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

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

Revision as of 16:01, 17 May 2021

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  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 termination 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 termination 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  $f_{\rm A}$  wird auch  $f_{\rm P}$  is also halved.
  • As a result, the aliasing error becomes somewhat larger with a smaller termination 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,  $\rm si$–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 termination error is unavoidable with this  $\rm si$–shaped time function. This leads to the large  $\rm MQF$ values given.