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Exercise 4.1Z: Other Basis Functions

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Energy-limited signals

This exercise pursues exactly the same goal as  "Exercise 4.1":

For  M=4  energy-limited signals  si(t)  with  i=1, ... ,4,  the  N  required orthonormal basis functions  φj(t)  are to be found,  which must satisfy the following condition:

<φj(t),φk(t)> = +φj(t)φk(t)dt=δjk={10j=kjk.

With  M  transmitted signals  si(t),  already fewer basis functions  φj(t)  can suffice,  namely  N.  Thus,  in general,  NM.

These are exactly the same energy-limited signals  si(t)  as in  "Exercise 4.1":

  • The difference is the different order of the signals  si(t).
  • In this exercise,  these are sorted in such a way that the basis functions can be found without using the more cumbersome  "Gram-Schmidt process"



Notes:

  • For numerical calculations,  use:   A = 1 \sqrt{\rm W} , \hspace{0.2cm} T = 1\,{\rm µ s} \hspace{0.05cm}.


Questions

1

In Exercise 4.1,  the Gram-Schmidt process resulted in  N = 3  basis functions.  How many basis functions are needed here?

N \ = \

2

Give the 2–norm of all these signals:

||s_1(t)|| \ = \

\ \cdot \ 10^{\rm –3} \ \rm \sqrt{Ws}
||s_2(t)|| \ = \

\ \cdot \ 10^{\rm –3} \ \rm \sqrt{Ws}
||s_3(t)|| \ = \

\ \cdot \ 10^{\rm –3} \ \rm \sqrt{Ws}
||s_4(t)|| \ = \

\ \cdot \ 10^{\rm –3} \ \rm \sqrt{Ws}

3

Which statements are true for the basis functions  \varphi_1(t)\varphi_2(t)  and  \varphi_3(t)?

The basis functions computed in  "Exericse 4.1"  are also appropriate here.
There are infinitely many possibilities for  \{\varphi_1(t),\ \varphi_2(t),\ \varphi_3(t)\}.
A possible set is  \{\varphi_{\it j}(t)\} = \{s_{\it j}(t)\},  with  j = 1,\ 2,\ 3.
A possible set is  \{\varphi_{\it j}(t)\} = \{s_{\it j}(t)/K\},  with  j = 1,\ 2,\ 3.

4

What are the coefficients of the signal  s_4(t)  with respect to the basis functions  \{\varphi_{\it j}(t)\} = \{s_{\it j}(t)/K\}, with  j = 1,\ 2,\ 3?

s_{\rm 41} \ = \

\ \cdot \ 10^{\rm –3} \ \rm \sqrt{Ws}
s_{\rm 42} \ = \

\ \cdot \ 10^{\rm –3} \ \rm \sqrt{Ws}
s_{\rm 43} \ = \

\ \cdot \ 10^{\rm –3} \ \rm \sqrt{Ws}


Solution

(1)  The only difference to Exercise 4.1 is the different numbering of the signals s_i(t).

  • Thus it is obvious that \underline {N = 3} must hold here as well.


(2)  The 2–norm gives the root of the signal energy and is comparable to the rms value for power-limited signals.

  • The first three signals all have the 2–norm
||s_1(t)|| = ||s_2(t)|| = ||s_3(t)|| = \sqrt{A^2 \cdot T}\hspace{0.1cm}\hspace{0.15cm}\underline { = 10^{-3}\sqrt{\rm Ws}} \hspace{0.05cm}.
  • The norm of the last signal is larger by a factor of \sqrt{2}:
||s_4(t)|| \hspace{0.1cm}\hspace{0.15cm}\underline { = 1.414 \cdot 10^{-3}\sqrt{\rm Ws}} \hspace{0.05cm}.

Basisfunktionssatz (3)  The first and last statements are true in contrast to statements 2 and 3:

  • It would be completely illogical if the basis functions found should no longer hold when the signals s_i(t) are sorted differently.
  • The Gram–Schmidt process yields only one possible set \{\varphi_{\it j}(t)\} of basis functions. A different sorting (possibly) yields a different one.
  • The number of permutations of  M = 4  signals is  4! = 24. In any case, there cannot be more basis function sets   ⇒   solution 2 is wrong.
  • However, there are probably (because of N = 3) only 3! = 6 possible sets of basis functions. As can be seen from the sample "solution" to Exercise 4.1, the same basis functions will result with the order s_1(t), s_2(t), s_4(t), s_3(t) as with s_1(t), s_2(t), s_3(t), s_4(t). However, this is only a conjecture of the authors; we have not checked it.
  • Statement 3 cannot be true simply because of the different units of s_i(t) and \varphi_{\it j}(t). Like A, the signals have the unit \sqrt{\rm W}, the basis functions the unit \sqrt{\rm 1/s}.
  • Thus, the last solution is correct, where for K holds:
K = ||s_1(t)|| = ||s_2(t)|| = ||s_3(t)|| = 10^{-3}\sqrt{\rm Ws} \hspace{0.05cm}.

Ende Basisfunktionssatz

(4)  From the comparison of the diagrams in the specification section we can see:

s_{4}(t) = s_{1}(t) - s_{2}(t) = K \cdot \varphi_1(t) - K \cdot \varphi_2(t)\hspace{0.05cm}.
  • Furthermore holds:
s_{4}(t) = s_{41}\cdot \varphi_1(t) + s_{42}\cdot \varphi_2(t) + s_{43}\cdot \varphi_3(t)
\Rightarrow \hspace{0.3cm}s_{41} = K \hspace{0.1cm}\hspace{0.15cm}\underline {= 10^{-3}\sqrt{\rm Ws}}\hspace{0.05cm}, \hspace{0.2cm}s_{42} = -K \hspace{0.1cm}\hspace{0.15cm}\underline {= -10^{-3}\sqrt{\rm Ws}}\hspace{0.05cm}, \hspace{0.2cm}s_{43} \hspace{0.1cm}\hspace{0.15cm}\underline { = 0}\hspace{0.05cm}.