infty} \frac{e^{j2\pi ft}}{\pi t}[/tex] periodic and nonconverging?