Aufgaben:Exercise 4.2Z: Mixed Random Variables: Difference between revisions

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*In subtask  '''(4)'''  the differential entropy  $h(Y)$  of  $Y$   is to be determined (in bit), assuming the following equation:
*In subtask  '''(4)'''  the differential entropy  $h(Y)$  of  $Y$   is to be determined (in bit), assuming the following equation:
:$$h(Y) =  
:$$h(Y) =\hspace{0.1cm} - \hspace{-0.45cm} \int\limits_{{\rm supp}\hspace{0.03cm}(\hspace{-0.03cm}f_Y)} \hspace{-0.35cm}  f_Y(y) \cdot {\rm log}_2 \hspace{0.1cm} \big[ f_Y(y) \big] \hspace{0.1cm}{\rm d}y\hspace{0.05cm}.$$
\hspace{0.1cm} - \hspace{-0.45cm} \int\limits_{{\rm supp}\hspace{0.03cm}(\hspace{-0.03cm}f_Y)} \hspace{-0.35cm}  f_Y(y) \cdot {\rm log}_2 \hspace{0.1cm} \big[ f_Y(y) \big] \hspace{0.1cm}{\rm d}y  
\hspace{0.05cm}.$$


*In subtask  '''(2)''',  calculate the differential entropy   $h(X)$  of the random variable  $X$  whose PDF  $f_X(x)$  is sketched above.  If one performs a suitable boundary transition, the random variable  $X$  also becomes a mixed random variable.
*In subtask  '''(2)''',  calculate the differential entropy   $h(X)$  of the random variable  $X$  whose PDF  $f_X(x)$  is sketched above.  If one performs a suitable boundary transition, the random variable  $X$  also becomes a mixed random variable.
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{{ML-Kopf}}
'''(1)'''&nbsp; <u>Proposed solution 2</u>&nbsp; is correct because the integral&nbsp; $1$&nbsp; over the PDF must yield:
'''(1)'''&nbsp; <u>Proposed solution 2</u>&nbsp; is correct because the integral&nbsp; $1$&nbsp; over the PDF must yield:
:$$f_X(x) \hspace{0.1cm}{\rm d}x =
:$$f_X(x) \hspace{0.1cm}{\rm d}x =0.25 \cdot 2 + (A - 0.25) \cdot \varepsilon \stackrel{!}{=} 1 \hspace{0.3cm}\Rightarrow\hspace{0.3cm}(A - 0.25) \cdot \varepsilon \stackrel{!}{=} 0.5\hspace{0.3cm}\Rightarrow\hspace{0.3cm} A = 0.5/\varepsilon +0.25\hspace{0.05cm}.$$
0.25 \cdot 2 + (A - 0.25) \cdot \varepsilon \stackrel{!}{=} 1 \hspace{0.3cm}
\Rightarrow\hspace{0.3cm}(A - 0.25) \cdot \varepsilon \stackrel{!}{=} 0.5
\hspace{0.3cm}\Rightarrow\hspace{0.3cm} A = 0.5/\varepsilon +0.25\hspace{0.05cm}.$$






'''(2)'''&nbsp; The differential entropy (in "bit") is given as follows:
'''(2)'''&nbsp; The differential entropy (in "bit") is given as follows:
:$$h(X) =  
:$$h(X) =\hspace{0.1cm}  \hspace{-0.45cm} \int\limits_{{\rm supp}(f_X)} \hspace{-0.35cm}  f_X(x) \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{f_X(x)} \hspace{0.1cm}{\rm d}x\hspace{0.05cm}.$$
\hspace{0.1cm}  \hspace{-0.45cm} \int\limits_{{\rm supp}(f_X)} \hspace{-0.35cm}  f_X(x) \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{f_X(x)} \hspace{0.1cm}{\rm d}x  
\hspace{0.05cm}.$$
We now divide the integral into three partial integrals:
We now divide the integral into three partial integrals:
:$$h(X) =  
:$$h(X) =\hspace{-0.25cm} \int\limits_{0}^{1-\varepsilon/2} \hspace{-0.15cm}  0.25 \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.25} \hspace{0.1cm}{\rm d}x +\hspace{-0.25cm}\int\limits_{1+\varepsilon/2}^{2} \hspace{-0.15cm}  0.25 \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.25} \hspace{0.1cm}{\rm d}x+  \hspace{-0.25cm}\int\limits_{1-\varepsilon/2}^{1+\varepsilon/2} \hspace{-0.15cm}  \big [0.5/\varepsilon + 0.25 \big ] \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.5/\varepsilon + 0.25} \hspace{0.1cm}{\rm d}x $$
\hspace{-0.25cm} \int\limits_{0}^{1-\varepsilon/2} \hspace{-0.15cm}  0.25 \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.25} \hspace{0.1cm}{\rm d}x +
:$$  \Rightarrow \hspace{0.3cm} h(X) = 2 \cdot 0.25 \cdot 2 \cdot (2-\varepsilon) - (0.5 + 0.25 \cdot \varepsilon) \cdot {\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon +0.25)\hspace{0.05cm}.$$
\hspace{-0.25cm}\int\limits_{1+\varepsilon/2}^{2} \hspace{-0.15cm}  0.25 \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.25} \hspace{0.1cm}{\rm d}x
  +  \hspace{-0.25cm}\int\limits_{1-\varepsilon/2}^{1+\varepsilon/2} \hspace{-0.15cm}  \big [0.5/\varepsilon + 0.25 \big ] \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.5/\varepsilon + 0.25} \hspace{0.1cm}{\rm d}x $$  
:$$  \Rightarrow \hspace{0.3cm} h(X) = 2 \cdot 0.25 \cdot 2 \cdot (2-\varepsilon) - (0.5 + 0.25 \cdot \varepsilon) \cdot {\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon +0.25)
\hspace{0.05cm}.$$
In particular, one obtains
In particular, one obtains
* for&nbsp; $\varepsilon = 0.1$:
* for&nbsp; $\varepsilon = 0.1$:
:$$h(X) =1.9 - 0.525 \cdot {\rm log}_2 \hspace{0.1cm}(5.25) = 1.9 - 1.256
:$$h(X) =1.9 - 0.525 \cdot {\rm log}_2 \hspace{0.1cm}(5.25) = 1.9 - 1.256\hspace{0.15cm}\underline{= 0.644\,{\rm bit}}\hspace{0.05cm},$$
\hspace{0.15cm}\underline{= 0.644\,{\rm bit}}
\hspace{0.05cm},$$
* for&nbsp; $\varepsilon = 0.01$:
* for&nbsp; $\varepsilon = 0.01$:
:$$h(X) =1.99 - 0.5025 \cdot {\rm log}_2 \hspace{0.1cm}(50.25)= 1.99 - 2.84  
:$$h(X) =1.99 - 0.5025 \cdot {\rm log}_2 \hspace{0.1cm}(50.25)= 1.99 - 2.84\hspace{0.15cm}\underline{= -0.850\,{\rm bit}}\hspace{0.05cm}$$
\hspace{0.15cm}\underline{= -0.850\,{\rm bit}}
\hspace{0.05cm}$$  
* for&nbsp; $\varepsilon = 0.001$:
* for&nbsp; $\varepsilon = 0.001$:
:$$h(X) =1.999 - 0.50025 \cdot {\rm log}_2 \hspace{0.1cm}(500.25) = 1.999 - 8.967
:$$h(X) =1.999 - 0.50025 \cdot {\rm log}_2 \hspace{0.1cm}(500.25) = 1.999 - 8.967\hspace{0.15cm}\underline{= -6.968\,{\rm bit}}\hspace{0.05cm}.$$
\hspace{0.15cm}\underline{= -6.968\,{\rm bit}}
\hspace{0.05cm}.$$




'''(3)'''&nbsp; <u>All the proposed solutions</u>&nbsp; $1$&nbsp; are correct:  
'''(3)'''&nbsp; <u>All the proposed solutions</u>&nbsp; $1$&nbsp; are correct:  
*After the boundary transition &nbsp; $\varepsilon &#8594; 0$ &nbsp; we obtain for the differential entropy
*After the boundary transition &nbsp; $\varepsilon &#8594; 0$ &nbsp; we obtain for the differential entropy
:$$h(X) = \lim\limits_{\varepsilon \hspace{0.05cm}\rightarrow \hspace{0.05cm} 0} \hspace{0.1cm}\big[(2-\varepsilon) - (0.5 + 0.25 \cdot \varepsilon) \cdot {\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon +0.25)\big]  
:$$h(X) = \lim\limits_{\varepsilon \hspace{0.05cm}\rightarrow \hspace{0.05cm} 0} \hspace{0.1cm}\big[(2-\varepsilon) - (0.5 + 0.25 \cdot \varepsilon) \cdot {\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon +0.25)\big]= 2\,{\rm bit} - 0.5 \cdot \lim\limits_{\varepsilon \hspace{0.05cm}\rightarrow \hspace{0.05cm} 0}\hspace{0.1cm}{\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon)\hspace{0.3cm}\Rightarrow\hspace{0.3cm} - \infty\hspace{0.05cm}.$$
  = 2\,{\rm bit} - 0.5 \cdot \lim\limits_{\varepsilon \hspace{0.05cm}\rightarrow \hspace{0.05cm} 0}\hspace{0.1cm}{\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon)
\hspace{0.3cm}\Rightarrow\hspace{0.3cm} - \infty
\hspace{0.05cm}.$$
[[File:P_ID2871__Inf_Z_4_2c_neu.png|right|frame|PDF and CDF of the mixed random variable&nbsp; $X$]]
[[File:P_ID2871__Inf_Z_4_2c_neu.png|right|frame|PDF and CDF of the mixed random variable&nbsp; $X$]]
*The probability density function (PDF) in this case is given by.
*The probability density function (PDF) in this case is given by.
:$$f_X(x) = \left\{ \begin{array}{c} 0.25 + 0.5 \cdot \delta (x-1) \\  0 \\  \end{array} \right. \begin{array}{*{20}c}  {\rm{f\ddot{u}r}} \hspace{0.1cm} 0 \le x \le 2, \\    {\rm sonst} \\ \end{array}
:$$f_X(x) = \left\{ \begin{array}{c} 0.25 + 0.5 \cdot \delta (x-1) \\  0 \\  \end{array} \right. \begin{array}{*{20}c}  {\rm{f\ddot{u}r}} \hspace{0.1cm} 0 \le x \le 2, \\    {\rm sonst} \\ \end{array}\hspace{0.05cm}.$$
\hspace{0.05cm}.$$
Consequently, it is a&nbsp; "mixed"&nbsp; random variable with
Consequently, it is a&nbsp; "mixed"&nbsp; random variable with
* a stochastic, uniformly distributed part in the range&nbsp; $0 \le x \le 2$, and
* a stochastic, uniformly distributed part in the range&nbsp; $0 \le x \le 2$, and
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[[Category:Information Theory: Exercises|^4.1  Differential Entropy^]]
[[Category:Information Theory: Exercises|^4.1  Differential Entropy^]]
[[de:Aufgaben:4.02Z_Gemischte_Zufallsgrößen]]
[[de:Aufgaben:Aufgabe 4.2Z: Gemischte Zufallsgrößen]]

Latest revision as of 17:56, 16 March 2026

PDF of  $X$  (top),  and
CDF of  $Y$  (bottom)

One speaks of a  "mixed random variable",  if the random variable contains discrete components in addition to a continuous component.

  • For example, the random variable  $Y$  with  cumulative distribution function  $F_Y(y)$  as shown in the sketch below has both a continuous and a discrete component.
  • The  probability density function  $f_Y(y)$  is obtained from  $F_Y(y)$  by differentiation.
  • The jump at  $y= 1$  in the CDF thus becomes a "Dirac" in the probability density function.
  • In subtask  (4)  the differential entropy  $h(Y)$  of  $Y$  is to be determined (in bit), assuming the following equation:
$$h(Y) =\hspace{0.1cm} - \hspace{-0.45cm} \int\limits_{{\rm supp}\hspace{0.03cm}(\hspace{-0.03cm}f_Y)} \hspace{-0.35cm} f_Y(y) \cdot {\rm log}_2 \hspace{0.1cm} \big[ f_Y(y) \big] \hspace{0.1cm}{\rm d}y\hspace{0.05cm}.$$
  • In subtask  (2),  calculate the differential entropy  $h(X)$  of the random variable  $X$  whose PDF  $f_X(x)$  is sketched above.  If one performs a suitable boundary transition, the random variable  $X$  also becomes a mixed random variable.



Hints:



Questions

1 What is the PDF height  $A$  of  $f_X(x)$  around  $x = 1$?

$A = 0.5/\varepsilon$,
$A = 0.5/\varepsilon+0.25$,
$A = 1/\varepsilon$.

2 Calculate the differential entropy for different  $\varepsilon$–values.

$ε = 10^{-1}\text{:} \ \ h(X) \ = \ $ $\ \rm bit$
$ε = 10^{-2}\text{:} \ \ h(X) \ = \ $ $\ \rm bit$
$ε = 10^{-3}\text{:} \ \ h(X) \ = \ $ $\ \rm bit$

3 What is the result of the limit  $ε \to 0$?

$f_X(x)$  now has a continuous and a discrete component.
The differential energy  $h(X)$  is negative.
The magnitude  $|h(X)|$  is infinite.

4 Which statements are true for the random variable  $Y$?

The CDF value at the point  $y = 1$  is  $0.5$.
$Y$  contains a discrete and a continuous component.
The discrete component at   $Y = 1$  occurs with  $10\%$  probability.
The continuous component of  $Y$  is uniformly distributed.
The differential entropies of  $X$  and  $Y$  are equal.


Solution

(1)  Proposed solution 2  is correct because the integral  $1$  over the PDF must yield:

$$f_X(x) \hspace{0.1cm}{\rm d}x =0.25 \cdot 2 + (A - 0.25) \cdot \varepsilon \stackrel{!}{=} 1 \hspace{0.3cm}\Rightarrow\hspace{0.3cm}(A - 0.25) \cdot \varepsilon \stackrel{!}{=} 0.5\hspace{0.3cm}\Rightarrow\hspace{0.3cm} A = 0.5/\varepsilon +0.25\hspace{0.05cm}.$$


(2)  The differential entropy (in "bit") is given as follows:

$$h(X) =\hspace{0.1cm} \hspace{-0.45cm} \int\limits_{{\rm supp}(f_X)} \hspace{-0.35cm} f_X(x) \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{f_X(x)} \hspace{0.1cm}{\rm d}x\hspace{0.05cm}.$$

We now divide the integral into three partial integrals:

$$h(X) =\hspace{-0.25cm} \int\limits_{0}^{1-\varepsilon/2} \hspace{-0.15cm} 0.25 \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.25} \hspace{0.1cm}{\rm d}x +\hspace{-0.25cm}\int\limits_{1+\varepsilon/2}^{2} \hspace{-0.15cm} 0.25 \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.25} \hspace{0.1cm}{\rm d}x+ \hspace{-0.25cm}\int\limits_{1-\varepsilon/2}^{1+\varepsilon/2} \hspace{-0.15cm} \big [0.5/\varepsilon + 0.25 \big ] \cdot {\rm log}_2 \hspace{0.1cm} \frac{1}{0.5/\varepsilon + 0.25} \hspace{0.1cm}{\rm d}x $$
$$ \Rightarrow \hspace{0.3cm} h(X) = 2 \cdot 0.25 \cdot 2 \cdot (2-\varepsilon) - (0.5 + 0.25 \cdot \varepsilon) \cdot {\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon +0.25)\hspace{0.05cm}.$$

In particular, one obtains

  • for  $\varepsilon = 0.1$:
$$h(X) =1.9 - 0.525 \cdot {\rm log}_2 \hspace{0.1cm}(5.25) = 1.9 - 1.256\hspace{0.15cm}\underline{= 0.644\,{\rm bit}}\hspace{0.05cm},$$
  • for  $\varepsilon = 0.01$:
$$h(X) =1.99 - 0.5025 \cdot {\rm log}_2 \hspace{0.1cm}(50.25)= 1.99 - 2.84\hspace{0.15cm}\underline{= -0.850\,{\rm bit}}\hspace{0.05cm}$$
  • for  $\varepsilon = 0.001$:
$$h(X) =1.999 - 0.50025 \cdot {\rm log}_2 \hspace{0.1cm}(500.25) = 1.999 - 8.967\hspace{0.15cm}\underline{= -6.968\,{\rm bit}}\hspace{0.05cm}.$$


(3)  All the proposed solutions  $1$  are correct:

  • After the boundary transition   $\varepsilon → 0$   we obtain for the differential entropy
$$h(X) = \lim\limits_{\varepsilon \hspace{0.05cm}\rightarrow \hspace{0.05cm} 0} \hspace{0.1cm}\big[(2-\varepsilon) - (0.5 + 0.25 \cdot \varepsilon) \cdot {\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon +0.25)\big]= 2\,{\rm bit} - 0.5 \cdot \lim\limits_{\varepsilon \hspace{0.05cm}\rightarrow \hspace{0.05cm} 0}\hspace{0.1cm}{\rm log}_2 \hspace{0.1cm}(0.5/\varepsilon)\hspace{0.3cm}\Rightarrow\hspace{0.3cm} - \infty\hspace{0.05cm}.$$
PDF and CDF of the mixed random variable  $X$
  • The probability density function (PDF) in this case is given by.
$$f_X(x) = \left\{ \begin{array}{c} 0.25 + 0.5 \cdot \delta (x-1) \\ 0 \\ \end{array} \right. \begin{array}{*{20}c} {\rm{f\ddot{u}r}} \hspace{0.1cm} 0 \le x \le 2, \\ {\rm sonst} \\ \end{array}\hspace{0.05cm}.$$

Consequently, it is a  "mixed"  random variable with

  • a stochastic, uniformly distributed part in the range  $0 \le x \le 2$, and
  • a discrete component at  $x = 1$  with probability  $0.5$.


The graph shows the PDF  $f_X(x)$  on the left and the CDF  $F_X(x)$ on the right.
(4)  The correct solutions are 2, 3 and 5.  The lower graph shows the PDF and the CDF of the random variable  $Y$.  You can see:

PDF and CDF of the mixed random variable $Y$
  • Like $X$ ,  $Y$  contains a continuous and a discrete part.
  • The discrete part occurs with probability  ${\rm Pr}(Y = 1) = 0.1$.
  • Since  $F_Y(y)= {\rm Pr}(Y \le y)$  holds, the right-hand side limit is:
$$F_Y(y = 1) = 0.55.$$
  • The continuous component is not uniformly distributed;  rather, there is a triangular PDF.
  • The last proposition is also correct:   $h(Y) = h(X) = - \infty$.


Because:   For every random quantity with a discrete part – and it is also extremely small, the differential entropy is equal minus infinity..