Difference between revisions of "Aufgaben:Exercise 5.2Z: About PN Modulation"
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===Solution=== | ===Solution=== | ||
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' The <u>last solution</u> is correct: | + | '''(1)''' The <u>last solution</u> is correct: |
*We are dealing here with an optimal receiver. | *We are dealing here with an optimal receiver. | ||
− | *Without noise, the signal b(t) within each bit is constantly equal to +1 or −1. | + | *Without noise, the signal b(t) within each bit is constantly equal to +1 or −1. |
*From the given equation for the integrator | *From the given equation for the integrator | ||
:d(νT)=1T⋅∫νT(ν−1)Tb(t)dt | :d(νT)=1T⋅∫νT(ν−1)Tb(t)dt | ||
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− | '''(2)''' Again the <u>last solution</u> is correct: | + | '''(2)''' Again the <u>last solution</u> is correct: |
* In the noise– and interference-free case ⇒ n(t)=0, the twofold multiplication by c(t) ∈ \{+1, –1\} can be omitted, | * In the noise– and interference-free case ⇒ n(t) = 0, the twofold multiplication by c(t) ∈ \{+1, –1\} can be omitted, | ||
*so that the upper model is identical to the lower model. | *so that the upper model is identical to the lower model. | ||
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− | '''(3)''' <u>Solution 1</u> is correct: | + | '''(3)''' <u>Solution 1</u> is correct: |
− | *Since both models are identical in the noise-free case, only the noise signal has to be adjusted: n'(t) = n(t) · c(t). | + | *Since both models are identical in the noise-free case, only the noise signal has to be adjusted: n'(t) = n(t) · c(t). |
− | *In contrast, the other two solutions are not applicable: | + | *In contrast, the other two solutions are not applicable: |
*The integration must still be done over T = J · T_c and the PN modulation does not reduce the AWGN noise. | *The integration must still be done over T = J · T_c and the PN modulation does not reduce the AWGN noise. | ||
− | '''(4)''' The <u>last solution</u> is correct: | + | '''(4)''' The <u>last solution</u> is correct: |
− | *Multiplying the AWGN noise by the high-frequency ±1 signal c(t), the product is also Gaussian and white. | + | *Multiplying the AWGN noise by the high-frequency ±1 signal c(t), the product is also Gaussian and white. |
*Because of {\rm E}\big[c^2(t)\big] = 1, the noise variance is not changed either. | *Because of {\rm E}\big[c^2(t)\big] = 1, the noise variance is not changed either. | ||
− | *Thus, the equation p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt {{2 E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right ) valid for BPSK is also applicable for PN modulation, independent of the spreading factor J and the specific spreading sequence. | + | *Thus, the equation p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt {{2 E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right ) valid for BPSK is also applicable for PN modulation, independent of the spreading factor J and the specific spreading sequence. |
− | *Ergo: For AWGN noise, band spreading neither increases nor decreases the error probability. | + | *Ergo: For AWGN noise, band spreading neither increases nor decreases the error probability. |
{{ML-Fuß}} | {{ML-Fuß}} | ||
Revision as of 16:09, 8 December 2021
The upper diagram shows the equivalent circuit of \rm PN modulation (Direct-Sequence Spread Spectrum, abbreviated \rm DS–SS) in the equivalent low-pass range, based on AWGN noise n(t).
Shown below is the low-pass model of binary phase shift keying \rm (BPSK). The low-pass transmitted signal s(t) is set equal to the rectangular source signal q(t) ∈ \{+1, –1\} with rectangular duration T for reasons of uniformity.
The function of the integrator can be described as follows:
- d (\nu T) = \frac{1}{T} \cdot \hspace{-0.1cm} \int_{(\nu -1 )T }^{\nu T} \hspace{-0.3cm} b (t )\hspace{0.1cm} {\rm d}t \hspace{0.05cm}.
The two models differ by multiplication with the ±1 spreading signal c(t) at transmitter and receiver, where only the spreading factor J is known from c(t).
It has to be investigated whether the lower BPSK model can also be used for PN modulation and whether the BPSK error probability
- p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt { {2 \cdot E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right )
is also valid for PN modulation, or how the given equation should be modified.
Notes:
- This exercise belongs to the chapter Direct-Sequence Spread Spectrum Modulation.
- For the solution of this exercise, the specification of the specific spreading sequence (M-sequence or Walsh function) is not important.
Questions
Solution
- We are dealing here with an optimal receiver.
- Without noise, the signal b(t) within each bit is constantly equal to +1 or -1.
- From the given equation for the integrator
- d (\nu T) = \frac{1}{T} \cdot \hspace{-0.1cm} \int_{(\nu -1 )T }^{\nu T} \hspace{-0.3cm} b (t )\hspace{0.1cm} {\rm d}t
- it follows that d(νT) can take only the values +1 and -1.
(2) Again the last solution is correct:
- In the noise– and interference-free case ⇒ n(t) = 0, the twofold multiplication by c(t) ∈ \{+1, –1\} can be omitted,
- so that the upper model is identical to the lower model.
(3) Solution 1 is correct:
- Since both models are identical in the noise-free case, only the noise signal has to be adjusted: n'(t) = n(t) · c(t).
- In contrast, the other two solutions are not applicable:
- The integration must still be done over T = J · T_c and the PN modulation does not reduce the AWGN noise.
(4) The last solution is correct:
- Multiplying the AWGN noise by the high-frequency ±1 signal c(t), the product is also Gaussian and white.
- Because of {\rm E}\big[c^2(t)\big] = 1, the noise variance is not changed either.
- Thus, the equation p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt {{2 E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right ) valid for BPSK is also applicable for PN modulation, independent of the spreading factor J and the specific spreading sequence.
- Ergo: For AWGN noise, band spreading neither increases nor decreases the error probability.