Difference between revisions of "Aufgaben:Exercise 3.7Z: Rectangular Signal with Echo"
m (Oezdemir moved page Aufgabe 3.7Z: Rechtecksignal mit Echo to Exercise 3.7Z: Square Wave With Echo) |
m (Text replacement - "Dirac impulse" to "Dirac delta") |
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− | [[File:EN_Sig_Z_3_7.png|right|frame| | + | [[File:EN_Sig_Z_3_7.png|right|frame|Transmission signal s(t), and <br>reception signal r(t) with echo]] |
− | + | We consider a periodic rectangular signal s(t) with the possible amplitude values 0 V and 2 V and the period duration T0=T=1 ms. At the jump points, e.g. at t=T/4, the signal value are 1 V. The DC component (i.e. the Fourier coefficient A0) of the signal is 1 V, too. | |
− | + | Further applies: | |
− | * | + | * Due to symmetry (even function), all sine coefficients Bn=0. |
− | * | + | * The coefficients An with even n are also zero. |
− | * | + | * For odd values of n, the following applies: |
:An=(−1)(n−1)/2⋅4Vn⋅π. | :An=(−1)(n−1)/2⋅4Vn⋅π. | ||
− | + | The signal s(t) reaches the receiver via two paths (see sketch below): | |
− | * | + | *Once on the direct path and secondly via a secondary path. |
− | * | + | *The latter is characterised by the attenuation factor α and the transit time τ . |
− | * | + | *Therefore, the following applies to the received signal: |
:r(t)=s(t)+α⋅s(t−τ). | :r(t)=s(t)+α⋅s(t−τ). | ||
− | + | The frequency response of the channel is H(f)=R(f)/S(f), the impulse response is denoted by h(t) . | |
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− | '' | + | ''Hints:'' |
− | * | + | *This exercise belongs to the chapter [[Signal_Representation/The_Convolution_Theorem_and_Operation|The Convolution Theorem and Operation]]. |
− | * | + | *Important information can be found on the page [[Signal_Representation/The_Convolution_Theorem_and_Operation#Convolution_of_a_function_with_a_Dirac_function|Convolution of a function with a Dirac function]]. |
− | === | + | ===Questions=== |
<quiz display=simple> | <quiz display=simple> | ||
− | { | + | {Which statements are true regarding the impulse response h(t)? |
|type="[]"} | |type="[]"} | ||
− | - | + | - For 0≤t<τ holds h(t)=1, and for t>τ holds h(t)=1+α. |
− | + | + | + It holds that h(t)=δ(t)+α⋅δ(t−τ). |
− | - h(t) | + | - h(t) has a Gaussian shape. |
− | { | + | {Calculate the reception signal r(t) for the channel parameters α=−0.5 and τ=T/4. <br>What values result at the given times? |
|type="{}"} | |type="{}"} | ||
r(t=0.2⋅T) = { 1 3% } V | r(t=0.2⋅T) = { 1 3% } V | ||
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− | { | + | {Calculate the reception signal r(t) with α=1 and τ=T/2. Interpret the result in the frequency domain. <br>What value results for t=T/2? |
|type="{}"} | |type="{}"} | ||
r(t=T/2) = { 2 3% } V | r(t=T/2) = { 2 3% } V | ||
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</quiz> | </quiz> | ||
− | === | + | ===Solution=== |
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' | + | '''(1)''' The <u>second suggested solution</u> is correct: |
− | * | + | *The impulse response is equal to the received signal r(t), if a single Dirac delta is present at the input at time t=0 : |
:h(t)=δ(t)+α⋅δ(t−τ). | :h(t)=δ(t)+α⋅δ(t−τ). | ||
− | [[File:P_ID532__Sig_Z_3_7_b_neu.png|right|frame| | + | [[File:P_ID532__Sig_Z_3_7_b_neu.png|right|frame|Convolution of square wave signal s(t) and impulse response h(t)]] |
− | '''(2)''' | + | '''(2)''' It holds r(t)=s(t)∗h(t). This convolution operation is most easily performed graphically: |
− | + | The values of the received signal are generally: | |
* 0.00<t/T<0.25:r(t)=+1 V, | * 0.00<t/T<0.25:r(t)=+1 V, | ||
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− | + | The values we are looking for are thus | |
:r(t=0.2⋅T)=+1 V_, | :r(t=0.2⋅T)=+1 V_, | ||
:r(t=0.3·T)=−1 V_. | :r(t=0.3·T)=−1 V_. | ||
− | '''(3)''' | + | '''(3)''' Using a similar procedure as in '''(2)''', a direct signal $\rm (DC)$ of $2\hspace{0.02cm}\text{ V} is obtained for r(t)$ : |
− | * | + | *The gaps in the signal s(t) are completely filled by the echo s(t−T/2). |
− | * | + | *This result can also be derived in the frequency domain. The channel frequency response is with α=1 and τ=T/2: |
− | |||
:H(f)=1+1⋅e−jπfT=1+cos(πfT)−j⋅sin(πfT). | :H(f)=1+1⋅e−jπfT=1+cos(πfT)−j⋅sin(πfT). | ||
− | * | + | *Apart from the DC component, the input signal s(t) only has components at f=f0=1/T, f=3⋅f0, f=5⋅f0, etc.. |
− | * | + | *At these frequencies, however, both the real– and the imaginary part of H(f) are equal to zero. |
− | * | + | *Thus, for the output spectrum with A0=1 V and H(f=0)=2 we obtain: |
:R(f)=A0⋅H(f=0)⋅δ(f)=2V⋅δ(f). | :R(f)=A0⋅H(f=0)⋅δ(f)=2V⋅δ(f). | ||
− | + | The inverse Fourier transformation thus also yields r(t)=2 V= const_. | |
{{ML-Fuß}} | {{ML-Fuß}} | ||
__NOEDITSECTION__ | __NOEDITSECTION__ | ||
− | [[Category: | + | [[Category:Signal Representation: Exercises|^3.4 The Convolution Theorem^]] |
Latest revision as of 09:05, 26 May 2021
We consider a periodic rectangular signal s(t) with the possible amplitude values 0 V and 2 V and the period duration T0=T=1 ms. At the jump points, e.g. at t=T/4, the signal value are 1 V. The DC component (i.e. the Fourier coefficient A0) of the signal is 1 V, too.
Further applies:
- Due to symmetry (even function), all sine coefficients Bn=0.
- The coefficients An with even n are also zero.
- For odd values of n, the following applies:
- An=(−1)(n−1)/2⋅4Vn⋅π.
The signal s(t) reaches the receiver via two paths (see sketch below):
- Once on the direct path and secondly via a secondary path.
- The latter is characterised by the attenuation factor α and the transit time τ .
- Therefore, the following applies to the received signal:
- r(t)=s(t)+α⋅s(t−τ).
The frequency response of the channel is H(f)=R(f)/S(f), the impulse response is denoted by h(t) .
Hints:
- This exercise belongs to the chapter The Convolution Theorem and Operation.
- Important information can be found on the page Convolution of a function with a Dirac function.
Questions
Solution
- The impulse response is equal to the received signal r(t), if a single Dirac delta is present at the input at time t=0 :
- h(t)=δ(t)+α⋅δ(t−τ).
(2) It holds r(t)=s(t)∗h(t). This convolution operation is most easily performed graphically:
The values of the received signal are generally:
- 0.00<t/T<0.25:r(t)=+1 V,
- 0.25<t/T<0.50:r(t)=−1 V,
- 0.50<t/T<0.75:r(t)=0 V,
- 0.75<t/T<1.00:r(t)=+2 V.
The values we are looking for are thus
- r(t=0.2⋅T)=+1 V_,
- r(t=0.3·T)=−1 V_.
(3) Using a similar procedure as in (2), a direct signal (DC) of 2 V is obtained for r(t) :
- The gaps in the signal s(t) are completely filled by the echo s(t−T/2).
- This result can also be derived in the frequency domain. The channel frequency response is with α=1 and τ=T/2:
- H(f)=1+1⋅e−jπfT=1+cos(πfT)−j⋅sin(πfT).
- Apart from the DC component, the input signal s(t) only has components at f=f0=1/T, f=3⋅f0, f=5⋅f0, etc..
- At these frequencies, however, both the real– and the imaginary part of H(f) are equal to zero.
- Thus, for the output spectrum with A0=1 V and H(f=0)=2 we obtain:
- R(f)=A0⋅H(f=0)⋅δ(f)=2V⋅δ(f).
The inverse Fourier transformation thus also yields r(t)=2 V= const_.