Aufgaben:Exercise 3.2Z: Sinc-Squared Spectrum with Diracs: Difference between revisions

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[[File:P_ID496__Sig_Z_3_2_neu.png|right|frame|$\rm si$-Quadrat-Spektrum mit Diracs]]
[[File:P_ID496__Sig_Z_3_2_neu.png|right|frame|$\rm sinc^2$– spectrum with Diracs]]
The sketched spectrum  ${X(f)}$  of a time signal  ${x(t)}$  is composed of
The sketched spectrum  ${X(f)}$  of a time signal  ${x(t)}$  is composed of


* a continuous component  $X_1(f)$,
* a continuous component  $X_1(f)$,


* plus three dirac-shaped spectral lines.
* plus three discrete spectral lines   ⇒    "Dirac functions".




The continuous component with  $f_0 = 200\, \text{kHz}$  and  $X_0 = 10^{–5} \text{ V/Hz}$is as follows:
The continuous component with  $f_0 = 200\, \text{kHz}$  and  $X_0 = 10^{–5} \text{ V/Hz}$ is as follows:
:$$X_1( f ) = X_0  \cdot {\mathop{\rm si}\nolimits} ^2 ( {\pi {f}/{f_0}} ),\quad {\rm where is}\quad {\mathop{\rm si}\nolimits} (x) = {\sin (x)}/{x}.$$
:$$X_1( f ) = X_0  \cdot {\mathop{\rm sinc}\nolimits} ^2 ( {{f}/{f_0}} ),\quad {\rm where is}\quad {\mathop{\rm sinc}\nolimits} (x) = {\sin (\pi x)}/(\pi x).$$
The spectral line at  $f = 0$  has the weight  $–\hspace{-0.08cm}1\,\text{V}$. In addition, there are two lines at frequencies  $\pm f_0$, both with weight  $0.5\,\text{V}$.
*The spectral line at  $f = 0$  has the weight  $–\hspace{-0.08cm}1\,\text{V}$.  
*In addition, there are two lines at frequencies  $\pm f_0$,  both with weight  $0.5\,\text{V}$.




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''Hints:''  
''Hints:''  
*This exercise belongs to the chapter  [[Signal_Representation/Fourier_Transform_and_Its_Inverse|Fourier Transform and Its Inverse]].
*This exercise belongs to the chapter  [[Signal_Representation/Fourier_Transform_and_Its_Inverse|Fourier Transform and its Inverse]].
*Further information on this topic can be found in the learning video  [[Kontinuierliche_und_diskrete_Spektren_(Lernvideo)|Kontinuierliche und diskrete Spektren]].
*Further information on this topic can be found in the (German language) learning video  [[Kontinuierliche_und_diskrete_Spektren_(Lernvideo)|Kontinuierliche und diskrete Spektren]]   ⇒   "Continuous and discrete spectra".
   
   
*It can be assumed as known that a triangular pulse  $y(t)$  symmetrical about  $t = 0$  with the amplitude  ${A}$  and the absolute duration  $2T$  $($i.e.:  he signal values are unequal to $ 0 $ only between  $–T$  and  $+T$ )  has the following spectral function:
*It can be assumed as known:  A triangular pulse  $y(t)$  with amplitude  ${A}$,  the absolute duration  $2T$  and symmetrical about  $t = 0$  $($i.e.:  the signal values are  $\ne 0 $  only between  $–T$  and  $+T$ )  has the following spectral function:
:$$Y( f ) = A  \cdot T \cdot {\rm si}^2 ( \pi f T ).$$
:$$Y( f ) = A  \cdot T \cdot {\rm sinc}^2 ( f T ).$$




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<quiz display=simple>
<quiz display=simple>
{What are the values of the parameters&nbsp; ${A}$&nbsp; (amplitude) and&nbsp; ${T}$&nbsp; (one-sided duration) of the triangular signal component&nbsp; $x_1(t)$?
{What are the values of the parameters&nbsp; ${A}$&nbsp; (maximum) and&nbsp; ${T}$&nbsp; (one-sided duration) of the triangular signal component&nbsp; $x_1(t)$?
|type="{}"}
|type="{}"}
$A\ = \ $ { 2 3% } &nbsp;$\text{V}$
$A\ = \ $ { 2 3% } &nbsp;$\text{V}$
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===Solution===
===Solution===
{{ML-Kopf}}
{{ML-Kopf}}
[[File:P_ID498__Sig_Z_3_2_a_neu.png|right|frame|Fläche des Dreieckimpulses]]
[[File:P_ID498__Sig_Z_3_2_a_neu.png|right|frame|Area of the triangular pulse]]
'''(1)'''&nbsp;  The one-sided duration of the symmetrical triangular pulse is&nbsp; $T = 1/f_0\hspace{0.15 cm}\underline{ = 5 \,{\rm &micro; s}}$.  
'''(1)'''&nbsp;  The one-sided duration of the symmetrical triangular pulse is&nbsp; $T = 1/f_0\hspace{0.15 cm}\underline{ = 5 \,{\rm &micro; s}}$.  


*The spectral value&nbsp; $X_0 = X_1(f = 0)$&nbsp; indicates the pulse area of&nbsp; $x_1(t)$&nbsp; an.  
*The spectral value&nbsp; $X_0 = X_1(f = 0)$&nbsp; indicates the pulse area of&nbsp; $x_1(t)$.  
*This is equal to&nbsp; ${A} \cdot {T}$.&nbsp; From this follows:
*This is equal to&nbsp; ${A} \cdot {T}$.&nbsp; From this follows:
:$$A = \frac{X_0 }{T}  = \frac{ 10^{-5}\rm V/Hz }{5 \cdot 10^{-6}{\rm s}}\hspace{0.15 cm}\underline{= 2\;{\rm V}}.$$
:$$A = \frac{X_0 }{T}  = \frac{ 10^{-5}\rm V/Hz }{5 \cdot 10^{-6}{\rm s}}\hspace{0.15 cm}\underline{= 2\;{\rm V}}.$$




'''(2)'''&nbsp;  The DC component is given by the Dirac weight at&nbsp; $f = 0$&nbsp;. One obtains&nbsp; ${B} \hspace{0.15 cm}\underline{= -1 \,\text{V}}$.
'''(2)'''&nbsp;  The DC component is given by the Dirac weight at&nbsp; $f = 0$.&nbsp; One obtains&nbsp; ${B} \hspace{0.15 cm}\underline{= -1 \,\text{V}}$.




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:$$x_{\text{max}} = A + B + C \hspace{0.15 cm}\underline{= +2 \text{V}}.$$  
:$$x_{\text{max}} = A + B + C \hspace{0.15 cm}\underline{= +2 \text{V}}.$$  


*The minimum values of&nbsp; ${x(t)}$&nbsp;  result when the triangular pulse has decayed and the cosine function delivers the value&nbsp; $–\hspace{-0.08 cm}1 \,\text{V}$&nbsp; liefert:  
*The minimum values of&nbsp; ${x(t)}$&nbsp;  result when the triangular pulse has decayed and the cosine function delivers the value&nbsp; $–\hspace{-0.08 cm}1 \,\text{V}$&nbsp;:  
:$$x_\text{min} = {B} - {C}\hspace{0.15 cm}\underline{ = -2\, \text{V}}.$$
:$$x_\text{min} = {B} - {C}\hspace{0.15 cm}\underline{ = -2\, \text{V}}.$$
{{ML-Fuß}}
{{ML-Fuß}}
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[[Category:Exercises for Signal Representation|^3.1 Fourier Transform and Its Inverse^]]
[[Category:Signal Representation: Exercises|^3.1 Fourier Transform and Its Inverse^]]
[[de:Aufgaben:Aufgabe 3.2Z: si-Quadrat-Spektrum mit Diracs]]

Latest revision as of 17:53, 16 March 2026

$\rm sinc^2$– spectrum with Diracs

The sketched spectrum  ${X(f)}$  of a time signal  ${x(t)}$  is composed of

  • a continuous component  $X_1(f)$,
  • plus three discrete spectral lines   ⇒   "Dirac functions".


The continuous component with  $f_0 = 200\, \text{kHz}$  and  $X_0 = 10^{–5} \text{ V/Hz}$ is as follows:

$$X_1( f ) = X_0 \cdot {\mathop{\rm sinc}\nolimits} ^2 ( {{f}/{f_0}} ),\quad {\rm where is}\quad {\mathop{\rm sinc}\nolimits} (x) = {\sin (\pi x)}/(\pi x).$$
  • The spectral line at  $f = 0$  has the weight  $–\hspace{-0.08cm}1\,\text{V}$.
  • In addition, there are two lines at frequencies  $\pm f_0$,  both with weight  $0.5\,\text{V}$.




Hints:

  • It can be assumed as known:  A triangular pulse  $y(t)$  with amplitude  ${A}$,  the absolute duration  $2T$  and symmetrical about  $t = 0$  $($i.e.:  the signal values are  $\ne 0 $  only between  $–T$  and  $+T$ )  has the following spectral function:
$$Y( f ) = A \cdot T \cdot {\rm sinc}^2 ( f T ).$$


Question

1 What are the values of the parameters  ${A}$  (maximum) and  ${T}$  (one-sided duration) of the triangular signal component  $x_1(t)$?

$A\ = \ $  $\text{V}$
$T\ = \ $  $\text{$µ$s}$

2 What is the DC component  ${B}$  of the signal?

$B\ = \ $  $\text{V}$

3 What is the amplitude  $C$  of the periodic component of  $x(t)$?

$C\ = \ $  $\text{V}$

4 What are the maximum and minimum values of the signal  $x(t)$?

$x_\text{max}\ = \ $  $\text{V}$
$x_\text{min}\hspace{0.2cm} = \ $  $\text{V}$


Solution

Area of the triangular pulse

(1)  The one-sided duration of the symmetrical triangular pulse is  $T = 1/f_0\hspace{0.15 cm}\underline{ = 5 \,{\rm µ s}}$.

  • The spectral value  $X_0 = X_1(f = 0)$  indicates the pulse area of  $x_1(t)$.
  • This is equal to  ${A} \cdot {T}$.  From this follows:
$$A = \frac{X_0 }{T} = \frac{ 10^{-5}\rm V/Hz }{5 \cdot 10^{-6}{\rm s}}\hspace{0.15 cm}\underline{= 2\;{\rm V}}.$$


(2)  The DC component is given by the Dirac weight at  $f = 0$.  One obtains  ${B} \hspace{0.15 cm}\underline{= -1 \,\text{V}}$.


(3)  The two spectral lines at  $\pm f_0$  together give a cosine signal with amplitude  ${C} \hspace{0.15 cm}\underline{= 1 \text{V}}$.


(4)  The maximum value occurs at time  ${t} = 0$    (here the triangular pulse and cosine signal are maximum):

$$x_{\text{max}} = A + B + C \hspace{0.15 cm}\underline{= +2 \text{V}}.$$
  • The minimum values of  ${x(t)}$  result when the triangular pulse has decayed and the cosine function delivers the value  $–\hspace{-0.08 cm}1 \,\text{V}$ :
$$x_\text{min} = {B} - {C}\hspace{0.15 cm}\underline{ = -2\, \text{V}}.$$