Exercise 1.4Z: Everything Rectangular
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We consider the periodic rectangular signal $x(t)$ , whose periodic duration is $T_0 = 2T$ , according to the sketch above.
- This signal has spectral components at the fundamental frequency $f_0 = 1/T_0 = 1/(2T)$ and at all odd multiples thereof, that is, at $3f_0$, $5f_0,$ and so on. In addition, there is a direct component.
- For this purpose, we consider two filters $\rm A$ and $\rm B$ each with rectangular impulse response $h_{\rm A}(t)$ with duration $6T$ and $h_{\rm B}(t)$ with duration $5T$, respectively.
- The heights of the two impulse responses are such that the areas of the rectangles each add up to $1$ .
Please note:
- The exercise belongs to the chapter System Description in Time Domain.
- For information on convolution, see the chapter convolution theorem and operation in the book "Signal Representation”.
- We also refer you to the interactive applet Zur Verdeutlichung der graphischen Faltung.
Questions
Solution
(1) The output signal is the result of the convolution operation between $x(t)$ and $h_{\rm A}(t)$:
- $$y_{\rm A}(t) = x (t) * h_{\rm A} (t) = \int_{ - \infty }^{ + \infty } {x ( \tau )} \cdot h_{\rm A} ( {t - \tau } ) \hspace{0.1cm}{\rm d}\tau.$$
- Because of the rectangular function and the duration $6T$ this can also be written as follows:
- $$y_{\rm A}(t) = \frac{1}{6T}\cdot \int_{t-6T}^{t}x(\tau)\hspace{0.15cm} {\rm d}\tau.$$
- It can be seen that this equation gives the same result $y_{\rm A}(t) \rm \underline{\: = 1V}$ for all $t$ .
(2) The magnitude of the frequency response is $|H_{\rm A}(f)| = |{\rm si}(\pi \cdot f \cdot 6T)|.$ This has zeros at an interval of $1/(6T)$ .
- So, there are also zeros at $f_0$, $3f_0$, $5f_0$ etc., respectively.
- In particular, $|H_{\rm A}(f = f_0)| \underline{\: = 0}$ holds, too.
- From the spectrum $X(f)$ only the direct component $1 \hspace{0.05cm} \rm V$ remains unchanged.
- In contrast to this, all other spectral lines in $Y_{\rm A}(f)$ are no longer included.
(3) Analogous to the subtask (1) for the output signal the following can be recorded:
- $$y_{\rm B}(t) = \frac{1}{5T}\cdot \int_{t-5T}^{t}x(\tau)\hspace{0.15cm} {\rm d}\tau.$$
- This results in a triangular shape fluctuating around the mean $1 \ \rm V$ ⇒ see bottom graph.
- Since two rectangles and three gaps each are covered by the integration interval, the following holds for $t = 0, t = 2T,$ etc.:
- $$y_{\rm B}(t) = \frac{2\,{\rm V} \cdot 2T }{5T} \hspace{0.15cm}\underline{= 0.8\,{\rm V} =y_{\rm B}(t=0) }.$$
- For $t = T,\ 3T, \ 5T, $ etc., there are three rectangles and two gaps each to be considered: One obtains:
- $$y_{\rm B}(t) \underline{\: = 1.2 \: {\rm V}=y_{\rm B}(t=T)}.$$
(4) The magnitude function is generally or at frequencies $f = f_0 = 1/(2T)$ and $f = 3f_0$:
- $$\begin{align*} |H_{\rm B}(f)| & = |{\rm si}(\pi \cdot f \cdot 5T)|, \\ |H_{\rm B}(f = f_0)| & = |{\rm si}(\pi \frac{5T}{2T})| = |{\rm si}(2.5\pi )| = \frac{1}{2.5 \pi} \hspace{0.15cm}\underline{= 0.127}, \\ |H_{\rm B}(f = 3f_0)| & = |{\rm si}(7.5\pi )| = \frac{1}{7.5 \pi} \hspace{0.15cm}\underline{=0.042}.\end{align*}$$
Interpretation:
- The spectral components of the rectangular signal at $f_0, 3f_0,$ etc., although now no longer suppressed, are increasingly attenuated as the frequency increases, in such a way that the rectangular curve is converted into a periodic triangular signal. The direct component $(1 \hspace{0.05cm} \rm V)$ remains unchanged here, too.
- Thus, both filters provide the average value of the input signal. For the signal $x(t)$ at hand the filter $\rm A$ is more suitable than the filter $\rm B$for the determination of the mean value, because for the former the length of the impulse response is a multiple of the period $T_0 = 2T$ .
- If this condition – as with the filter $\rm B$ – is not fulfilled, an error signal (triangular in this example) is still superimposed on the mean value.