Aufgaben:Exercise 5.3: Mean Square Error: Difference between revisions

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[[File:P_ID1145__Sig_A_5_3.png|250px|right|frame|Gaussian pulse, square pulse, sinc pulse and some parameters]]
[[File:P_ID1145__Sig_A_5_3.png|250px|right|frame|Gaussian pulse, square pulse, <br>sinc pulse and some parameters]]


We consider three pulse-like signals, namely
We consider three pulses, namely
*a&nbsp; [[Signal_Representation/Special_Cases_of_Impulse_Signals#Gaussian_Impulse|Gaussian pulse]]&nbsp; with amplitude&nbsp; $A$&nbsp; and  equivalent duration&nbsp; $T$:
*a&nbsp; [[Signal_Representation/Special_Cases_of_Pulses#Gaussian_pulse|Gaussian pulse]]&nbsp; with amplitude&nbsp; $A$&nbsp; and  equivalent duration&nbsp; $T$:
   
   
:$$x_1(t) = A \cdot {\rm e}^{- \pi (t/T)^2} \hspace{0.05cm},$$
:$$x_1(t) = A \cdot {\rm e}^{- \pi (t/T)^2} \hspace{0.05cm},$$


*a&nbsp; [[Signal_Representation/Special_Cases_of_Impulse_Signals#Rectangular_Impulse|Rectangular pulse]]&nbsp; $x_2(t)$&nbsp; with amplitude&nbsp; $A$&nbsp; and (equivalent) duration&nbsp; $T$:
*a&nbsp; [[Signal_Representation/Special_Cases_of_Pulses#Rectangular_pulse|rectangular pulse]]&nbsp; $x_2(t)$&nbsp; with amplitude&nbsp; $A$&nbsp; and (equivalent) duration&nbsp; $T$:
   
   
:$$x_2(t)  = \left\{ \begin{array}{c} A \\
:$$x_2(t)  = \left\{ \begin{array}{c} A \\0 \\  \end{array} \right.\quad\begin{array}{*{10}c}    {\rm{f\ddot{u}r}}\\  {\rm{f\ddot{u}r}} \\ \end{array}\begin{array}{*{20}c}|t| < T/2 \hspace{0.05cm}, \\|t| > T/2 \hspace{0.05cm}, \\\end{array}$$*a so called&nbsp; "sinc pulse"&nbsp; according to the following definition::$$x_3(t) = A \cdot {\rm sinc}(t/ T) ,\hspace{0.15cm}{\rm sinc}(x) =\sin(\pi x)/(\pi  x)\hspace{0.05cm}.$$
0 \\  \end{array} \right.\quad
\begin{array}{*{10}c}    {\rm{f\ddot{u}r}}
\\  {\rm{f\ddot{u}r}} \\ \end{array}\begin{array}{*{20}c}
|t| < T/2 \hspace{0.05cm}, \\
|t| > T/2 \hspace{0.05cm}, \\
\end{array}$$
 
*a so called&nbsp; ''Sinc pulse''&nbsp; according to the following definition:
:$$x_3(t) = A \cdot {\rm si}(\pi \cdot t/ T) ,\hspace{0.15cm}{\rm si}(x) =
\sin(x)/x\hspace{0.05cm}.$$


Let the signal parameters be&nbsp; $A = 1\ {\rm V}$&nbsp;  and&nbsp; $T = 1\ {\rm ms}$ in each case.
Let the signal parameters be&nbsp; $A = 1\ {\rm V}$&nbsp;  and&nbsp; $T = 1\ {\rm ms}$ in each case.


The conventional&nbsp; [[Signal_Representation/Fourier_Transform_and_Its_Inverse|Fourier Transform]]&nbsp;  leads to the following spectral functions:
The conventional&nbsp; [[Signal_Representation/Fourier_Transform_and_Its_Inverse|Fourier transform]]&nbsp;  leads to the following spectral functions:
* $X_1(f)$&nbsp; is also Gaussian,
* $X_1(f)$&nbsp; is also Gaussian,
* $X_2(f)$&nbsp; runs according to the&nbsp; $\rm si$–function,
* $X_2(f)$&nbsp; runs according to the&nbsp; $\rm sinc$ function,
* $X_3(f)$&nbsp; is constant for&nbsp; $|f| < 1/(2 T)$&nbsp; and outside zero.
* $X_3(f)$&nbsp; is constant for&nbsp; $|f| < 1/(2 T)$&nbsp; and outside zero.


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For all spectral functions,&nbsp; $X(f = 0) = A \cdot T$.
For all spectral functions,&nbsp; $X(f = 0) = A \cdot T$.


If the discrete-frequency spectrum is determined by the&nbsp; [[Signal_Representation/Discrete_Fourier_Transform_(DFT)|Discrete Fourier Transform(DFT)]]&nbsp; with the DFT parameters  
If the discrete-frequency spectrum is determined by the&nbsp; [[Signal_Representation/Discrete_Fourier_Transform_(DFT)|Discrete Fourier Transform]]&nbsp; $\rm (DFT)$&nbsp; with the DFT parameters  
* $N = 512$ &nbsp; &rArr; &nbsp; number of samples considered in the time and frequency domain,*$f_{\rm A}$  &nbsp; &rArr; &nbsp; interpolation distance in the frequency domain,
* $N = 512$ &nbsp; &rArr; &nbsp; number of samples considered in the time and frequency domain,
*$f_{\rm A}$  &nbsp; &rArr; &nbsp; interpolation distance in the frequency domain,




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The other DFT parameters are clearly fixed withn&bsp; $N$&nbsp; uan&nbsp; $f_{\rm A}$&nbsp; .The following applies to these:  
The other DFT parameters are clearly fixed withn&nbsp; $N$&nbsp; and&nbsp; $f_{\rm A}$.&nbsp; The following applies to these:  
:$$f_{\rm P} = N \cdot f_{\rm A},\hspace{0.3cm}T_{\rm P} = 1/f_{\rm A},\hspace{0.3cm}T_{\rm A} = T_{\rm
:$$f_{\rm P} = N \cdot f_{\rm A},\hspace{0.3cm}T_{\rm P} = 1/f_{\rm A},\hspace{0.3cm}T_{\rm A} = T_{\rm P}/N\hspace{0.05cm}.$$
P}/N
  \hspace{0.05cm}.$$


The accuracy of the respective DFT approximation is captured by thenbsp; ''mean square error''&nbsp; (MSE, here MQF):  
The accuracy of the respective DFT approximation is captured by the&nbsp; "mean square error"&nbsp; $\rm (MSE)$.&nbsp; <br>Here, we use the designation&nbsp; $\rm MQF$ &nbsp; &rArr; &nbsp; (German:&nbsp; "Mittlerer Quadratischer Fehler"):  
:$${\rm MQF} =  \frac{1}{N}\cdot \sum_{\mu = 0 }^{N-1}
:$${\rm MQF} =  \frac{1}{N}\cdot \sum_{\mu = 0 }^{N-1}\left|X(\mu \cdot f_{\rm A})-\frac{D(\mu)}{f_{\rm A}}\right|^2 \hspace{0.05cm}.$$
\left|X(\mu \cdot f_{\rm A})-\frac{D(\mu)}{f_{\rm A}}\right|^2 \hspace{0.05cm}.$$


The resulting MQF values are given in the graph above, valid for&nbsp; $N = 512$&nbsp; as well as for
The resulting MQF values are given in the graph above, valid for&nbsp; $N = 512$&nbsp; as well as for
Line 64: Line 51:


''Hints:''  
''Hints:''  
*This task belongs to the chapter&nbsp; [[Signal_Representation/Possible_Errors_When_Using_DFT|Possible Errors when Using DFT]].
*This task belongs to the chapter&nbsp; [[Signal_Representation/Possible_Errors_When_Using_DFT|Possible errors when using DFT]].
   
   
*The theory for this chapter is summarised in the learning video&nbsp; [[Fehlermöglichkeiten_bei_Anwendung_der_DFT_(Lernvideo)|Possible Errors when Using DFT]]&nbsp;.
*The theory for this chapter is summarised in the (German language) learning video <br> &nbsp; &nbsp; &nbsp;[[Fehlermöglichkeiten_bei_Anwendung_der_DFT_(Lernvideo)|Fehlermöglichkeiten bei Anwendung der DFT]] &nbsp; &rArr; &nbsp; "Possible errors when using DFT".




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$T_{\rm A}/T\ = \ $ { 0.01562 3% }
$T_{\rm A}/T\ = \ $ { 0.01562 3% }


{Due to which effects does the MQF value for the Gaussian pulse increase when using &nbsp;  $f_{\rm A} \cdot T = 1/4$&nbsp; instead of&nbsp; $f_{\rm A} \cdot T = 1/8$&nbsp; verwendet?
{Due to which effect does the MQF value for the Gaussian pulse increase when using &nbsp;  $f_{\rm A} \cdot T = 1/4$&nbsp; instead of&nbsp; $f_{\rm A} \cdot T = 1/8$?
|type="()"}
|type="()"}
+ The truncation error is significantly increased.
+ The truncation error is significantly increased.
- The aliasing error is significantly increased.
- The aliasing error is significantly increased.


{Due to what effects does the MQF value for the Gaussian momentum increase when using&nbsp; $f_{\rm A} \cdot T = 1/16$&nbsp; instead of  $f_{\rm A} \cdot T = 1/4$&nbsp; verwendet?
{Due to what effect does the MQF value for the Gaussian pulse increase when using&nbsp; $f_{\rm A} \cdot T = 1/16$&nbsp; instead of  $f_{\rm A} \cdot T = 1/4$?
|type="()"}
|type="()"}
- The termination error is significantly increased.termination
- The truncation error is significantly increased.
+ The aliasing error is significantly increased.
+ The aliasing error is significantly increased.


{Compare the MQF(MSE) values of the rectangular pulse&nbsp; $x_2(t)$&nbsp; with those of the Gaussian pulse&nbsp; $x_1(t)$. Which of the following statements are true?
{Compare the&nbsp; $\rm MQF$&nbsp; values of the rectangular pulse&nbsp; $x_2(t)$&nbsp; with those of the Gaussian pulse&nbsp; $x_1(t)$.&nbsp; Which of the following statements are true?
|type="[]"}
|type="[]"}
+ $\rm MQF$&nbsp; becomes larger because the spectral function&nbsp; $X_2(f)$&nbsp; decays asymptotically slower than&nbsp; $X_1(f)$.
+ $\rm MQF$&nbsp; becomes larger because the spectral function&nbsp; $X_2(f)$&nbsp; decays asymptotically slower than&nbsp; $X_1(f)$.
+ The aliasing error dominates.
+ The aliasing error dominates.
- The termination error dominates.
- The truncation error dominates.


{Compare the MQF values of the slit pulse&nbsp; $x_3(t)$&nbsp; with those of the Gaussian pulse&nbsp; $x_1(t)$. Which of the following statements are true?
{Compare the&nbsp; $\rm MQF$&nbsp; values of the "sinc pulse"&nbsp; $x_3(t)$&nbsp; with those of the Gaussian pulse&nbsp; $x_1(t)$.&nbsp; Which of the following statements are true?
|type="[]"}
|type="[]"}
- $\rm MQF$&nbsp; becomes larger because the spectral function&nbsp; $X_3(f)$&nbsp; decays asymptotically slower than&nbsp; $X_1(f)$.
- $\rm MQF$&nbsp; becomes larger because the spectral function&nbsp; $X_3(f)$&nbsp; decays asymptotically slower than&nbsp; $X_1(f)$.
- The aliasing error dominates.
- The aliasing error dominates.
+ The termination error dominates.
+ The truncation error dominates.


</quiz>
</quiz>
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'''(1)'''&nbsp; With the DFT parameters&nbsp; $N = 512$&nbsp; and&nbsp; $f_{\rm A} \cdot T = 1/8$&nbsp; the following follows after multiplying the two quantities:
'''(1)'''&nbsp; With the DFT parameters&nbsp; $N = 512$&nbsp; and&nbsp; $f_{\rm A} \cdot T = 1/8$&nbsp; the following follows after multiplying the two quantities:
:$$f_{\rm P} \cdot T = N \cdot (f_{\rm A} \cdot T) = 64.$$
:$$f_{\rm P} \cdot T = N \cdot (f_{\rm A} \cdot T) = 64.$$
*This covers the frequency range&nbsp; $–f_{\rm P}/2 \leq f < f_{\rm P}/2$&nbsp;:
*This covers the frequency range&nbsp; $-f_{\rm P}/2 \leq f < +f_{\rm P}/2$:
:$$f_{\rm max }\cdot T \hspace{0.15 cm}\underline{= 32}\hspace{0.05cm}.$$
:$$f_{\rm max }\cdot T \hspace{0.15 cm}\underline{= 32}\hspace{0.05cm}.$$


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'''(3)'''&nbsp; Correct is the <u>proposed solution 1 &nbsp; &rArr; &nbsp;  increase of the termination error</u>:
'''(3)'''&nbsp; Correct is the <u>proposed solution 1 &nbsp; &rArr; &nbsp;  increase of the truncation error</u>:
*This measure simultaneously halves&nbsp; $T_{\rm P}$&nbsp; from&nbsp; $8T$&nbsp; to&nbsp; $4T$&nbsp;.*Thus, only samples in the range&nbsp; $–2T \leq t < 2T$, are taken into account, which increases the termination error.  
*This measure simultaneously halves&nbsp; $T_{\rm P}$&nbsp; from&nbsp; $8T$&nbsp; to&nbsp; $4T$&nbsp;.
*The mean square error&nbsp; $(\rm MQF)$&nbsp; increases from&nbsp; $0.15 \cdot 10^{-15}$&nbsp; to&nbsp; $8 \cdot 10^{-15}$ for the Gaussian pulse&nbsp; $x_1(t)$&nbsp;, although the aliasing error actually decreases slightly by this measure.
*Thus, only samples in the range&nbsp; $–2T \leq t < 2T$ are taken into account, which increases the truncation error.  
*The mean square error&nbsp; $(\rm MQF)$&nbsp; increases from&nbsp; $0.15 \cdot 10^{-15}$&nbsp; to&nbsp; $8 \cdot 10^{-15}$ for the Gaussian pulse&nbsp; $x_1(t)$,&nbsp;  
*although the aliasing error actually decreases slightly by this measure.






'''(4)'''&nbsp; Correct is the <u>proposed solution 2 &nbsp; &rArr; &nbsp;  increase of the aliasing error:</u>:
'''(4)'''&nbsp; Correct is the <u>proposed solution 2 &nbsp; &rArr; &nbsp;  increase of the aliasing error:</u>:
*By halving&nbsp; $f_{\rm A}$&nbsp; wird auch&nbsp; $f_{\rm P}$&nbsp; is also halved.  
*By halving&nbsp; $f_{\rm A}$&nbsp; &rArr; &nbsp; $f_{\rm P}$&nbsp; is also halved.  
*As a result, the aliasing error becomes somewhat larger with a smaller termination error at the same time.  
*As a result, the aliasing error becomes somewhat larger with a smaller truncation error at the same time.  
*Overall, for the Gaussian pulse&nbsp; $x_1(t)$&nbsp;, the mean square error&nbsp; $(\rm MQF)$&nbsp; increases from&nbsp; $1.5 \cdot 10^{-16}$&nbsp; to&nbsp; $3.3 \cdot 10^{-16}$.
*Overall, for the Gaussian pulse&nbsp; $x_1(t)$, the mean square error&nbsp; $(\rm MQF)$&nbsp; increases from&nbsp; $1.5 \cdot 10^{-16}$&nbsp; to&nbsp; $3.3 \cdot 10^{-16}$.




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'''(5)'''&nbsp;  <u>Proposed solutions 1 and 2</u> are correct:
'''(5)'''&nbsp;  <u>Proposed solutions 1 and 2</u> are correct:
*As can be seen from the graph, the last statement is not true in contrast to the first two.  
*As can be seen from the graph, the last statement is not true in contrast to the first two.  
*Due to the slow,&nbsp; $\rm si$–shaped decay of the spectral function, the aliasing error dominates.  
*Due to the slow&nbsp; ($\rm sinc$–shaped)&nbsp; decay of the spectral function, the aliasing error dominates.  
*The&nbsp; $\rm MQF$ value at&nbsp; $f_{\rm A} \cdot T = 1/8$&nbsp; with&nbsp; $1.4 \cdot 10^{-5}$&nbsp; is therefore significantly larger than for the Gaussian pulse&nbsp; $(1.5 \cdot 10^{-16})$.
*The&nbsp; $\rm MQF$ value at&nbsp; $f_{\rm A} \cdot T = 1/8$&nbsp; with&nbsp; $1.4 \cdot 10^{-5}$&nbsp; is therefore significantly larger than for the Gaussian pulse&nbsp; $(1.5 \cdot 10^{-16})$.


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'''(6)'''&nbsp;  <u>Proposed solution 3</u> is correct:
'''(6)'''&nbsp;  <u>Proposed solution 3</u> is correct:
*The spectral function&nbsp; $X_3(f)$&nbsp; here has a rectangular lead, so that the first two statements do not apply.  
*The spectral function&nbsp; $X_3(f)$&nbsp; here has a rectangular lead, so that the first two statements do not apply.  
*On the other hand, a termination error is unavoidable with this&nbsp; $\rm si$–shaped time function. This leads to the large&nbsp; $\rm MQF$ values given.
*On the other hand, a truncation error is unavoidable with this&nbsp; $\rm sinc$–shaped time function.&nbsp; This leads to the large&nbsp; $\rm MQF$ values given.
{{ML-Fuß}}
{{ML-Fuß}}


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[[Category:Exercises for Signal Representation|^5.3 Possible DFT Errors^]]
[[Category:Signal Representation: Exercises|^5.3 Possible DFT Errors^]]
[[de:Aufgaben:Aufgabe 5.3: Mittlerer Quadratischer Fehler]]

Latest revision as of 17:56, 16 March 2026

Gaussian pulse, square pulse,
sinc pulse and some parameters

We consider three pulses, namely

  • Gaussian pulse  with amplitude  $A$  and equivalent duration  $T$:
$$x_1(t) = A \cdot {\rm e}^{- \pi (t/T)^2} \hspace{0.05cm},$$
  • rectangular pulse  $x_2(t)$  with amplitude  $A$  and (equivalent) duration  $T$:
$$x_2(t) = \left\{ \begin{array}{c} A \\0 \\ \end{array} \right.\quad\begin{array}{*{10}c} {\rm{f\ddot{u}r}}\\ {\rm{f\ddot{u}r}} \\ \end{array}\begin{array}{*{20}c}|t| < T/2 \hspace{0.05cm}, \\|t| > T/2 \hspace{0.05cm}, \\\end{array}$$*a so called  "sinc pulse"  according to the following definition::$$x_3(t) = A \cdot {\rm sinc}(t/ T) ,\hspace{0.15cm}{\rm sinc}(x) =\sin(\pi x)/(\pi x)\hspace{0.05cm}.$$

Let the signal parameters be  $A = 1\ {\rm V}$  and  $T = 1\ {\rm ms}$ in each case.

The conventional  Fourier transform  leads to the following spectral functions:

  • $X_1(f)$  is also Gaussian,
  • $X_2(f)$  runs according to the  $\rm sinc$ function,
  • $X_3(f)$  is constant for  $|f| < 1/(2 T)$  and outside zero.


For all spectral functions,  $X(f = 0) = A \cdot T$.

If the discrete-frequency spectrum is determined by the  Discrete Fourier Transform  $\rm (DFT)$  with the DFT parameters

  • $N = 512$   ⇒   number of samples considered in the time and frequency domain,
  • $f_{\rm A}$   ⇒   interpolation distance in the frequency domain,


this will lead to distortions due to truncation and/or aliasing errors.


The other DFT parameters are clearly fixed withn  $N$  and  $f_{\rm A}$.  The following applies to these:

$$f_{\rm P} = N \cdot f_{\rm A},\hspace{0.3cm}T_{\rm P} = 1/f_{\rm A},\hspace{0.3cm}T_{\rm A} = T_{\rm P}/N\hspace{0.05cm}.$$

The accuracy of the respective DFT approximation is captured by the  "mean square error"  $\rm (MSE)$. 
Here, we use the designation  $\rm MQF$   ⇒   (German:  "Mittlerer Quadratischer Fehler"):

$${\rm MQF} = \frac{1}{N}\cdot \sum_{\mu = 0 }^{N-1}\left|X(\mu \cdot f_{\rm A})-\frac{D(\mu)}{f_{\rm A}}\right|^2 \hspace{0.05cm}.$$

The resulting MQF values are given in the graph above, valid for  $N = 512$  as well as for

  • $f_{\rm A} \cdot T = 1/4$,
  • $f_{\rm A} \cdot T = 1/8$,
  • $f_{\rm A} \cdot T = 1/16$.





Hints:



Questions

1 Which range  $|f| \leq f_{\text{max}}$  is covered with  $N = 512$  and  $f_{\rm A} \cdot T = 1/8$ ?

$f_{\text{max}} \cdot T\ = \ $

2 At what time interval  $T_{\rm A}$  are the sampled values of  $x(t)$  available?

$T_{\rm A}/T\ = \ $

3 Due to which effect does the MQF value for the Gaussian pulse increase when using   $f_{\rm A} \cdot T = 1/4$  instead of  $f_{\rm A} \cdot T = 1/8$?

The truncation error is significantly increased.
The aliasing error is significantly increased.

4 Due to what effect does the MQF value for the Gaussian pulse increase when using  $f_{\rm A} \cdot T = 1/16$  instead of $f_{\rm A} \cdot T = 1/4$?

The truncation error is significantly increased.
The aliasing error is significantly increased.

5 Compare the  $\rm MQF$  values of the rectangular pulse  $x_2(t)$  with those of the Gaussian pulse  $x_1(t)$.  Which of the following statements are true?

$\rm MQF$  becomes larger because the spectral function  $X_2(f)$  decays asymptotically slower than  $X_1(f)$.
The aliasing error dominates.
The truncation error dominates.

6 Compare the  $\rm MQF$  values of the "sinc pulse"  $x_3(t)$  with those of the Gaussian pulse  $x_1(t)$.  Which of the following statements are true?

$\rm MQF$  becomes larger because the spectral function  $X_3(f)$  decays asymptotically slower than  $X_1(f)$.
The aliasing error dominates.
The truncation error dominates.


Solution

(1)  With the DFT parameters  $N = 512$  and  $f_{\rm A} \cdot T = 1/8$  the following follows after multiplying the two quantities:

$$f_{\rm P} \cdot T = N \cdot (f_{\rm A} \cdot T) = 64.$$
  • This covers the frequency range  $-f_{\rm P}/2 \leq f < +f_{\rm P}/2$:
$$f_{\rm max }\cdot T \hspace{0.15 cm}\underline{= 32}\hspace{0.05cm}.$$


(2)  The periodisation of the time function is based on the parameter  $T_{\rm P} = 1/f_{\rm A} = 8T$.

  • The distance between two samples is therefore
$$T_{\rm A}/T = \frac{T_{\rm P}/T}{N} = \frac{8}{512}\hspace{0.15 cm}\underline{ = 0.015625}\hspace{0.05cm}.$$


(3)  Correct is the proposed solution 1   ⇒   increase of the truncation error:

  • This measure simultaneously halves  $T_{\rm P}$  from  $8T$  to  $4T$ .
  • Thus, only samples in the range  $–2T \leq t < 2T$ are taken into account, which increases the truncation error.
  • The mean square error  $(\rm MQF)$  increases from  $0.15 \cdot 10^{-15}$  to  $8 \cdot 10^{-15}$ for the Gaussian pulse  $x_1(t)$, 
  • although the aliasing error actually decreases slightly by this measure.


(4)  Correct is the proposed solution 2   ⇒   increase of the aliasing error::

  • By halving  $f_{\rm A}$  ⇒   $f_{\rm P}$  is also halved.
  • As a result, the aliasing error becomes somewhat larger with a smaller truncation error at the same time.
  • Overall, for the Gaussian pulse  $x_1(t)$, the mean square error  $(\rm MQF)$  increases from  $1.5 \cdot 10^{-16}$  to  $3.3 \cdot 10^{-16}$.


(5)  Proposed solutions 1 and 2 are correct:

  • As can be seen from the graph, the last statement is not true in contrast to the first two.
  • Due to the slow  ($\rm sinc$–shaped)  decay of the spectral function, the aliasing error dominates.
  • The  $\rm MQF$ value at  $f_{\rm A} \cdot T = 1/8$  with  $1.4 \cdot 10^{-5}$  is therefore significantly larger than for the Gaussian pulse  $(1.5 \cdot 10^{-16})$.


(6)  Proposed solution 3 is correct:

  • The spectral function  $X_3(f)$  here has a rectangular lead, so that the first two statements do not apply.
  • On the other hand, a truncation error is unavoidable with this  $\rm sinc$–shaped time function.  This leads to the large  $\rm MQF$ values given.