Difference between revisions of "Aufgaben:Exercise 1.7: PDF of Rice Fading"

From LNTwww
Line 36: Line 36:
  
  
===Questionnaire==
+
===Questionnaire===
 
<quiz display=simple>
 
<quiz display=simple>
 
{Calculate some PDF values for&nbsp; $|z_0| = 0$&nbsp; and&nbsp; $\sigma = 2$:
 
{Calculate some PDF values for&nbsp; $|z_0| = 0$&nbsp; and&nbsp; $\sigma = 2$:
Line 62: Line 62:
  
 
===Sample solution===
 
===Sample solution===
{{{ML-Kopf}}
+
{{ML-Kopf}}
 
'''(1)'''&nbsp; With $|z_0| = 2$ and $\sigma = 2$ the Rice PDF is
 
'''(1)'''&nbsp; With $|z_0| = 2$ and $\sigma = 2$ the Rice PDF is
 
$$f_a(a) = a \cdot {\rm exp} [ -\frac{a^2 + 4}{2}] \cdot {\rm I}_0 (2a)\hspace{0.05cm}.$$
 
$$f_a(a) = a \cdot {\rm exp} [ -\frac{a^2 + 4}{2}] \cdot {\rm I}_0 (2a)\hspace{0.05cm}.$$
Line 81: Line 81:
  
 
'''(3)'''&nbsp; For the red curve the WDF&ndash;value $f_a(a = 1) \approx 0.35$ can be read from the [[Tasks:1.7_WDF_des_Rice%E2%80%93Fadings|Graphic]] on the data page. From this follows:
 
'''(3)'''&nbsp; For the red curve the WDF&ndash;value $f_a(a = 1) \approx 0.35$ can be read from the [[Tasks:1.7_WDF_des_Rice%E2%80%93Fadings|Graphic]] on the data page. From this follows:
$${\rm Pr}(a \le 1) = \frac{1}{2} \cdot 0.35 \hspace{0.15cm} \underline{ \approx 17.5\,\%} \hspace{0.05cm}.$
+
$${\rm Pr}(a \le 1) = \frac{1}{2} \cdot 0.35 \hspace{0.15cm} \underline{ \approx 17.5\,\%} \hspace{0.05cm}.$$
  
 
*This probability value will be a little too small because the red curve is concave in the range between $0$ and $1$.
 
*This probability value will be a little too small because the red curve is concave in the range between $0$ and $1$.
Line 88: Line 88:
  
 
'''(4)'''&nbsp; The Gaussian approximation states that one can approximate the Rice distribution by a Gaussian distribution with mean $|z_0| = \sqrt{10} = 3.16$ and dispersion $\sigma = 1$ if the quotient $|z_0|/\sigma$ is sufficiently large. Then applies:
 
'''(4)'''&nbsp; The Gaussian approximation states that one can approximate the Rice distribution by a Gaussian distribution with mean $|z_0| = \sqrt{10} = 3.16$ and dispersion $\sigma = 1$ if the quotient $|z_0|/\sigma$ is sufficiently large. Then applies:
$${\rm Pr}(a \le 1) \approx {\rm Pr}(g \le -2.16) = {\rm Q}(2.16) \hspace{0.15cm} \underline{ \approx 1.5\,\%} \hspace{0.05cm}.$
+
$${\rm Pr}(a \le 1) \approx {\rm Pr}(g \le -2.16) = {\rm Q}(2.16) \hspace{0.15cm} \underline{ \approx 1.5\,\%} \hspace{0.05cm}.$$
  
 
*Here $g$ denotes a Gaussian distributed random variable with the mean value $0$ and the dispersion $\sigma = 1$.  
 
*Here $g$ denotes a Gaussian distributed random variable with the mean value $0$ and the dispersion $\sigma = 1$.  

Revision as of 13:00, 15 April 2020

Rice-Fading für verschiedene Werte von  $|z_0|^2$

As you can see in the diagram, we consider the same scenario as in  Exercise 1.6:

  • Rice fading  with variance of the Gaussian processes   $\sigma^2 = 1$&nbsp, and parameter  $|z_0|$  for the direct path.
  • Regarding direct path, we are interested in the parameter values  $|z_0|^2 = 0, \ 2, \ 4, \ 10, \ 20$  (see graph).
  • The PDF of the magnitude  $a(t) = |z(t)|$  is
$$f_a(a) = \frac{a}{\sigma^2} \cdot {\rm exp} [ -\frac{a^2 + |z_0|^2}{2\sigma^2}] \cdot {\rm I}_0 \left [ \frac{a \cdot |z_0|}{\sigma^2} \right ]\hspace{0.05cm}.$$
  • For example, the modified zeroth order Bessel function returns the following values:

$${\rm I }_0 (2) = 2.28\hspace{0.05cm},\hspace{0.2cm}{\rm I }_0 (4) = 11.30\hspace{0.05cm},\hspace{0.2cm}{\rm I }_0 (3) = 67.23 \hspace{0.05cm}.$$

  • The power (noncentral second moment) of the multiplicative factor  $|z(t)|$ is

$${\rm E}\left [ a^2 \right ] = {\rm E}\left [ |z(t)|^2 \right ] = 2 \cdot \sigma^2 + |z_0|^2 \hspace{0.05cm}.$$

  • With  $z_0 = 0$,  the Rice fading  becomes Rayleigh fading, which is more critical. In this case, the probability that  $a$  lies in the yellow-shaded area between  $0$  and  $1$  is

$$ {\rm Pr}(a \le 1) = 1 - {\rm e}^{-0.5/\sigma^2} \approx 0.4 \hspace{0.05cm}.$$

In this task the probability  ${\rm Pr}(a ≤ 1)$  for  $|z_0| ≠ 0$  is to be approximated. There are two ways to do this, namely:

  • the triangular approximation:

$${\rm Pr}(a \le 1) = {1}/{2} \cdot f_a(a=1) \hspace{0.05cm}.$$

  • the Gaussian approximation:   If   $|z_0| \gg \sigma$, then the Rice distribution can be approximated by a Gaussian distribution with mean  $|z_0|$  and standard deviation  $\sigma$ .




Notes:



Questionnaire

1

Calculate some PDF values for  $|z_0| = 0$  and  $\sigma = 2$:

$f_a(a = 1) \ = \ $

$f_a(a = 2) \ = \ $

$f_a(a = 3) \ = \ $

2

Let   $|z_0| = 2$   ⇒   $|z_0|^2 = 4$  (blue curve). How big is  ${\rm Pr}(a ≤ 1)$? Use the  triangular approximation.

${\rm Pr}(a ≤ 1)\ = \ $

$\ \%$

3

Let   $|z_0|^2 = 2$  (red curve). How big is  ${\rm Pr}(a ≤ 1)$? Use the  triangular approximation.

${\rm Pr}(a ≤ 1) \ = \ $

$\ \%$

4

Let  $|z_0|^2 = 10$  (green curve). How big is  ${\rm Pr}(a ≤ 1)$? Use the  Gaussian approximation.

${\rm Pr}(a ≤ 1) \ = \ $

$\ \%$

5

Let  $|z_0|^2 = 20$  (purple curve). How big is  ${\rm Pr}(a ≤ 1)$? Use the  Gaussian approximation.

${\rm Pr}(a ≤ 1) \ = \ $

$\ \%$


Sample solution

(1)  With $|z_0| = 2$ and $\sigma = 2$ the Rice PDF is $$f_a(a) = a \cdot {\rm exp} [ -\frac{a^2 + 4}{2}] \cdot {\rm I}_0 (2a)\hspace{0.05cm}.$$

  • This gives the desired values:
$$f_a(a = 1) \hspace{-0.1cm} \ = \ \hspace{-0.1cm} 1 \cdot {\rm e}^{-2.5} \cdot {\rm I}_0 (2) = 0.082 \cdot 2.28 \hspace{0.15cm} \underline{ = 0.187}\hspace{0.05cm},$$
$$f_a(a = 2) \hspace{-0.1cm} \ = \ \hspace{-0.1cm} 2 \cdot {\rm e}^{-4} \cdot {\rm I}_0 (4) = 2 \cdot 0.0183 \cdot 11.3 \hspace{0.15cm} \underline{ = 0.414}\hspace{0.05cm},$$
$$f_a(a = 3) \hspace{-0.1cm} \ = \ \hspace{-0.1cm} 3 \cdot {\rm e}^{-6.5} \cdot {\rm I}_0 (6) = 3 \cdot 0.0015 \cdot 67.23 \hspace{0.15cm} \underline{ = 0.303}\hspace{0.05cm}.$$
  • The results fit well with the blue curve on the graph.


(2)  With the result of the subtask (1)   ⇒   $f_a(a = 1) = 0.187$ is obtained with the triangle approximation: $${\rm Pr}(a \le 1) = {1}/{2} \cdot 0.187 \cdot 1\hspace{0.15cm} \underline{ \approx 9.4\,\%} \hspace{0.05cm}.$$

  • This result will be a bit too large, because the blue curve is below the connecting line from $(0, 0)$ to $(1, 0.187)$   ⇒   convex curve.

(3)  For the red curve the WDF–value $f_a(a = 1) \approx 0.35$ can be read from the Graphic on the data page. From this follows: $${\rm Pr}(a \le 1) = \frac{1}{2} \cdot 0.35 \hspace{0.15cm} \underline{ \approx 17.5\,\%} \hspace{0.05cm}.$$

  • This probability value will be a little too small because the red curve is concave in the range between $0$ and $1$.


(4)  The Gaussian approximation states that one can approximate the Rice distribution by a Gaussian distribution with mean $|z_0| = \sqrt{10} = 3.16$ and dispersion $\sigma = 1$ if the quotient $|z_0|/\sigma$ is sufficiently large. Then applies: $${\rm Pr}(a \le 1) \approx {\rm Pr}(g \le -2.16) = {\rm Q}(2.16) \hspace{0.15cm} \underline{ \approx 1.5\,\%} \hspace{0.05cm}.$$

  • Here $g$ denotes a Gaussian distributed random variable with the mean value $0$ and the dispersion $\sigma = 1$.
  • The numerical value was determined with the specified interactive Applet.


Note:   The Gaussian approximation is certainly associated with a certain error here:

  • From the graph you can see that the average value of the green curve is not $a = $3.16$, but rather $3.31$. *Then the power of the Gaussian approximation $(3.31^2 + 1^2 = 12)$ is exactly the same as that of the Rice distribution: :'"`UNIQ-MathJax35-QINU`"' '''(5)'''  Using the same calculation method, replace the Rice–WDF with a Gauss–WDF with mean value $\sqrt{20} \approx $4.47 and spread $\sigma = $1 and you get '"`UNIQ-MathJax36-QINU`"' *If one assumes the equal power Gaussian distribution (see the note to the last subtask), the mean value is $m_g = \sqrt{21}\approx 4.58$, and the probability would then be

$${\rm Pr}(a \le 1) \approx {\rm Q}(3.58) \hspace{0.15cm} \underline{ \approx 0.02\,\%} \hspace{0.05cm}.$$