Difference between revisions of "Aufgaben:Exercise 1.7Z: Overall Systems Analysis"

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:$$w(t) = {5\,\rm V}\cdot {\rm e}^{-\pi\hspace{0.05cm}\cdot \hspace{0.05cm}(t/T)^2}.$$
 
:$$w(t) = {5\,\rm V}\cdot {\rm e}^{-\pi\hspace{0.05cm}\cdot \hspace{0.05cm}(t/T)^2}.$$
 
What needs to be investigated is the range in which the equivalent impulse duration  $T$  of this Gaussian pulse can vary such that the overall system can be entirely described by the frequency response
 
What needs to be investigated is the range in which the equivalent impulse duration  $T$  of this Gaussian pulse can vary such that the overall system can be entirely described by the frequency response
:$$H_{\rm G}(f) = K \cdot {\rm e}^{-\pi\hspace{0.05cm}\cdot \hspace{0.05cm}(f/\Delta f_{\rm G})^2}$$. Here, the subscript "G" in frequency response and bandwidth stands for "Gesamtsystem" (German for "overall system").
+
:$$H_{\rm G}(f) = K \cdot {\rm e}^{-\pi\hspace{0.05cm}\cdot \hspace{0.05cm}(f/\Delta f_{\rm G})^2}.$$ Here, the subscript "G" in frequency response and bandwidth stands for "Gesamtsystem" (German for "overall system").
  
  

Revision as of 14:20, 8 September 2021

System with Gaussian low-passe filters and non-linear characteristic curve

An overall system  $G$  with input $w(t)$  and output  $z(t)$  consists of three components:

  • The first component is a Gaussian low-pass filter with impulse response
$$h_1(t) = \frac{1}{\Delta t_1} \cdot {\rm e}^{-\pi\hspace{0.05cm}\cdot \hspace{0.05cm} (t/\Delta t_1)^2}, \hspace{0.5cm} \Delta t_1= {0.3\,\rm ms}.$$
  • This is then followed by a non-linearity with the characteristic curve
$$y(t) = \left\{ \begin{array}{c} +{8\,\rm V} \\ 2 \cdot x(t) \\ {-8\,\rm V} \\ \end{array} \right.\quad \quad \begin{array}{*{10}c} {\rm{f\ddot{u}r}} \\ {\rm{f\ddot{u}r}} \\ {\rm{f\ddot{u}r}} \\ \end{array}\begin{array}{*{20}c} {x(t) \ge +{4\,\rm V}}, \\ {{-4\,\rm V} < x(t) < +{4\,\rm V}}, \\ {x(t)\le {-4\,\rm V}}. \\ \end{array}$$
⇒   The input signal  $x(t)$  of the non-linearity is amplified by the factor  $2$  and – if necessary – limited to the range  $±8 \ \rm V$ .
  • At the end of the chain there is again a Gaussian low-pass filter given by its frequency response:
$$H_3(f) = {\rm e}^{-\pi\hspace{0.05cm}\cdot \hspace{0.05cm}(f/\Delta f_3)^2}, \hspace{0.5cm} \Delta f_3= {2.5\,\rm kHz}.$$

Let the input signal $w(t)$  of the overall system be a Gaussian pulse with amplitude  $5 \ \rm V$  and variable (equivalent) duration  $T$:

$$w(t) = {5\,\rm V}\cdot {\rm e}^{-\pi\hspace{0.05cm}\cdot \hspace{0.05cm}(t/T)^2}.$$

What needs to be investigated is the range in which the equivalent impulse duration  $T$  of this Gaussian pulse can vary such that the overall system can be entirely described by the frequency response

$$H_{\rm G}(f) = K \cdot {\rm e}^{-\pi\hspace{0.05cm}\cdot \hspace{0.05cm}(f/\Delta f_{\rm G})^2}.$$ Here, the subscript "G" in frequency response and bandwidth stands for "Gesamtsystem" (German for "overall system").





Please note:



Questions

1

What conditions must be satisfied for the overall system to be describable by a single frequency response?

There is a linear relationship between  $w(t)$  and  $z(t)$.
$H_3(f)$  must be more narrow-band than  $H_1(f)$.
The signal  $x(t)$  must not be greater in magnitude than  $4 \ \rm V$.

2

Compute the maximum value for the equivalent impulse duration  $T$ so that the conditions given in  (1)  are satisfiable.

$T_{\rm max} \ = \ $

$\ \rm ms$

3

Specify the parameters of the overall frequency response  $H_{\rm G}(f)$ .

$K \ = \ $

$\Delta f_{\rm G} = \ $

$\ \rm kHz$


Solution

(1)  Answers 1 and 3 are correct:

  • The first statement is correct:   Only for a linear system a frequency response can be specified.
  • For this to be possible here nonlinearity must not play a role.
  • That is, it must be ensured that  $|x(t)|$  is not greater than  $4 \ \rm V$ .
  • In contrast to this, the second statement is not true:   The bandwidth of  $H_3(f)$  does not affect whether the non-linearity can be eliminated or not.


(2)  The first Gaussian low-pass filter is described in the frequency domain as follows:

$$X(f) = W(f) \cdot H_1(f) = {5\,\rm V}\cdot T \cdot {\rm e}^{-\pi(f \cdot T)^2} \cdot {\rm e}^{-\pi(f/\Delta f_1)^2} = {5\,\rm V}\cdot T \cdot {\rm e}^{-\pi f^2 (T^2 + \Delta t_1^2)}= {5\,\rm V}\cdot T \cdot {\rm e}^{-\pi(f/\Delta f_x)^2}.$$
  • Here,   $Δf_x$  denotes the equivalent bandwidth of  $X(f)$.
  • The signal value at  $t = 0$  is equal to the spectral area and at the same time to the maximum value of the signal:
  • This should not exceed $4 \ \rm V$:
$$x_{\rm max} = x(t =0) = {5\,\rm V}\cdot T \cdot \Delta f_x \le {4\,\rm V}.$$
  • From this it follows by comparison of coefficients:
$$\frac{1}{T \cdot \Delta f_x} > \frac{5}{4}\hspace{0.1cm} \Rightarrow \hspace{0.1cm} \frac{1}{T^2 \cdot \Delta f_x^2} > \frac{25}{16} \Rightarrow \hspace{0.3cm}\frac{T^2 + \Delta t_1^2}{T^2} > \frac{25}{16}$$
$$ \Rightarrow \hspace{0.1cm}\frac{ \Delta t_1^2}{T^2} > \frac{9}{16}\hspace{0.3cm}\Rightarrow \hspace{0.5cm}\frac{T^2}{ \Delta t_1^2} \le \frac{16}{9}\hspace{0.3cm}\Rightarrow \hspace{0.3cm} T \le \frac{4}{3} \cdot \Delta t_1 \hspace{0.15cm}\underline{= {0.4\,\rm ms}}.$$
  • The control calculation yields:
$$\Delta t_x = \sqrt{T^2 + \Delta t_1^2} = \sqrt{({0.4\,\rm ms})^2 + ({0.3\,\rm ms})^2} = {0.5\,\rm ms} \hspace{0.3cm}\Rightarrow \hspace{0.3cm}\Delta f_x = {1}/{\Delta t_x}= {2\,\rm kHz}$$
$$\Rightarrow \hspace{0.3cm} x(t=0) = {5\,\rm V}\cdot T \cdot \Delta f_x = {5\,\rm V}\cdot {0.4\,\rm ms} \cdot {2\,\rm kHz} = {4\,\rm V}.$$


(3)  The Gaussian low-pass filters satisfy the condition  $H_1(f = 0) = H_3(f = 0) = 1$.

  • Taking into account the gain of the second block in the linear domain the following is thus obtained for the total gain:
$$\underline{K \ = \ 2}.$$
  • For the equivalent impulse duration of the overall system it holds that:
$$\Delta t_{\rm G} = \sqrt{\Delta t_1^2 + \frac{1}{\Delta f_3^2}} = \sqrt{({0.3\,\rm ms})^2 + \left( \frac{1}{{2.5\,\rm kHz}}\right)^2}={0.5\,\rm ms} \; \; \Rightarrow \; \; \Delta f_{\rm G} = {1}/{\Delta t_{\rm G}} \hspace{0.15cm}\underline{= {2\,\rm kHz}}.$$