Difference between revisions of "Aufgaben:Exercise 3.7Z: Rectangular Signal with Echo"
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'''(1)''' The <u>second suggested solution</u> is correct: | '''(1)''' The <u>second suggested solution</u> is correct: | ||
− | *The impulse response is equal to the received signal r(t), if a single Dirac | + | *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). | ||
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_.