Aufgaben:Exercise 1.10: BPSK Baseband Model: Difference between revisions
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{{quiz-Header|Buchseite= | {{quiz-Header|Buchseite=Digital_Signal_Transmission/Linear_Digital_Modulation_-_Coherent_Demodulation | ||
}} | }} | ||
[[File:P_ID1683__Dig_A_4_3.png|right|frame| | [[File:P_ID1683__Dig_A_4_3.png|right|frame|Unbalanced channel frequency response]] | ||
In this exercise, we consider a BPSK system with coherent demodulation, i.e. | |||
:$$s(t) \ = \ z(t) \cdot q(t),$$ | :$$s(t) \ = \ z(t) \cdot q(t),$$ | ||
:$$b(t) \ = \ 2 \cdot z(t) \cdot r(t) .$$ | :$$b(t) \ = \ 2 \cdot z(t) \cdot r(t) .$$ | ||
The designations chosen here are based on the [[Digital_Signal_Transmission/Linear_Digital_Modulation_-_Coherent_Demodulation#Common_block_diagram_for_ASK_and_BPSK|"block diagram"]] in the theory section. | |||
The influence of a channel frequency response $H_{\rm K}(f)$ can be taken into account in a simple way if it is described together with modulator and demodulator by a common baseband frequency response: | |||
:$$H_{\rm MKD}(f) = {1}/{2} \cdot \big [ H_{\rm K}(f-f_{\rm T}) + H_{\rm K}(f+f_{\rm T})\big ] .$$ | |||
*Thus the modulator and demodulator are virtually shortened against each other, and | |||
*the band-pass channel $H_{\rm K}(f)$ is transformed into the low-pass range. | |||
=== | The resulting transmission function $H_{\rm MKD}(f)$ should not be confused with the low-pass transmission function $H_{\rm K, \, TP}(f)$ as described in the chapter [[Signal_Representation/Equivalent_Low-Pass_Signal_and_its_Spectral_Function|"Equivalent Low-Pass Signal and its Spectral Function"]] of the book "Signal Representation", which results from $H_{\rm K}(f)$ by truncating the components at negative frequencies as well as a frequency shift by the carrier frequency $f_{\rm T}$ to the left. | ||
For frequency responses, in contrast to spectral functions, the doubling of the components at positive frequencies must be omitted. | |||
Notes: | |||
*The exercise belongs to the chapter [[Digital_Signal_Transmission/Linear_Digital_Modulation_-_Coherent_Demodulation|"Linear Digital Modulation - Coherent Demodulation"]]. | |||
*Reference is made in particular to the section [[Digital_Signal_Transmission/Linear_Digital_Modulation_-_Coherent_Demodulation#Baseband_model_for_ASK_and_BPSK|"Baseband model for ASK and BPSK"]]. | |||
*The subscript "MKD" stands for "modulator – channel – demodulator" German: "Modulator – Kanal – Demodulator"). | |||
===Questions=== | |||
<quiz display=simple> | <quiz display=simple> | ||
{ | |||
{Which statements are valid for the equivalent low-pass function $H_{\rm K, \, TP}(f)$ ? | |||
|type="[]"} | |type="[]"} | ||
- | - $H_{\rm K, \, TP}(f=0)= 2$. | ||
+ | + $H_{\rm K, \, TP}(f = \Delta f_{\rm K}/4) = 1$. | ||
+ $H_{\rm K, \, TP}(f = -\Delta f_{\rm K}/4) = 0.75$. | |||
+ The corresponding time function $h_{\rm K, \, TP}(t)$ is complex. | |||
{Which statements are valid for the frequency response $H_{\rm MKD}(f)$ ? | |||
|type="[]"} | |||
- $H_{\rm MKD}(f=0)= 2$. | |||
- $H_{\rm MKD}(f = \Delta f_{\rm K}/4) = 1$. | |||
+ $H_{\rm MKD}(f = -\Delta f_{\rm K}/4) = 0.75$. | |||
- The corresponding time function $h_{\rm MKD}(t)$ is complex. | |||
{ | {Calculate the time function $h_{\rm MKD}(t)$. Specify the value at $t = 0$. | ||
|type="{}"} | |type="{}"} | ||
$\ | $ h_{\rm MKD}(t = 0)/\Delta f_{\rm K} \ = \ $ { 0.75 3% } | ||
{Which of the following statements are true? | |||
|type="[]"} | |||
-$h_{\rm MKD}(t)$ has equidistant zero crossings at distance $1/\Delta f_{\rm K}$. | |||
+$h_{\rm MKD}(t)$ has equidistant zero crossings at distance $2/\Delta f_{\rm K}$. | |||
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</quiz> | </quiz> | ||
=== | ===Solution=== | ||
{{ML-Kopf}} | {{ML-Kopf}} | ||
'''(1)''' | '''(1)''' <u>Statements 2, 3 and 4</u> are correct: | ||
'''(2)''' | *$H_{\rm K,TP}(f)$ results from $H_{\rm K}(f)$ by cutting off the negative frequency components and shifting $f_{\rm T}$ to the left. | ||
'''(3)''' | |||
'''(4)''' | * For frequency responses – in contrast to spectra – the doubling of the components at positive frequencies is omitted. Therefore: | ||
:$$H_{\rm K,\hspace{0.04cm} TP}(f= 0) = H_{\rm K}(f= f_{\rm T})=1.$$ | |||
*Because of the real and asymmetrical spectral functions $H_{\rm K,\hspace{0.04cm}TP}(f),$ the corresponding time function (inverse Fourier transform) $h_{\rm K,\hspace{0.04cm}TP}(t)$ is complex according to the "Allocation Theorem". | |||
[[File:P_ID1684__Dig_A_4_3_a.png|right|frame|Low-pass functions for $H_{\rm K}(f)$]] | |||
'''(2)''' Here only the <u>third proposed solution</u> is correct: | |||
*The spectral function $H_{\rm MKD}(f)$ always has an even real part and no imaginary part. Consequently $h_{\rm MKD}(t)$ is always real. | |||
*If $H_{\rm K}(f)$ had additionally an imaginary part odd by $f= f_{\rm T}$, $H_{\rm MKD}(f)$ would have an imaginary part odd by $f = 0$. Thus $h_{\rm MKD}(t)$ would still be a real function. | |||
The diagram illustrates the differences between $H_{\rm K,\hspace{0.04cm}TP}(f)$ and $H_{\rm MKD}(f)$. The parts of $H_{\rm MKD}(f)$ in the range around $\pm 2f_{\rm T}$ need not be considered further. | |||
'''(3)''' $H_{\rm MKD}(f)$ is additively composed of a rectangle and a triangle, each with width $\Delta f_{\rm K}$ and height $0.5$. It follows: | |||
:$$h_{\rm MKD}(t) = \frac{\Delta f_{\rm K}}{2} \cdot {\rm sinc} ( \Delta f_{\rm K} \cdot t)+ \frac{\Delta f_{\rm K}}{4} \cdot {\rm sinc}^2 ( \frac{\Delta f_{\rm K}}{2} \cdot t)$$ | |||
:$$ \Rightarrow \hspace{0.3cm}h_{\rm MKD}(t = 0) = \frac{\Delta f_{\rm K}}{2} + \frac{\Delta f_{\rm K}}{4} = 0.75 \cdot \Delta f_{\rm K}\hspace{0.3cm}\Rightarrow \hspace{0.3cm}h_{\rm MKD}(t = 0)/{\Delta f_{\rm K}} \hspace{0.1cm}\underline {= 0.75} .$$ | |||
'''(4)''' The <u>second proposed solution</u> is correct: | |||
*The first sinc–function does have equidistant zero crossings at the distance $1/\Delta f_{\rm K}$. | |||
*But the equidistant zero crossings of the whole time function $h_{\rm MKD}(t)$ are determined by the second term: | |||
:$$h_{\rm MKD}(t = \frac{1}{\Delta f_{\rm K}}) = \ \frac{\Delta f_{\rm K}}{2} \cdot {\rm sinc} (1 )+\frac{\Delta f_{\rm K}}{4} \cdot {\rm sinc}^2 (0.5) = \frac{\Deltaf_{\rm K}}{4},$$ | |||
:$$h_{\rm MKD}(t = \frac{2}{\Delta f_{\rm K}}) = \ \frac{\Deltaf_{\rm K}}{2} \cdot {\rm sinc} (2 )+ \frac{\Delta f_{\rm K}}{4}\cdot {\rm sinc}^2 (1) = 0.$$ | |||
{{ML-Fuß}} | {{ML-Fuß}} | ||
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[[Category: | [[Category:Digital Signal Transmission: Exercises|^1.5 Linear Digital Modulation^]] | ||
[[de:Aufgaben:Aufgabe 1.10: BPSK–Basisbandmodell]] | |||
Latest revision as of 17:55, 16 March 2026

In this exercise, we consider a BPSK system with coherent demodulation, i.e.
- $$s(t) \ = \ z(t) \cdot q(t),$$
- $$b(t) \ = \ 2 \cdot z(t) \cdot r(t) .$$
The designations chosen here are based on the "block diagram" in the theory section.
The influence of a channel frequency response $H_{\rm K}(f)$ can be taken into account in a simple way if it is described together with modulator and demodulator by a common baseband frequency response:
- $$H_{\rm MKD}(f) = {1}/{2} \cdot \big [ H_{\rm K}(f-f_{\rm T}) + H_{\rm K}(f+f_{\rm T})\big ] .$$
- Thus the modulator and demodulator are virtually shortened against each other, and
- the band-pass channel $H_{\rm K}(f)$ is transformed into the low-pass range.
The resulting transmission function $H_{\rm MKD}(f)$ should not be confused with the low-pass transmission function $H_{\rm K, \, TP}(f)$ as described in the chapter "Equivalent Low-Pass Signal and its Spectral Function" of the book "Signal Representation", which results from $H_{\rm K}(f)$ by truncating the components at negative frequencies as well as a frequency shift by the carrier frequency $f_{\rm T}$ to the left.
For frequency responses, in contrast to spectral functions, the doubling of the components at positive frequencies must be omitted.
Notes:
- The exercise belongs to the chapter "Linear Digital Modulation - Coherent Demodulation".
- Reference is made in particular to the section "Baseband model for ASK and BPSK".
- The subscript "MKD" stands for "modulator – channel – demodulator" German: "Modulator – Kanal – Demodulator").
Questions
Solution
- $H_{\rm K,TP}(f)$ results from $H_{\rm K}(f)$ by cutting off the negative frequency components and shifting $f_{\rm T}$ to the left.
- For frequency responses – in contrast to spectra – the doubling of the components at positive frequencies is omitted. Therefore:
- $$H_{\rm K,\hspace{0.04cm} TP}(f= 0) = H_{\rm K}(f= f_{\rm T})=1.$$
- Because of the real and asymmetrical spectral functions $H_{\rm K,\hspace{0.04cm}TP}(f),$ the corresponding time function (inverse Fourier transform) $h_{\rm K,\hspace{0.04cm}TP}(t)$ is complex according to the "Allocation Theorem".

(2) Here only the third proposed solution is correct:
- The spectral function $H_{\rm MKD}(f)$ always has an even real part and no imaginary part. Consequently $h_{\rm MKD}(t)$ is always real.
- If $H_{\rm K}(f)$ had additionally an imaginary part odd by $f= f_{\rm T}$, $H_{\rm MKD}(f)$ would have an imaginary part odd by $f = 0$. Thus $h_{\rm MKD}(t)$ would still be a real function.
The diagram illustrates the differences between $H_{\rm K,\hspace{0.04cm}TP}(f)$ and $H_{\rm MKD}(f)$. The parts of $H_{\rm MKD}(f)$ in the range around $\pm 2f_{\rm T}$ need not be considered further.
(3) $H_{\rm MKD}(f)$ is additively composed of a rectangle and a triangle, each with width $\Delta f_{\rm K}$ and height $0.5$. It follows:
- $$h_{\rm MKD}(t) = \frac{\Delta f_{\rm K}}{2} \cdot {\rm sinc} ( \Delta f_{\rm K} \cdot t)+ \frac{\Delta f_{\rm K}}{4} \cdot {\rm sinc}^2 ( \frac{\Delta f_{\rm K}}{2} \cdot t)$$
- $$ \Rightarrow \hspace{0.3cm}h_{\rm MKD}(t = 0) = \frac{\Delta f_{\rm K}}{2} + \frac{\Delta f_{\rm K}}{4} = 0.75 \cdot \Delta f_{\rm K}\hspace{0.3cm}\Rightarrow \hspace{0.3cm}h_{\rm MKD}(t = 0)/{\Delta f_{\rm K}} \hspace{0.1cm}\underline {= 0.75} .$$
(4) The second proposed solution is correct:
- The first sinc–function does have equidistant zero crossings at the distance $1/\Delta f_{\rm K}$.
- But the equidistant zero crossings of the whole time function $h_{\rm MKD}(t)$ are determined by the second term:
- $$h_{\rm MKD}(t = \frac{1}{\Delta f_{\rm K}}) = \ \frac{\Delta f_{\rm K}}{2} \cdot {\rm sinc} (1 )+\frac{\Delta f_{\rm K}}{4} \cdot {\rm sinc}^2 (0.5) = \frac{\Deltaf_{\rm K}}{4},$$
- $$h_{\rm MKD}(t = \frac{2}{\Delta f_{\rm K}}) = \ \frac{\Deltaf_{\rm K}}{2} \cdot {\rm sinc} (2 )+ \frac{\Delta f_{\rm K}}{4}\cdot {\rm sinc}^2 (1) = 0.$$