Difference between revisions of "Aufgaben:Exercise 2.1Z: 2D-Frequency and 2D-Time Representations"
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$$h(\tau,\hspace{0.05cm}t) = \sum_{m = 1}^{M} z_m(t) \cdot {\rm \delta} (\tau - \tau_m)\hspace{0.05cm}.$$ | $$h(\tau,\hspace{0.05cm}t) = \sum_{m = 1}^{M} z_m(t) \cdot {\rm \delta} (\tau - \tau_m)\hspace{0.05cm}.$$ | ||
− | The first parameter $(\tau)$ indicates the delay | + | The first parameter $(\tau)$ indicates the delay, the second $(t)$ is related to the time variance of the channel. |
− | The Fourier | + | The Fourier transform of $h(\tau, t)$ in $\tau$ is the <i>time-variant transfer function</i> |
:$$H(f,\hspace{0.05cm} t) | :$$H(f,\hspace{0.05cm} t) | ||
\hspace{0.2cm} \stackrel {f,\hspace{0.05cm}{\a6}{\bullet}{\bullet\!-\!-\!-\!-\!-\!\circ} \hspace{0.2cm} h(\tau,\hspace{0.05cm}t) | \hspace{0.2cm} \stackrel {f,\hspace{0.05cm}{\a6}{\bullet}{\bullet\!-\!-\!-\!-\!-\!\circ} \hspace{0.2cm} h(\tau,\hspace{0.05cm}t) |
Revision as of 13:34, 15 April 2020
To describe a time-variant channel with several paths, the two-dimensional impulse response is used $$h(\tau,\hspace{0.05cm}t) = \sum_{m = 1}^{M} z_m(t) \cdot {\rm \delta} (\tau - \tau_m)\hspace{0.05cm}.$$
The first parameter $(\tau)$ indicates the delay, the second $(t)$ is related to the time variance of the channel.
The Fourier transform of $h(\tau, t)$ in $\tau$ is the time-variant transfer function
- $$H(f,\hspace{0.05cm} t) \hspace{0.2cm} \stackrel {f,\hspace{0.05cm}{\a6}{\bullet}{\bullet\!-\!-\!-\!-\!-\!\circ} \hspace{0.2cm} h(\tau,\hspace{0.05cm}t) \hspace{0.05cm}.$$
In the graph, $H(f, t)$ is displayed as a function of frequency, for different values of absolute time $t$ in the range of $0 \ \text{...} \ 10 \ \rm ms$.
In general, $H(f, t)$ is complex. The real part (top) and the imaginary part (bottom) are drawn separately.
Notes:
- This task belongs to the topic of the chapter Allgemeine Beschreibung zeitvarianter Systeme.
- In the above equation, an echo-free channel is represented with the parameter $M = 1$ .
- Here are some numerical values of the specified time-variant transfer function:
$$H(f,\hspace{0.05cm} t \hspace{-0.1cm} \ = \ \hspace{-0.1cm} 0\, {\rm ms}) \approx 0.3 - {\rm j} \cdot 0.4 \hspace{0.05cm},\hspace{0.2cm} H(f,\hspace{0.05cm} t = 2\, {\rm ms}) \approx 0.0 - {\rm j} \cdot 1.3 \hspace{0.05cm},$$ $$H(f,\hspace{0.05cm} t \hspace{-0.1cm} \ = \ \hspace{-0.1cm} 4\, {\rm ms}) \approx 0.1 - {\rm j} \cdot 1.5 \hspace{0.05cm},\hspace{0.2cm} H(f,\hspace{0.05cm} t = 6\, {\rm ms}) \approx 0.5 - {\rm j} \cdot 0.8 \hspace{0.05cm},$$ $$H(f,\hspace{0.05cm} t \hspace{-0.1cm} \ = \ \hspace{-0.1cm} 8\, {\rm ms}) \approx 0.9 - {\rm j} \cdot 0.1 \hspace{0.05cm},\hspace{0.2cm} H(f,\hspace{0.05cm} t = 10\, {\rm ms}) \approx 1.4 \hspace{0.05cm}.$$
- As can already be guessed from the above graphic, neither the real nor the imaginary part of the 2D–transfer function $H(f, t)$ are free of mean values.
=Questionnaire
Sample solution
{
(2) If we look at a fixed point in time, for example $t = 2 \ \rm ms$, we obtain the following for the time-variant transfer function
$$H(f,\hspace{0.05cm} t = 2\, {\rm ms}) = - {\rm j} \cdot 1.3 \hspace{0.05cm} = {\rm const.}$$
Thus the corresponding 2D–impulse response is $$h(\tau,\hspace{0.05cm} t = 2\, {\rm ms}) = - {\rm j} \cdot 1.3 \cdot \delta (\tau) \hspace{0.05cm} \hspace{0.3cm}\Rightarrow \hspace{0.3cm} M = 1 \hspace{0.05cm}.$$
With a path, however, multipath propagation cannot occur. This means that the correct solution is no.
(3) The correct solution is solution 3:
- There is time variance but no frequency selectivity.
- Proposals 1 and 2, on the other hand, describe time-invariant systems.
(4) Correct is the solution 4:
- For the AWGN–channel no transfer function can be specified.
- For a two-way channel, $H(f, t)$ is at no time $t$ constant.
- Since in the $H(f, t)$–graph in real– and imaginary part in each case an equal part not equal to zero can be recognized, the Rayleigh–channel can also be excluded.
- The data for the present task comes from a Rice–Channel with the following parameters:
- $$\sigma = {1}/{\sqrt{2}} \hspace{0.05cm},\hspace{0.2cm} x_0 = {1}/{\sqrt{2}} \hspace{0.05cm},\hspace{0.2cm}y_0 = -{1}/{\sqrt{2}} \hspace{0.05cm},\hspace{0.2cm} f_{\rm D,\hspace{0.05cm} max} = 100\,\,{\rm Hz}\hspace{0.05cm}.$