Aufgaben:Exercise 4.5: Mutual Information from 2D-PDF: Difference between revisions

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For the differential entropies used here, the following equations apply:
For the differential entropies used here, the following equations apply:
:$$h(X) = -\hspace{-0.7cm}  \int\limits_{x \hspace{0.05cm}\in \hspace{0.05cm}{\rm supp}(f_X)} \hspace{-0.55cm}  f_X(x) \cdot {\rm log} \hspace{0.1cm} \big[f_X(x)\big] \hspace{0.1cm}{\rm d}x
:$$h(X) = -\hspace{-0.7cm}  \int\limits_{x \hspace{0.05cm}\in \hspace{0.05cm}{\rm supp}(f_X)} \hspace{-0.55cm}  f_X(x) \cdot {\rm log} \hspace{0.1cm} \big[f_X(x)\big] \hspace{0.1cm}{\rm d}x\hspace{0.05cm},$$
\hspace{0.05cm},$$
:$$h(Y) = -\hspace{-0.7cm}  \int\limits_{y \hspace{0.05cm}\in \hspace{0.05cm}{\rm supp}(f_Y)} \hspace{-0.55cm}  f_Y(y) \cdot {\rm log} \hspace{0.1cm} \big[f_Y(y)\big] \hspace{0.1cm}{\rm d}y\hspace{0.05cm},$$
:$$h(Y) = -\hspace{-0.7cm}  \int\limits_{y \hspace{0.05cm}\in \hspace{0.05cm}{\rm supp}(f_Y)} \hspace{-0.55cm}  f_Y(y) \cdot {\rm log} \hspace{0.1cm} \big[f_Y(y)\big] \hspace{0.1cm}{\rm d}y
:$$h(XY) = \hspace{0.1cm}-\hspace{0.2cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{XY}\hspace{-0.08cm})}\hspace{-0.6cm} f_{XY}(x, y) \cdot {\rm log} \hspace{0.1cm} \big[ f_{XY}(x, y) \big]\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y\hspace{0.05cm}.$$
\hspace{0.05cm},$$
:$$h(XY) = \hspace{0.1cm}-\hspace{0.2cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{XY}\hspace{-0.08cm})}  
\hspace{-0.6cm} f_{XY}(x, y) \cdot {\rm log} \hspace{0.1cm} \big[ f_{XY}(x, y) \big]
\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y\hspace{0.05cm}.$$
*For the two marginal probability density functions, the following holds:
*For the two marginal probability density functions, the following holds:
:$$f_X(x) = \hspace{-0.5cm}  \int\limits_{\hspace{-0.2cm}y \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{Y}\hspace{-0.08cm})} \hspace{-0.4cm} f_{XY}(x, y)  
:$$f_X(x) = \hspace{-0.5cm}  \int\limits_{\hspace{-0.2cm}y \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{Y}\hspace{-0.08cm})} \hspace{-0.4cm} f_{XY}(x, y)\hspace{0.15cm}{\rm d}y\hspace{0.05cm},$$
\hspace{0.15cm}{\rm d}y\hspace{0.05cm},$$
:$$f_Y(y) = \hspace{-0.5cm}  \int\limits_{\hspace{-0.2cm}x \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{X}\hspace{-0.08cm})} \hspace{-0.4cm} f_{XY}(x, y)\hspace{0.15cm}{\rm d}x\hspace{0.05cm}.$$
:$$f_Y(y) = \hspace{-0.5cm}  \int\limits_{\hspace{-0.2cm}x \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{X}\hspace{-0.08cm})} \hspace{-0.4cm} f_{XY}(x, y)  
\hspace{0.15cm}{\rm d}x\hspace{0.05cm}.$$




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Hints:  
Hints:  
*The exercise belongs to the chapter   [[Information_Theory/AWGN_Channel_Capacity_for_Continuous_Input#Mutual_information_between_continuous_random_variables|Mutual information with continuous input]].
*The exercise belongs to the chapter   [[Information_Theory/AWGN_Channel_Capacity_for_Continuous-Valued_Input#Mutual_information_between_continuous_random_variables|Mutual information with continuous input]].


*Let the following differential entropies also be given:
*Let the following differential entropies also be given:
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*Since  $f_{XY}(x, y)$  is constant in this area and the volume under  $f_{XY}(x, y)$  must be equal to  $1$,  the height is  $C = 1/F = 1/4$.  
*Since  $f_{XY}(x, y)$  is constant in this area and the volume under  $f_{XY}(x, y)$  must be equal to  $1$,  the height is  $C = 1/F = 1/4$.  
*From this follows for the differential joint entropy in  "bit":
*From this follows for the differential joint entropy in  "bit":
:$$h(XY) \  =  \  \hspace{0.1cm}-\hspace{0.2cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} \hspace{0.03cm}(\hspace{-0.03cm}f_{XY}\hspace{-0.08cm})}  
:$$h(XY) \  =  \  \hspace{0.1cm}-\hspace{0.2cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} \hspace{0.03cm}(\hspace{-0.03cm}f_{XY}\hspace{-0.08cm})}\hspace{-0.6cm} f_{XY}(x, y) \cdot {\rm log}_2 \hspace{0.1cm} [ f_{XY}(x, y) ]\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y$$
\hspace{-0.6cm} f_{XY}(x, y) \cdot {\rm log}_2 \hspace{0.1cm} [ f_{XY}(x, y) ]
:$$\Rightarrow \hspace{0.3cm} h(XY) \  =  \  \  {\rm log}_2 \hspace{0.1cm} (4) \cdot \hspace{0.02cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} \hspace{0.03cm}(\hspace{-0.03cm}f_{XY}\hspace{-0.08cm})}\hspace{-0.6cm} f_{XY}(x, y)\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y = 2 \,{\rm bit}\hspace{0.05cm}.$$
\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y$$
:$$\Rightarrow \hspace{0.3cm} h(XY) \  =  \  \  {\rm log}_2 \hspace{0.1cm} (4) \cdot \hspace{0.02cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} \hspace{0.03cm}(\hspace{-0.03cm}f_{XY}\hspace{-0.08cm})}  
\hspace{-0.6cm} f_{XY}(x, y)  
\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y = 2 \,{\rm bit}\hspace{0.05cm}.$$
*It is considered that the double integral is equal to&nbsp; $1$&nbsp;.&nbsp; The pseudo-unit&nbsp; "bit"&nbsp; corresponds to the&nbsp; "binary logarithm" &nbsp;&#8658;&nbsp; "log<sub>2</sub>".  
*It is considered that the double integral is equal to&nbsp; $1$&nbsp;.&nbsp; The pseudo-unit&nbsp; "bit"&nbsp; corresponds to the&nbsp; "binary logarithm" &nbsp;&#8658;&nbsp; "log<sub>2</sub>".  


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* Substituting these results into the above equation, we obtain:
* Substituting these results into the above equation, we obtain:
:$$I(X;Y) = h(X) + h(Y) - h(XY) = 1 \,{\rm bit} + 1 \,{\rm bit} - 2 \,{\rm bit} = 0 \,{\rm (bit)}
:$$I(X;Y) = h(X) + h(Y) - h(XY) = 1 \,{\rm bit} + 1 \,{\rm bit} - 2 \,{\rm bit} = 0 \,{\rm (bit)}\hspace{0.05cm}.$$
\hspace{0.05cm}.$$




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*In contrast,&nbsp; $X$&nbsp; is triangularly distributed between&nbsp; $0$&nbsp; and&nbsp; $4$&nbsp; $($with maximum at $2)$.&nbsp;  
*In contrast,&nbsp; $X$&nbsp; is triangularly distributed between&nbsp; $0$&nbsp; and&nbsp; $4$&nbsp; $($with maximum at $2)$.&nbsp;  
*This results in the same differential entropy&nbsp; $h(Y)$&nbsp; as for a symmetric triangular distribution in the range between&nbsp; $&plusmn;2$&nbsp;  (see specification sheet):
*This results in the same differential entropy&nbsp; $h(Y)$&nbsp; as for a symmetric triangular distribution in the range between&nbsp; $&plusmn;2$&nbsp;  (see specification sheet):
:$$h(X) = {\rm log}_2 \hspace{0.1cm} \big[\hspace{0.05cm}2 \cdot \sqrt{ e} \hspace{0.05cm}\big ]
:$$h(X) = {\rm log}_2 \hspace{0.1cm} \big[\hspace{0.05cm}2 \cdot \sqrt{ e} \hspace{0.05cm}\big ]= 1.721 \,{\rm bit}$$
= 1.721 \,{\rm bit}$$
:$$\Rightarrow \hspace{0.3cm} I(X;Y) =  1.721 \,{\rm bit} + 1 \,{\rm bit} - 2 \,{\rm bit}\hspace{0.05cm}\underline{ = 0.721 \,{\rm (bit)}}\hspace{0.05cm}.$$
:$$\Rightarrow \hspace{0.3cm} I(X;Y) =  1.721 \,{\rm bit} + 1 \,{\rm bit} - 2 \,{\rm bit}\hspace{0.05cm}\underline{ = 0.721 \,{\rm (bit)}}
\hspace{0.05cm}.$$
<br clear=all>
<br clear=all>
[[File:P_ID2889__Inf_A_4_5c_neu.png|right|frame|"„Green"&nbsp; probability density functions]]
[[File:P_ID2889__Inf_A_4_5c_neu.png|right|frame|"„Green"&nbsp; probability density functions]]
'''(3)'''&nbsp; The following properties are obtained for the green conditions:
'''(3)'''&nbsp; The following properties are obtained for the green conditions:
:$$F = A \cdot B \hspace{0.3cm}  \Rightarrow \hspace{0.3cm} C = \frac{1}{A \cdot B}
:$$F = A \cdot B \hspace{0.3cm}  \Rightarrow \hspace{0.3cm} C = \frac{1}{A \cdot B}\hspace{0.05cm}\hspace{0.3cm}\Rightarrow \hspace{0.3cm} h(XY)  =  {\rm log}_2 \hspace{0.1cm} (A \cdot B)\hspace{0.05cm}.$$
\hspace{0.05cm}\hspace{0.3cm}  
\Rightarrow \hspace{0.3cm} h(XY)  =  {\rm log}_2 \hspace{0.1cm} (A \cdot B)  
\hspace{0.05cm}.$$
*The random variable&nbsp; $Y$&nbsp; is now uniformly distributed between&nbsp; $0$&nbsp; and&nbsp; $A$&nbsp; and the random variable&nbsp; $X$&nbsp; is triangularly distributed between&nbsp; $0$&nbsp; and&nbsp; $2B$&nbsp; $($with maximum at&nbsp; $B)$:
*The random variable&nbsp; $Y$&nbsp; is now uniformly distributed between&nbsp; $0$&nbsp; and&nbsp; $A$&nbsp; and the random variable&nbsp; $X$&nbsp; is triangularly distributed between&nbsp; $0$&nbsp; and&nbsp; $2B$&nbsp; $($with maximum at&nbsp; $B)$:
:$$h(X)  \ =  \  {\rm log}_2 \hspace{0.1cm} (B \cdot \sqrt{ e})  
:$$h(X)  \ =  \  {\rm log}_2 \hspace{0.1cm} (B \cdot \sqrt{ e})\hspace{0.05cm},$$ $$h(Y)  \  =  \  {\rm log}_2 \hspace{0.1cm} (A)\hspace{0.05cm}.$$
\hspace{0.05cm},$$ $$
h(Y)  \  =  \  {\rm log}_2 \hspace{0.1cm} (A)\hspace{0.05cm}.$$
*Thus, for the mutual information between&nbsp; $X$&nbsp; and&nbsp; $Y$:
*Thus, for the mutual information between&nbsp; $X$&nbsp; and&nbsp; $Y$:
:$$I(X;Y)  \  =      {\rm log}_2 \hspace{0.1cm} (B \cdot \sqrt{ {\rm e}}) + {\rm log}_2 \hspace{0.1cm} (A) - {\rm log}_2 \hspace{0.1cm} (A \cdot B)$$  
:$$I(X;Y)  \  =      {\rm log}_2 \hspace{0.1cm} (B \cdot \sqrt{ {\rm e}}) + {\rm log}_2 \hspace{0.1cm} (A) - {\rm log}_2 \hspace{0.1cm} (A \cdot B)$$  
:$$\Rightarrow \hspace{0.3cm} I(X;Y)  =  \ {\rm log}_2 \hspace{0.1cm} \frac{B \cdot \sqrt{ {\rm e}} \cdot A}{A \cdot B} = {\rm log}_2 \hspace{0.1cm} (\sqrt{ {\rm e}})\hspace{0.15cm}\underline{= 0.721\,{\rm bit}}
:$$\Rightarrow \hspace{0.3cm} I(X;Y)  =  \ {\rm log}_2 \hspace{0.1cm} \frac{B \cdot \sqrt{ {\rm e}} \cdot A}{A \cdot B} = {\rm log}_2 \hspace{0.1cm} (\sqrt{ {\rm e}})\hspace{0.15cm}\underline{= 0.721\,{\rm bit}}\hspace{0.05cm}.$$
\hspace{0.05cm}.$$
[[File: P_ID2890__Inf_A_4_5d.png |right|frame|Other examples of 2D PDF&nbsp; $f_{XY}(x, y)$]]
[[File: P_ID2890__Inf_A_4_5d.png |right|frame|Other examples of 2D PDF&nbsp; $f_{XY}(x, y)$]]
*$I(X;Y)$&nbsp; thus independent of th PDF parameters&nbsp; $A$&nbsp; and&nbsp; $B$.
*$I(X;Y)$&nbsp; thus independent of th PDF parameters&nbsp; $A$&nbsp; and&nbsp; $B$.
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[[Category:Information Theory: Exercises|^4.2 AWGN and Value-Continuous Input^]]
[[Category:Information Theory: Exercises|^4.2 AWGN and Value-Continuous Input^]]
[[de:Aufgaben:Aufgabe 4.5: Transinformation aus 2D-WDF]]

Latest revision as of 17:58, 16 March 2026

Given joint PDF

Given here are the three different two-dimensional regions  $f_{XY}(x, y)$,  which in the task are identified by their fill colors with

  • red joint PDF,
  • blue joint PDF,
  • green joint PDF,


respectively.  Within each of the regions shown, let  $f_{XY}(x, y) = C = \rm const.$

For example, the mutual information between the continuous random variables  $X$  and  $Y$  can be calculated as follows:

$$I(X;Y) = h(X) + h(Y) - h(XY)\hspace{0.05cm}.$$

For the differential entropies used here, the following equations apply:

$$h(X) = -\hspace{-0.7cm} \int\limits_{x \hspace{0.05cm}\in \hspace{0.05cm}{\rm supp}(f_X)} \hspace{-0.55cm} f_X(x) \cdot {\rm log} \hspace{0.1cm} \big[f_X(x)\big] \hspace{0.1cm}{\rm d}x\hspace{0.05cm},$$
$$h(Y) = -\hspace{-0.7cm} \int\limits_{y \hspace{0.05cm}\in \hspace{0.05cm}{\rm supp}(f_Y)} \hspace{-0.55cm} f_Y(y) \cdot {\rm log} \hspace{0.1cm} \big[f_Y(y)\big] \hspace{0.1cm}{\rm d}y\hspace{0.05cm},$$
$$h(XY) = \hspace{0.1cm}-\hspace{0.2cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{XY}\hspace{-0.08cm})}\hspace{-0.6cm} f_{XY}(x, y) \cdot {\rm log} \hspace{0.1cm} \big[ f_{XY}(x, y) \big]\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y\hspace{0.05cm}.$$
  • For the two marginal probability density functions, the following holds:
$$f_X(x) = \hspace{-0.5cm} \int\limits_{\hspace{-0.2cm}y \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{Y}\hspace{-0.08cm})} \hspace{-0.4cm} f_{XY}(x, y)\hspace{0.15cm}{\rm d}y\hspace{0.05cm},$$
$$f_Y(y) = \hspace{-0.5cm} \int\limits_{\hspace{-0.2cm}x \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} (f_{X}\hspace{-0.08cm})} \hspace{-0.4cm} f_{XY}(x, y)\hspace{0.15cm}{\rm d}x\hspace{0.05cm}.$$




Hints:

  • Let the following differential entropies also be given:
  • If  $X$  is triangularly distributed between  $x_{\rm min}$  and  $x_{\rm max}$,  then:
$$h(X) = {\rm log} \hspace{0.1cm} [\hspace{0.05cm}\sqrt{ e} \cdot (x_{\rm max} - x_{\rm min})/2\hspace{0.05cm}]\hspace{0.05cm}.$$
  • If  $Y$  is equally distributed between  $y_{\rm min}$  and  $y_{\rm max}$,  then holds:
$$h(Y) = {\rm log} \hspace{0.1cm} \big [\hspace{0.05cm}y_{\rm max} - y_{\rm min}\hspace{0.05cm}\big ]\hspace{0.05cm}.$$
  • All results should be expressed in  "bit".   This is achieved with   $\log$  ⇒  $\log_2$.



Questions

1 What is the mutual information of  the red joint PDF?

$I(X; Y) \ = \ $ $\ \rm bit$

2 What is the mutual information of  the blue joint PDF?

$I(X; Y) \ = \ $ $\ \rm bit$

3 What is the mutual information of  the green joint PDF?

$I(X; Y) \ = \ $ $\ \rm bit$

4 What conditions must the random variables  $X$  and  $Y$  satisfy simultaneously for  $I(X;Y) = 1/2 \cdot \log (\rm e)$  to hold in general?

The two-dimensional PDF  $f_{XY}(x, y)$  results in a parallelogram.
One of the random variables  $(X$  or  $Y)$  is uniformly distributed.
The other random variable  $(Y$  or  $X)$  is triangularly distributed.


Solution

"Red"  probability density functions;
! Note:  Ordinate of  $f_{Y}(y)$  is directed to the left !

(1)  For the rectangular two-dimensional PDF  $f_{XY}(x, y)$  there are no statistical dependences between  $X$  and  $Y$    ⇒   $\underline{I(X;Y) = 0}$.

Formally, this result can be proved with the following equation:

$$I(X;Y) = h(X) \hspace{-0.05cm}+\hspace{-0.05cm} h(Y) \hspace{-0.05cm}- \hspace{-0.05cm}h(XY)\hspace{0.02cm}.$$
  • The red area of the two-dimensional PDF  $f_{XY}(x, y)$  is  $F = 4$. 
  • Since  $f_{XY}(x, y)$  is constant in this area and the volume under  $f_{XY}(x, y)$  must be equal to  $1$,  the height is  $C = 1/F = 1/4$.
  • From this follows for the differential joint entropy in  "bit":
$$h(XY) \ = \ \hspace{0.1cm}-\hspace{0.2cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} \hspace{0.03cm}(\hspace{-0.03cm}f_{XY}\hspace{-0.08cm})}\hspace{-0.6cm} f_{XY}(x, y) \cdot {\rm log}_2 \hspace{0.1cm} [ f_{XY}(x, y) ]\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y$$
$$\Rightarrow \hspace{0.3cm} h(XY) \ = \ \ {\rm log}_2 \hspace{0.1cm} (4) \cdot \hspace{0.02cm} \int \hspace{-0.9cm} \int\limits_{\hspace{-0.5cm}(x, y) \hspace{0.1cm}\in \hspace{0.1cm}{\rm supp} \hspace{0.03cm}(\hspace{-0.03cm}f_{XY}\hspace{-0.08cm})}\hspace{-0.6cm} f_{XY}(x, y)\hspace{0.15cm}{\rm d}x\hspace{0.15cm}{\rm d}y = 2 \,{\rm bit}\hspace{0.05cm}.$$
  • It is considered that the double integral is equal to  $1$ .  The pseudo-unit  "bit"  corresponds to the  "binary logarithm"  ⇒  "log2".


Furthermore:

  • The marginal probability density functions  $f_{X}(x)$  and  $f_{Y}(y)$  are rectangular   ⇒   uniform distribution between  $0$  and  $2$:
$$h(X) = h(Y) = {\rm log}_2 \hspace{0.1cm} (2) = 1 \,{\rm bit}\hspace{0.05cm}.$$
"Blue"  probability density functions
  • Substituting these results into the above equation, we obtain:
$$I(X;Y) = h(X) + h(Y) - h(XY) = 1 \,{\rm bit} + 1 \,{\rm bit} - 2 \,{\rm bit} = 0 \,{\rm (bit)}\hspace{0.05cm}.$$


(2)  Also for this parallelogram we get  $F = 4, \ C = 1/4$  as well as  $h(XY) = 2$ bit.

  • Here, as in subtask  (1) , the variable  $Y$  is uniformly distributed between  $0$  and  $2$   ⇒   $h(Y) = 1$ bit.
  • In contrast,  $X$  is triangularly distributed between  $0$  and  $4$  $($with maximum at $2)$. 
  • This results in the same differential entropy  $h(Y)$  as for a symmetric triangular distribution in the range between  $±2$  (see specification sheet):
$$h(X) = {\rm log}_2 \hspace{0.1cm} \big[\hspace{0.05cm}2 \cdot \sqrt{ e} \hspace{0.05cm}\big ]= 1.721 \,{\rm bit}$$
$$\Rightarrow \hspace{0.3cm} I(X;Y) = 1.721 \,{\rm bit} + 1 \,{\rm bit} - 2 \,{\rm bit}\hspace{0.05cm}\underline{ = 0.721 \,{\rm (bit)}}\hspace{0.05cm}.$$


"„Green"  probability density functions

(3)  The following properties are obtained for the green conditions:

$$F = A \cdot B \hspace{0.3cm} \Rightarrow \hspace{0.3cm} C = \frac{1}{A \cdot B}\hspace{0.05cm}\hspace{0.3cm}\Rightarrow \hspace{0.3cm} h(XY) = {\rm log}_2 \hspace{0.1cm} (A \cdot B)\hspace{0.05cm}.$$
  • The random variable  $Y$  is now uniformly distributed between  $0$  and  $A$  and the random variable  $X$  is triangularly distributed between  $0$  and  $2B$  $($with maximum at  $B)$:
$$h(X) \ = \ {\rm log}_2 \hspace{0.1cm} (B \cdot \sqrt{ e})\hspace{0.05cm},$$ $$h(Y) \ = \ {\rm log}_2 \hspace{0.1cm} (A)\hspace{0.05cm}.$$
  • Thus, for the mutual information between  $X$  and  $Y$:
$$I(X;Y) \ = {\rm log}_2 \hspace{0.1cm} (B \cdot \sqrt{ {\rm e}}) + {\rm log}_2 \hspace{0.1cm} (A) - {\rm log}_2 \hspace{0.1cm} (A \cdot B)$$
$$\Rightarrow \hspace{0.3cm} I(X;Y) = \ {\rm log}_2 \hspace{0.1cm} \frac{B \cdot \sqrt{ {\rm e}} \cdot A}{A \cdot B} = {\rm log}_2 \hspace{0.1cm} (\sqrt{ {\rm e}})\hspace{0.15cm}\underline{= 0.721\,{\rm bit}}\hspace{0.05cm}.$$
Other examples of 2D PDF  $f_{XY}(x, y)$
  • $I(X;Y)$  thus independent of th PDF parameters  $A$  and  $B$.






(4)  All of the above conditions are required.  However, the requirements  (2)  and  (3)  are not satisfied for every parallelogram. 

  • The adjacent graph shows two constellations, where the random variable  $X$  is equally distributed between  $0$  and  $1$  in each case.
  • For the top graph, the plotted points lie at a height   ⇒   $f_{Y}(y)$  is triangularly distributed   ⇒   $I(X;Y) = 0.721$ bit.
  • The lower composite PDF has a different mutual information, since the two plotted points are not at the same height  
    ⇒   the PDF  $f_{Y}(y)$  here has a trapezoidal shape.
  • Feeling, I guess  $I(X;Y) < 0.721$  bit,  since the two-dimensional area is more approaching a rectangle.  If you still feel like it, so check this statement.