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Constellation diagram of a communication system is given.

enter image description here

enter image description here

S1(t) -> 0, S2(t) -> 1

Φ1 and Φ2 are basis functions and Tb is the bit period.

How can I draw S1(t),S2(t) and decision boundaries?

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  • \$\begingroup\$ This is not a homework, I'm just studying for an exam and I couldn't find how to do that. Any help is greatly appreciated. \$\endgroup\$
    – Jenny94
    Commented Jul 7, 2014 at 15:45
  • \$\begingroup\$ I think you mean "constellation" diagram. \$\endgroup\$ Commented Jul 7, 2014 at 16:10
  • \$\begingroup\$ What is \$r\$? Is that a typo, or a hint at the nature of \$\Phi_1\$? \$\endgroup\$ Commented Jul 7, 2014 at 16:40
  • \$\begingroup\$ @SimonRichter thank you, I fixed the typos and added some more information. \$\endgroup\$
    – Jenny94
    Commented Jul 7, 2014 at 16:57

1 Answer 1

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Let's see if I can guess how this is meant to be interpreted:

  1. We have two basis functions, giving us a two-dimensional space in which to align symbols.

  2. For successful decoding, the basis functions need to be at least linearly independent, and ideally, they should be orthogonal.

  3. Testing for orthogonality, we multiply and integrate:

    \$\int\Phi_1(t)\Phi_2(t)dt = 0\$

  4. Good thing that worked, otherwise we would have had to prove \$\nexists x | \Phi_1(t) = x\Phi_2(t)\$.

    For a two-basis system, that is somewhat sane, but with more basis functions, this starts to get really cumbersome. Fortunately, non-orthogonal systems are not that relevant in practice.

  5. The amplitude is written in a manner that I find to be completely non-intuitive. Someone more enlightened than me could possibly comment on how that is useful beyond hinting at #7 below.

  6. Constructing the time representation for each symbol is straightforward -- you multiply the symbol's constellation position with the basis function, and add these up (i.e. all you do here is a basis transformation of a vector):

    \$S_1(t) = (2V\sqrt{T_b})\Phi_1(t) + (-2V\sqrt{T_b})\Phi2(t)\$

  7. This system is equivalent to a Fourier transformation with two points. \$\Phi_1(t)\$ is the DC part, \$\Phi_2(t)\$ is the base frequency. Decoding this schema works likewise, by multiplying the basis function again, and correcting the linear amplification resulting from the integration (probably that's why the \$1/\sqrt{T_b}\$ is there).

    The difference with the square waves is that you need to reconstruct the timing, which I assume is pretty much a given in that hypothetical scenario. If you don't have the timing information, the multiplication and integration become a full convolution, and you have to find the middle of the symbol.

  8. The decision boundary would most likely be placed so that for each constellation point, the nearest valid symbol is selected. You have two valid symbols, so just draw a line in the middle between them.

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  • \$\begingroup\$ I'm trying hard to understand your answer. So is it possible to draw S1 and S2 in (0,Tb) range? \$\endgroup\$
    – Jenny94
    Commented Jul 7, 2014 at 20:23
  • \$\begingroup\$ @Jenny94, Simon's point 6 tells you how to do it. We can't go any further without knowing what \$\Phi_1(t)\$ and \$\Phi_2(t)\$ are. \$\endgroup\$
    – The Photon
    Commented Jul 7, 2014 at 20:27
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    \$\begingroup\$ The definition for \$\Phi_1(t)\$ is \$1/\sqrt{T_b}\$ for \$0 \leq t < T_b\$, and \$0\$ for all other \$t\$. If you multiply that by the symbol value on the \$Phi_1(t)\$ axis, you get \$2V\sqrt{T_b}/\sqrt{T_b}\$ for \$0 \leq t < T_b\$, and \$0\$ for all other \$t\$. The right hand side of the addition works exactly the same, except that there are two nonzero ranges, \$0 \leq t < T_b/2\$ and \$T_b/2 \leq t < T_b\$. \$\endgroup\$ Commented Jul 7, 2014 at 21:51
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    \$\begingroup\$ Φ2(t) is -1/√Tb for 0≤t<Tb/2 and 1/√Tb for Tb/2≤t<Tb, correct? \$\endgroup\$
    – Jenny94
    Commented Jul 7, 2014 at 22:29
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    \$\begingroup\$ Exactly. You will notice that the integral over the entire function \$\Phi_2(t)\$ is zero, which is the only way the orthogonality condition #3 holds. Using this condition, you can finally test your solution for correctness: \$\int S_1(t)\Phi_1(t) dt = 2V\sqrt{T_b}\$, which is exactly the coordinate of the \$S_1\$ symbol along the \$\Phi_1\$ axis. \$\endgroup\$ Commented Jul 7, 2014 at 22:39

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