Difference between revisions of "Aufgaben:Exercise 2.12: Non-coherent Demodulation"
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Revision as of 15:26, 9 April 2022
Consider an amplitude modulated signal:
- $$ s(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$
Reaching the receiver based on the channel propagation time, the signal is
- $$ r(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \hspace{0.05cm}.$$
The arrangement shown here allows perfect demodulation – that is: $v(t) = q(t)$ – without knowledge of the phase $Δϕ_T$, but only if the source signal $q(t)$ satisfies certain conditions.
The two receiver-side carrier signals are:
- $$ z_{\rm 1, \hspace{0.08cm}E}(t) = 2 \cdot \cos(\omega_{\rm T} \cdot t) \hspace{0.05cm},$$
- $$ z_{\rm 2, \hspace{0.08cm}E}(t) = -2 \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$
$\rm LP_1$ and $\rm LP_2$ denote two ideal (rectangular) low-pass filters, each with cutoff frequency equal to the carrier frequency $f_{\rm T}$.
We consider as (digital) source signals:
- the unipolar square wave signal $q_1(t)$ with dimensionless amplitude values $0$ and $3$,
- the bipolar square wave signal $q_2(t)$ with the dimensionless amplitude values $±3$.
With respect to $s(t)$, these two signals result in
- an ASK signal,
- a BPSK signal.
The nonlinear function $v = g(b)$ is to be determined in this exercise.
Hints:
- This exercise belongs to the chapter Further AM Variants.
- Particular reference is made to the page Incoherent (non-coherent) Demodulation.
- The following trigonometric transformations are given:
- $$ \cos(\alpha) \cdot \cos(\beta) = 1/2 \cdot \big[ \cos(\alpha - \beta)+ \cos(\alpha + \beta) \big],$$
- $$ \sin(\alpha) \cdot \sin(\beta) = 1/2 \cdot \big[ \cos(\alpha - \beta)- \cos(\alpha + \beta) \big],$$
- $$ \sin(\alpha) \cdot \cos(\beta) = 1/2 \cdot \big[ \sin(\alpha - \beta)+ \sin(\alpha + \beta) \big] \hspace{0.05cm}.$$
Questions
Solution
- $$b_1(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \cdot 2 \cdot \cos(\omega_{\rm T} \cdot t) = q(t) \cdot \cos(\Delta \phi_{\rm T})\hspace{0.05cm},$$
- $$ b_2(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \cdot (-2) \cdot \sin(\omega_{\rm T} \cdot t) = q(t) \cdot \sin(\Delta \phi_{\rm T})\hspace{0.05cm}.$$
- Thus, the first and fourth answers are correct.
(2) The sum of the squares of the two partial signals gives:
- $$ b(t) = b_1^2(t) + b_2^2(t)= q^2(t) \cdot \left( \cos^2(\Delta \phi_{\rm T})+ \sin^2(\Delta \phi_{\rm T})\right) = q^2(t)\hspace{0.05cm}.$$
The possible amplitude values are thus:
- $$b_{\rm min}\hspace{0.15cm}\underline{ = 0},$$
- $$ b_{\rm max}\hspace{0.15cm}\underline{ =9}.$$
(3) The second answer is correct:
- $$v=g(b) = \sqrt{b} \hspace{0.3cm} \Rightarrow \hspace{0.3cm} v(t) = \sqrt{ q^2(t) } = q(t)\hspace{0.05cm}.$$
(4) The result $b(t) = q^2(t)$ – see subtask (2) – leads here to the result:
- $$b_{\rm min}\hspace{0.15cm}\underline{ = 9},$$
- $$b_{\rm max}\hspace{0.15cm}\underline{ =9}.$$
This shows that the demodulator considered here only functions,
- if at all times $q(t) ≥ 0$ or $q(t) ≤ 0$ holds,
- and this is known at the receiver.