Difference between revisions of "Aufgaben:Exercise 1.3Z: Rayleigh Fading Revisited"

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'''(1)'''&nbsp; <u>YES</u>:  
 
'''(1)'''&nbsp; <u>YES</u>:  
*You can see the rotational symmetry here, too, if you consider that only $N = 10\hspace{0.05cm}000$ samples were displayed in the complex plane.  
+
*You can see the rotational symmetry here, too, if you consider that only&nbsp; $N = 10\hspace{0.05cm}000$&nbsp; samples were displayed in the complex plane.  
*Furthermore the following questions would not make sense if you answer NO.
+
*Furthermore the following questions would not make sense if you answer "NO".
  
  
  
'''(2)'''&nbsp; By measuring the two drawn circles you can see that for the &bdquo;blue&rdquo; channel the scattering of real&ndash; and imaginary part are larger by a factor of about 1.4 (exactly: $\sqrt{2}$) than for the &bdquo;red&rdquo; channel:
+
'''(2)'''&nbsp; By measuring the two drawn circles you can see that for the "blue" channel the scattering of real&ndash; and imaginary part are larger by a factor of about&nbsp; $1.4$&nbsp; <br>$($exactly:&nbsp; $\sqrt{2})$&nbsp; than for the "red" channel:
 
$$\sigma_{\rm B} = \sigma_{\rm R} \cdot \sqrt{2} = 0.5 \cdot \sqrt{2}= {1}/{\sqrt{2}}\hspace{0.15cm} \underline{\approx 0.707}
 
$$\sigma_{\rm B} = \sigma_{\rm R} \cdot \sqrt{2} = 0.5 \cdot \sqrt{2}= {1}/{\sqrt{2}}\hspace{0.15cm} \underline{\approx 0.707}
 
  \hspace{0.05cm}.$$
 
  \hspace{0.05cm}.$$
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'''(3)'''&nbsp; <u>NO</u>:  
 
'''(3)'''&nbsp; <u>NO</u>:  
*In both cases $f_{\it \phi}(\phi)$ describes a uniform distribution between $-\pi$ and $+\pi$.  
+
*In both cases&nbsp; $f_{\it \phi}(\phi)$&nbsp; describes a uniform distribution between&nbsp; $-\pi$&nbsp; and&nbsp; $+\pi$.  
*The larger amplitudes of channel &nbsp;$\rm B$&nbsp; are not important for the phase function $\phi(t)$.
+
*The larger amplitudes of channel&nbsp; &nbsp;$\rm B$&nbsp; are not important for the phase function&nbsp; $\phi(t)$.
  
  
  
 
'''(4)'''&nbsp; <u>Solution 2</u> is correct:  
 
'''(4)'''&nbsp; <u>Solution 2</u> is correct:  
*With Rayleigh fading, the real part $x(t)$ and the imaginary part $y(t)$ are each Gaussian distributed.  
+
*With Rayleigh fading, the real part&nbsp; $x(t)$&nbsp; and the imaginary part&nbsp; $y(t)$&nbsp; are each Gaussian distributed.  
*The exponential distribution results for the square of the absolute value $p(t) = |z(t)|^2$.
+
*The exponential distribution results for the square of the absolute value&nbsp; $p(t) = |z(t)|^2$.
  
  
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'''(6)'''&nbsp; The magnitude $a(t)$ is Rayleigh distributed. Therefore, the following holds for the desired probability:
+
'''(6)'''&nbsp; The magnitude&nbsp; $a(t)$ &nbsp;is Rayleigh distributed.&nbsp; Therefore, the following holds for the desired probability:
$${\rm Pr}(a > A) = \int_{A}^{\infty}\frac{a}{\sigma^2} \cdot {\rm e}^{ -{a^2}/(2\sigma^2)} \hspace{0.15cm}{\rm d}a \hspace{0.05cm}.$$
+
:$${\rm Pr}(a > A) = \int_{A}^{\infty}\frac{a}{\sigma^2} \cdot {\rm e}^{ -{a^2}/(2\sigma^2)} \hspace{0.15cm}{\rm d}a \hspace{0.05cm}.$$
  
 
*In some formula collections you can find the solution for this integral, but not in all.  
 
*In some formula collections you can find the solution for this integral, but not in all.  
*But it is also valid with the one-sided&ndash;exponentially distributed random variable $p = a^2$:
+
*But it is also valid with the one-sided exponentially distributed random variable&nbsp; $p = a^2$:
$${\rm Pr}(a > A) = {\rm Pr}(p > A^2) = \frac{1}{2\sigma^2} \cdot\int_{A^2}^{\infty} {\rm e}^{ -{p}/(2\sigma^2)} \hspace{0.15cm}{\rm d}p \hspace{0.05cm}.$$
+
:$${\rm Pr}(a > A) = {\rm Pr}(p > A^2) = \frac{1}{2\sigma^2} \cdot\int_{A^2}^{\infty} {\rm e}^{ -{p}/(2\sigma^2)} \hspace{0.15cm}{\rm d}p \hspace{0.05cm}.$$
  
 
*This integral is elementary and gives the result:
 
*This integral is elementary and gives the result:
$${\rm Pr}(a > A) = {\rm e}^{ -{A^2}/(2\sigma^2)} \hspace{0.05cm}.$$
+
:$${\rm Pr}(a > A) = {\rm e}^{ -{A^2}/(2\sigma^2)} \hspace{0.05cm}.$$
  
 
The correct answer is therefore <u>solution 2</u>.
 
The correct answer is therefore <u>solution 2</u>.
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'''(7)'''&nbsp; For the channel &nbsp;$\rm R$&nbsp; and $\sigma = 0.5$, we have
 
'''(7)'''&nbsp; For the channel &nbsp;$\rm R$&nbsp; and $\sigma = 0.5$, we have
$${\rm Pr}(|z(t)| > 1) = {\rm e}^{-2} \hspace{0.15cm} \underline{\approx 0.135}
+
:$${\rm Pr}(|z(t)| > 1) = {\rm e}^{-2} \hspace{0.15cm} \underline{\approx 0.135}
 
  \hspace{0.05cm}.$$
 
  \hspace{0.05cm}.$$
  
*In the upper graph this corresponds to the number of all points outside the circle drawn, based on the number $N = 10,000$ of all points.
+
*In the upper graph this corresponds to the number of all points outside the circle drawn, based on the number&nbsp; $N = 10,000$&nbsp; of all points.
  
*For the channel &nbsp;$\rm B$&nbsp; because of the double variance $\sigma^2 = 0.5$, we have ${\rm Pr}(|z(t)|>1) = {\rm e}^{-1}. \ \underline {\approx \ 0.368}$.  
+
*For the channel &nbsp;$\rm B$&nbsp; because of the double variance&nbsp; $\sigma^2 = 0.5$, we have&nbsp; ${\rm Pr}(|z(t)|>1) = {\rm e}^{-1} \ \underline {\approx \ 0.368}$.  
  
*The (not drawn) reference circle would also have radius 1 in the bottom graph.  
+
*The (not drawn) reference circle would also have radius&nbsp; $1$&nbsp; in the bottom graph.  
*The circle drawn in the bottom graph has a larger radius than $A = 1$, namely $A = \sqrt{2}\approx $1,414$.
+
*The circle drawn in the bottom graph has a larger radius than&nbsp; $A = 1$,&nbsp; namely&nbsp; $A = \sqrt{2}\approx 1.414$.
 
{{ML-Fuß}}
 
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[[Category:Exercises for Mobile Communications|^1.2 PDF of Rayleigh Fading^]]
 
[[Category:Exercises for Mobile Communications|^1.2 PDF of Rayleigh Fading^]]

Revision as of 16:06, 26 July 2020

Two channels, characterized by complex factor  $z(t)$

The graph shows the multiplicative factor  $z(t) = x(t) + {\rm j} \cdot y(t)$  of two mobile radio channels  (both without multipath propagation)  in 2D–representation.  The following is assumed:

  • The channel  $\rm R$  $($the designation results from the color "Red" of the point cloud$)$  is Rayleigh distributed with  $\sigma_{\rm R} = 0.5$.
  • The probability density functions (PDF) of the magnitude  $a(t) = |z(t)|$  or   the squared magnitude $p(t) = |z(t)|^2$  are $($with  $\sigma = \sigma_{\rm R})$:
$$f_a(a) = \left\{ \begin{array}{c} a/\sigma^2 \cdot {\rm e}^{ -{a^2}/(2\sigma^2)} \\ 0 \end{array} \right.\quad \begin{array}{*{1}c} {\rm f\ddot{u}r}\hspace{0.15cm} a \ge 0 \\ {\rm f\ddot{u}r}\hspace{0.15cm} a < 0 \\ \end{array} \hspace{0.05cm},$$
$$f_p(p) = \left\{ \begin{array}{c} 1/(2\sigma^2) \cdot {\rm e}^{ -{p}/(2\sigma^2)} \\ 0 \end{array} \right.\quad \begin{array}{*{1}c} {\rm f\ddot{u}r}\hspace{0.15cm} p \ge 0 \\ {\rm f\ddot{u}r}\hspace{0.15cm} p < 0 \\ \end{array} .$$
  • For channel  $\rm B$  ("Blue") only the point cloud is given. It must be estimated whether Rayleigh fading is also present here, and if YES, how large the parameter  $\sigma = \sigma_{\rm B}$  is for this channel.
  • Finally, subtask (3) also refers to the PDF  $f_{\it \phi}(\phi)$  of the phase function  $\phi(t)$ , which is defined as follows:
$$\phi(t) = \arctan \hspace{0.15cm} \frac{y(t)}{x(t)} \hspace{0.05cm}.$$




Notes:


Questionnaire

1

Can the channel  $\rm B$  also be modeled as Rayleigh fading?

Yes.
No.

2

Estimate the Rayleigh parameter of channel  $\rm B$.  Reminder:   For channel  $\rm R$  this parameter has the value  $\sigma_{\rm R} = 0.5$.

$\sigma_{\rm B}\ = \ $

3

Are the probability density functions  (PDFs)  $f_{\it \phi}(\phi)$  of the phases different for channel  $\rm R$  and  $\rm B$  and if   YES,   how?

Yes.
No.

4

What is the PDF  $f_a(a)$  with  $a(t) = |z(t)|$  in both cases?

The random variable  $a(t)$  is Gaussian distributed.
The random variable  $a(t)$  is Rayleigh distributed.
The random variable  $a(t)$  is positive and exponentially distributed.

5

What is the PDF  $f_p(p)$  in both cases with  $p(t) = |z(t)|^2$?

The random variable  $p(t)$  is Gaussian distributed.
The random variable  $p(t)$  is Rayleigh distributed.
The random variable  $p(t)$  is positive and exponentially distributed.

6

What is the probability that the random variable  $a(t) = |z(t)|$  is greater than a given value  $A$?

${\rm Pr}(|z(t)|) > A) = {\rm ln}(A/\sigma).$
${\rm Pr}(|z(t)|) > A) = {\rm e}^{-A^2/2\sigma^2}.$
${\rm Pr}(|z(t)|) > A) = {\rm e}^{-A/\sigma}.$

7

Calculate the probability  ${\rm Pr}(|z(t)| > 1)$ for both channels.

Channel  $\rm R$:$\hspace{0.4cm} {\rm Pr}(|z(t)| > 1)\ = \ $

Channel  $\rm B$:$\hspace{0.4cm} {\rm Pr}(|z(t)| > 1)\ = \ $


Sample solution

(1)  YES:

  • You can see the rotational symmetry here, too, if you consider that only  $N = 10\hspace{0.05cm}000$  samples were displayed in the complex plane.
  • Furthermore the following questions would not make sense if you answer "NO".


(2)  By measuring the two drawn circles you can see that for the "blue" channel the scattering of real– and imaginary part are larger by a factor of about  $1.4$ 
$($exactly:  $\sqrt{2})$  than for the "red" channel: $$\sigma_{\rm B} = \sigma_{\rm R} \cdot \sqrt{2} = 0.5 \cdot \sqrt{2}= {1}/{\sqrt{2}}\hspace{0.15cm} \underline{\approx 0.707} \hspace{0.05cm}.$$


(3)  NO:

  • In both cases  $f_{\it \phi}(\phi)$  describes a uniform distribution between  $-\pi$  and  $+\pi$.
  • The larger amplitudes of channel   $\rm B$  are not important for the phase function  $\phi(t)$.


(4)  Solution 2 is correct:

  • With Rayleigh fading, the real part  $x(t)$  and the imaginary part  $y(t)$  are each Gaussian distributed.
  • The exponential distribution results for the square of the absolute value  $p(t) = |z(t)|^2$.


(5)  Solution 3 is correct, as already explained in the sample solution for (4).


(6)  The magnitude  $a(t)$  is Rayleigh distributed.  Therefore, the following holds for the desired probability:

$${\rm Pr}(a > A) = \int_{A}^{\infty}\frac{a}{\sigma^2} \cdot {\rm e}^{ -{a^2}/(2\sigma^2)} \hspace{0.15cm}{\rm d}a \hspace{0.05cm}.$$
  • In some formula collections you can find the solution for this integral, but not in all.
  • But it is also valid with the one-sided exponentially distributed random variable  $p = a^2$:
$${\rm Pr}(a > A) = {\rm Pr}(p > A^2) = \frac{1}{2\sigma^2} \cdot\int_{A^2}^{\infty} {\rm e}^{ -{p}/(2\sigma^2)} \hspace{0.15cm}{\rm d}p \hspace{0.05cm}.$$
  • This integral is elementary and gives the result:
$${\rm Pr}(a > A) = {\rm e}^{ -{A^2}/(2\sigma^2)} \hspace{0.05cm}.$$

The correct answer is therefore solution 2.


(7)  For the channel  $\rm R$  and $\sigma = 0.5$, we have

$${\rm Pr}(|z(t)| > 1) = {\rm e}^{-2} \hspace{0.15cm} \underline{\approx 0.135} \hspace{0.05cm}.$$
  • In the upper graph this corresponds to the number of all points outside the circle drawn, based on the number  $N = 10,000$  of all points.
  • For the channel  $\rm B$  because of the double variance  $\sigma^2 = 0.5$, we have  ${\rm Pr}(|z(t)|>1) = {\rm e}^{-1} \ \underline {\approx \ 0.368}$.
  • The (not drawn) reference circle would also have radius  $1$  in the bottom graph.
  • The circle drawn in the bottom graph has a larger radius than  $A = 1$,  namely  $A = \sqrt{2}\approx 1.414$.