Aufgaben:Exercise 2.2: DC Component of Signals: Difference between revisions
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[[File:P_ID273__Sig_A_2_2.png|right|frame| | [[File:P_ID273__Sig_A_2_2.png|right|frame|Square wave signal with/ without DC component]] | ||
The graph shows six time signals defined for all times $($from $-\infty$ to $+\infty)$. For all sample signals $x_i(t)$ the associated spectral function can be written as: | |||
$$X_i(f)=A_0\cdot{\rm \delta}(f)+\Delta X_i(f).$$ | :$$X_i(f)=A_0\cdot{\rm \delta}(f)+\Delta X_i(f).$$ | ||
Here: | |||
*$A_0$ | *$A_0$ is the DC component of the signal. | ||
*$\Delta X_i(f)$ | *$\Delta X_i(f)$ is the spectrum of the residual signal reduced by the DC component: | ||
:$$\Delta x_i(t) = x_i(t) - A_0.$$ | |||
''Hint:'' | |||
*This exercise belongs to the chapter <br>[[Signal_Representation/Direct_Current_Signal_-_Limit_Case_of_a_Periodic_Signal|Direct Current Signal - Limit Case of a Periodic Signal]]. | |||
=== | ===Questions=== | ||
<quiz display=simple> | <quiz display=simple> | ||
{ | {Which of the signals contains a DC component, i.e. for which signals is $A_0 \neq 0$? | ||
|type="[]"} | |type="[]"} | ||
+ Signal $x_1(t),$ | + Signal $x_1(t),$ | ||
- | - signal $x_2(t),$ | ||
+ | + signal $x_3(t),$ | ||
+ | + signal $x_4(t),$ | ||
+ | + signal $x_5(t),$ | ||
+ | + signal $x_6(t).$ | ||
{ | {For which of the signals is the „residual spectrum” $\Delta X_i(f) =0$? | ||
|type="[]"} | |type="[]"} | ||
- Signal $x_1(t),$ | - Signal $x_1(t),$ | ||
- | - signal $x_2(t),$ | ||
- | - signal $x_3(t),$ | ||
- | - signal $x_4(t),$ | ||
+ | + signal $x_5(t),$ | ||
- | - signal $x_6(t).$ | ||
{ | {What is the DC component of the signal $x_3(t)$? | ||
|type="{}"} | |type="{}"} | ||
$x_3(t)\hspace{-0.1cm}:\,\,A_0 \ = \ $ { -0.35--0.31 } ${\rm V}$ | $x_3(t)\hspace{-0.1cm}:\,\,A_0 \ = \ $ { -0.35--0.31 } ${\rm V}$ | ||
{ | {What is the DC component of the signal $x_4(t)$? | ||
|type="{}"} | |type="{}"} | ||
$x_4(t)\hspace{-0.1cm}:\,\,A_0\ = \ $ { 0.5 3% } ${\rm V}$ | $x_4(t)\hspace{-0.1cm}:\,\,A_0\ = \ $ { 0.5 3% } ${\rm V}$ | ||
{ | {What is the DC component of the signal $x_6(t)$? | ||
|type="{}"} | |type="{}"} | ||
$x_6(t)\hspace{-0.1cm}:\,\,A_0\ = \ $ { 0.5 3% } ${\rm V}$ | $x_6(t)\hspace{-0.1cm}:\,\,A_0\ = \ $ { 0.5 3% } ${\rm V}$ | ||
| Line 59: | Line 59: | ||
</quiz> | </quiz> | ||
=== | ===Solution=== | ||
{{ML-Kopf}} | {{ML-Kopf}} | ||
'''(1)''' | '''(1)''' The correct <u>answers are 1, 3, 4, 5 and 6</u>. | ||
*All signals except $x_2(t)$ contain a DC signal component. | |||
'''(2)''' | '''(2)''' Only <u>solution 5 is correct</u>: | ||
*If the DC component $1\text{V}$ is subtracted from the signal $x_5(t)$, the residual signal $\Delta x_5(t) = x5(t) - 1\text{V}$ is zero. | |||
*Accordignly, the spectral function is $\Delta X_5(f) = 0$. | |||
*For all other time courses $\Delta x_i(t)ßne 0$ and thus the associated spectral function $\Delta X_i(f)\ne 0$, too. | |||
'''(3)''' | '''(3)''' Given a periodic signal, averaging over a period duration is sufficient to calculate the DC signal component $A_0$ . | ||
*For signal $x_3(t)$ the period duration is $T_0 = 3\,\text{ms}$. This results in the required DC component:$$A_0=\rm \frac{1}{3\,ms}\cdot \big[1\,V\cdot 1\,ms+(-1\,V)\cdot 2\,ms \big]\hspace{0.15cm}\underline{=-0.333\,V}.$$ | |||
$$A_0=\rm \frac{1}{3\,ms}\cdot [1\,V\cdot 1\,ms+(-1\,V)\cdot 2\,ms] | |||
\hspace{0.15cm}\underline{=-0.333\,V}.$$ | |||
'''(4)''' The signal $x_4(t)$ can be written as: $x_4(t) = 0.5 \,{\rm V} + Δx_4(t)$. | |||
*Here $Δx_4(t)$ denotes a rectangular pulse with amplitude $0.5 \,{\rm V} $ and duration $4 \,{\rm ms} $, | |||
*which due to its finite duration does not contribute to the DC signal component. | |||
*Therefore $A_0 \hspace{0.15cm}\underline{=0.5 \,{\rm V}}$ applies here. | |||
'''(5)''' | '''(5)''' The general equation for calculating the DC signal component is: | ||
$$A_0=\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int_{-T_{\rm M}/2}^{+T_{\rm M}/2}x(t)\, {\rm d }t.$$ | :$$A_0=\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int_{-T_{\rm M}/2}^{+T_{\rm M}/2}x(t)\, {\rm d }t.$$ | ||
*If one splits this integral into two partial integrals, one obtains: | |||
$$A_0=\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int _{-T_{\rm M}/2}^{0}0 {\rm V} \cdot\, {\rm d } {\it t }+\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int _{0}^{+T_{\rm M}/2}1 \rm V\ | :$$A_0=\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int _{-T_{\rm M}/2}^{0}0 {\rm V} \cdot\, {\rm d } {\it t }+\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int _{0}^{+T_{\rm M}/2}1 \rm V \ {\rm d }{\it t }.$$ | ||
*Only the second term makes a contribution. From this follows again : $A_0 \hspace{0.15cm}\underline{=0.5 \,{\rm V}}$. | |||
{{ML-Fuß}} | {{ML-Fuß}} | ||
__NOEDITSECTION__ | __NOEDITSECTION__ | ||
[[Category: | [[Category:Signal Representation: Exercises|^2.2 Direct Current Signal^]] | ||
[[de:Aufgaben:Aufgabe 2.2: Gleichsignalanteile]] | |||
Latest revision as of 17:53, 16 March 2026

The graph shows six time signals defined for all times $($from $-\infty$ to $+\infty)$. For all sample signals $x_i(t)$ the associated spectral function can be written as:
- $$X_i(f)=A_0\cdot{\rm \delta}(f)+\Delta X_i(f).$$
Here:
- $A_0$ is the DC component of the signal.
- $\Delta X_i(f)$ is the spectrum of the residual signal reduced by the DC component:
- $$\Delta x_i(t) = x_i(t) - A_0.$$
Hint:
- This exercise belongs to the chapter
Direct Current Signal - Limit Case of a Periodic Signal.
Questions
Solution
(1) The correct answers are 1, 3, 4, 5 and 6.
- All signals except $x_2(t)$ contain a DC signal component.
(2) Only solution 5 is correct:
- If the DC component $1\text{V}$ is subtracted from the signal $x_5(t)$, the residual signal $\Delta x_5(t) = x5(t) - 1\text{V}$ is zero.
- Accordignly, the spectral function is $\Delta X_5(f) = 0$.
- For all other time courses $\Delta x_i(t)ßne 0$ and thus the associated spectral function $\Delta X_i(f)\ne 0$, too.
(3) Given a periodic signal, averaging over a period duration is sufficient to calculate the DC signal component $A_0$ .
- For signal $x_3(t)$ the period duration is $T_0 = 3\,\text{ms}$. This results in the required DC component:$$A_0=\rm \frac{1}{3\,ms}\cdot \big[1\,V\cdot 1\,ms+(-1\,V)\cdot 2\,ms \big]\hspace{0.15cm}\underline{=-0.333\,V}.$$
(4) The signal $x_4(t)$ can be written as: $x_4(t) = 0.5 \,{\rm V} + Δx_4(t)$.
- Here $Δx_4(t)$ denotes a rectangular pulse with amplitude $0.5 \,{\rm V} $ and duration $4 \,{\rm ms} $,
- which due to its finite duration does not contribute to the DC signal component.
- Therefore $A_0 \hspace{0.15cm}\underline{=0.5 \,{\rm V}}$ applies here.
(5) The general equation for calculating the DC signal component is:
- $$A_0=\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int_{-T_{\rm M}/2}^{+T_{\rm M}/2}x(t)\, {\rm d }t.$$
- If one splits this integral into two partial integrals, one obtains:
- $$A_0=\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int _{-T_{\rm M}/2}^{0}0 {\rm V} \cdot\, {\rm d } {\it t }+\lim_{T_{\rm M}\to \infty}\frac{1}{T_{\rm M}}\int _{0}^{+T_{\rm M}/2}1 \rm V \ {\rm d }{\it t }.$$
- Only the second term makes a contribution. From this follows again : $A_0 \hspace{0.15cm}\underline{=0.5 \,{\rm V}}$.