Signal Representation/Discrete-Time Signal Representation

1. Signal Representation
2. Time and Frequency-Discrete Signal Representation
3. Discrete-Time Signal Representation

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# OVERVIEW OF THE FIFTH MAIN CHAPTER #

A prerequisite for the system-theoretical investigation of digital systems or for their computer simulation is a suitable discrete-time signal description. 

This chapter clarifies the mathematical transition from time-continuous to time-discrete signals, starting from the  Fourier transform theorems.

The chapter includes in detail:

• the  "time and frequency domain representation"  of discrete-time signals,
• the  "sampling theorem", which must be strictly observed in time discretization,
• the  "reconstruction of the analog signal"  from the time-discrete representation,
• the  "Discrete Fourier Transform"  (DFT) and its inverse (IDFT),
• the  "possibilities for error"  when applying DFT and IDFT,
• the application of  "spectral analysis"  to the improvement of metrological procedures, and.
• the  "FFT algorithm"  particularly suitable for computer implementation.

Principle and motivation

Many source signals are analog and thus simultaneously  time-continuous  and  value-continuous.  If such an analog signal is to be transmitted by means of a digital system, the following preprocessing steps are required:

• the  $\text{sampling}$  of the source signal  $x(t)$, which is expediently - but not necessarily - performed at equidistant times   ⇒   $\text{time discretization}$,
• the  $\text{quantization}$  of the samples, so as to limit the number  $M$  of possible values to a finite value   ⇒   $\text{value discretization}$.

Quantization is not discussed in detail until the chapter  Pulse Code Modulation  of the book  "Modulation Methods".

On time discretization of the time-continuous signal  $x(t)$

In the following, we use the following nomenclature to describe the sampling:

• Let the continuous-time signal be  $x(t)$.
• Let the sampled signal sampled at equidistant intervals  $T_{\rm A}$  be  $x_{\rm A}(t)$.
• Let the run variable  $\nu$  of the sample be an  integer:

$$\nu \in \mathbb{Z} = \{\hspace{0.05cm} \text{...}\hspace{0.05cm} , –3, –2, –1, \hspace{0.2cm}0, +1, +2, +3, \text{...} \hspace{0.05cm}\} .$$

• Outside the sampling time points  $\nu \cdot T_{\rm A}$  always holds  $x_{\rm A}(t) = 0$.

• At the equidistant sampling times with the constant $K$, the result is:

$$x_{\rm A}(\nu \cdot T_{\rm A}) = K \cdot x(\nu \cdot T_{\rm A})\hspace{0.05cm}.$$

• $K$  depends on the time discretization type.  For the sketch:  $K = 1$.

Time domain representation

$\text{Definition:}$  Here,  $\text{"sampling"}$  shall be understood as the multiplication of the time-continuous signal  $x(t)$  by the  Dirac comb  $p_{\delta}(t)$:

$$x_{\rm A}(t) = x(t) \cdot p_{\delta}(t)\hspace{0.05cm}.$$

It should be noted that other description forms are found in the literature. However, to the authors, the form chosen here appears to be the most appropriate in terms of spectral representation and derivation of the  Discrete Fourier Transform  $\rm (DFT)$.

$\text{Definition:}$  The  $\text{Dirac comb}$  (in the time domain)  consists of infinitely many Dirac impulses, each equally spaced  $T_{\rm A}$  and all with equal impulse weight  $T_{\rm A}$:

$$p_{\delta}(t) = \sum_{\nu = - \infty }^{+\infty} T_{\rm A} \cdot \delta(t- \nu \cdot T_{\rm A} )\hspace{0.05cm}.$$

Sometimes  $p_{\delta}(t)$  is also called  "Dirac impulse train".

Based on this definition, the sampled signal  $x_{\rm A}(t)$  has the following properties:

• The sampled signal at the considered time  $(\nu \cdot T_{\rm A})$  is equal  $T_{\rm A} \cdot x(\nu \cdot T_{\rm A}) \cdot \delta (0)$.
• Since the Dirac function  $\delta (t)$  is infinite at time  $t = 0$  all signal values  $x_{\rm A}(\nu \cdot T_{\rm A})$  are also infinite.
• Thus, the factor  $K$  introduced on the last page is actually infinite as well.
• However, two samples  $x_{\rm A}(\nu_1 \cdot T_{\rm A})$  and  $x_{\rm A}(\nu_2 \cdot T_{\rm A})$  differ in the same proportion as the signal values  $x(\nu_1 \cdot T_{\rm A})$  and  $x(\nu_2 \cdot T_{\rm A})$.
• The samples of  $x(t)$  appear in the momentum weights of the Dirac functions:

$$x_{\rm A}(t) = \sum_{\nu = - \infty }^{+\infty} T_{\rm A} \cdot x(\nu \cdot T_{\rm A})\cdot \delta (t- \nu \cdot T_{\rm A} )\hspace{0.05cm}.$$

• The additional multiplication by  $T_{\rm A}$  is necessary so that  $x(t)$  and  $x_{\rm A}(t)$  have the same unit.  Note here that  $\delta (t)$  itself has the unit "1/s".

The following pages will show that these equations, which take some getting used to, do lead to reasonable results, if they are applied consistently.

Dirac comb in time and frequency domain

$\text{Theorem:}$  Developing the  $\text{Dirac comb}$  into a  Fourier series  and transforming it into the frequency domain using the  Shift Theorem  gives the following Fourier correspondence:

$$p_{\delta}(t) = \sum_{\nu = - \infty }^{+\infty} T_{\rm A} \cdot \delta(t- \nu \cdot T_{\rm A} )\hspace{0.2cm}\circ\!\!-\!\!\!-\!\!\!-\!\!\bullet\, \hspace{0.2cm} P_{\delta}(f) = \sum_{\mu = - \infty }^{+\infty} \delta (f- \mu \cdot f_{\rm A} ).$$

Here  $f_{\rm A} = 1/T_{\rm A}$  gives the distance between two adjacent Dirac lines in the frequency domain.

$\text{Proof:}$  The derivation of the spectral function  $P_{\delta}(f)$  given here is done in several steps:

(1)   Since  $p_{\delta}(t)$  is periodic with the constant distance  $T_{\rm A}$  between two Dirac lines, the  complex Fourier series  can be applied:

$$p_{\delta}(t) = \sum_{\mu = - \infty }^{+\infty} D_{\mu} \cdot {\rm e}^{\hspace{0.05cm}{\rm j} \hspace{0.05cm} \cdot 2 \hspace{0.05cm} \pi \hspace{0.05cm}\cdot \hspace{0.05cm}\mu \hspace{0.05cm}\cdot \hspace{0.05cm}t/T_{\rm A} } \hspace{0.3cm}{\rm mit}\hspace{0.3cm} D_{\mu} = \frac{1}{T_{\rm A} } \cdot \int_{-T_{\rm A}/2 }^{+T_{\rm A}/2}p_{\delta}(t) \cdot {\rm e}^{- {\rm j} \hspace{0.05cm}\cdot \hspace{0.05cm} 2 \pi \hspace{0.05cm}\cdot \hspace{0.05cm}\mu \hspace{0.05cm} \cdot \hspace{0.05cm}t/T_{\rm A} }\hspace{0.1cm} {\rm d}t\hspace{0.05cm}.$$

(2)   In the range from  $-T_{\rm A}/2$  to  $+T_{\rm A}/2$  holds for the Dirac comb in the time domain:   $p_{\delta}(t) = T_{\rm A} \cdot \delta(t)$.  Thus one can write for the complex Fourier coefficients:  

$$D_{\mu} = \int_{-T_{\rm A}/2 }^{+T_{\rm A}/2}{\delta}(t) \cdot {\rm e}^{- {\rm j} \hspace{0.05cm}\cdot \hspace{0.05cm} 2 \pi \hspace{0.05cm}\cdot \hspace{0.05cm}\mu \hspace{0.05cm} \cdot \hspace{0.05cm}t/T_{\rm A} }\hspace{0.1cm} {\rm d}t\hspace{0.05cm}.$$

(3)   Considering that for  $t \neq 0$  the Dirac impulse is zero and for  $t = 0$  the complex rotation factor is equal to  $1$, it holds further:

$$D_{\mu} = \int_{- T_{\rm A}/2 }^{+T_{\rm A}/2}{\delta}(t) \hspace{0.1cm} {\rm d}t = 1\hspace{0.5cm}{\Rightarrow}\hspace{0.5cm} p_{\delta}(t) = \sum_{\mu = - \infty }^{+\infty} {\rm e}^{ {\rm j} \hspace{0.05cm} \cdot 2 \hspace{0.05cm} \pi \cdot \hspace{0.05cm}\mu \hspace{0.05cm}\cdot \hspace{0.05cm}t/T_{\rm A} }\hspace{0.05cm}. $$

(4)   The   Shifting Theorem in the frequency domain  with  $f_{\rm A} = 1/T_{\rm A}$:

$${\rm e}^{ {\rm j} \hspace{0.05cm} \hspace{0.05cm} \cdot 2 \hspace{0.05cm} \pi \hspace{0.05cm}\cdot \hspace{0.05cm}\mu \hspace{0.05cm}\cdot \hspace{0.05cm} f_{\rm A}\hspace{0.05cm}\cdot \hspace{0.05cm}t}\hspace{0.2cm}\circ\!\!-\!\!\!-\!\!\!-\!\!\bullet\, \hspace{0.2cm} \delta (f- \mu \cdot f_{\rm A} )\hspace{0.05cm}.$$

(5)   If you apply this result to each individual summand, you finally get:

$$P_{\delta}(f) = \sum_{\mu = - \infty }^{+\infty} \delta (f- \mu \cdot f_{\rm A} )\hspace{0.05cm}.$$

q.e.d.

The result states:

• The Dirac comb  $p_{\delta}(t)$  in the time domain consists of infinitely many Dirac impulses, each at the same distance  $T_{\rm A}$  and all with the same impulse weight  $T_{\rm A}$.
• The Fourier transform of  $p_{\delta}(t)$  gives again a Dirac comb, but now in the frequency range   ⇒   $P_{\delta}(f)$.
• $P_{\delta}(f)$  also consists of infinitely many Dirac impulses, but now in the respective distance  $f_{\rm A} = 1/T_{\rm A}$  and all with impulse weights  $1$.
• The distances of the Dirac lines in the time and frequency domain representation thus follow the  Reciprocity Theorem:  

$$T_{\rm A} \cdot f_{\rm A} = 1 \hspace{0.05cm}.$$

Dirac comb in the time- and frequency domain

$\text{Example 1:}$  The graph illustrates the above statements for

• $T_{\rm A} = 50\,{\rm µs}$,
• $f_{\rm A} = 1/T_{\rm A} = 20\,\text{kHz}$ .

One can also see from this sketch the different impulse weights of  $p_{\delta}(t)$  and  $P_{\delta}(f)$.

Frequency domain representation

The spectrum of the sampled signal  $x_{\rm A}(t)$  is obtained by applying the  convolution theorem in the frequency domain.This states that multiplication in the time domain corresponds to convolution in the spectral domain:

$$x_{\rm A}(t) = x(t) \cdot p_{\delta}(t)\hspace{0.2cm}\circ\!\!-\!\!\!-\!\!\!-\!\!\bullet\, \hspace{0.2cm} X_{\rm A}(f) = X(f) \star P_{\delta}(f)\hspace{0.05cm}.$$

From the spectrum  $X(f)$  by convolution with the diracline shifted by  $\mu \cdot f_{\rm A}$  we get:

$$X(f) \star \delta (f- \mu \cdot f_{\rm A} )= X (f- \mu \cdot f_{\rm A} )\hspace{0.05cm}.$$

Applying this result to all diraclines of the Dirac pulse, we finally obtain:

$$X_{\rm A}(f) = X(f) \star \sum_{\mu = - \infty }^{+\infty} \delta (f- \mu \cdot f_{\rm A} ) = \sum_{\mu = - \infty }^{+\infty} X (f- \mu \cdot f_{\rm A} )\hspace{0.05cm}.$$

The sampling of the analogue time signal  $x(t)$  at equidistant intervals  $T_{\rm A}$  leads in the spectral domain to a  periodic continuation  of  $X(f)$  with frequency spacing of   $f_{\rm A} = 1/T_{\rm A}$.

$\text{Example 2:}$  The upper graph shows  (schematically!)  the spectrum  $X(f)$  of an analogue signal  $x(t)$, which includes frequencies up to  $5 \text{ kHz}$ .

Spectrum of the Sampled Signal

Sampling the signal at the sampling rate  $f_{\rm A}\,\text{ = 20 kHz}$, i.e. at the respective distance  $T_{\rm A}\, = {\rm 50 \, µs}$  we obtain the periodic spectrum  $X_{\rm A}(f)$ sketched below.

• Since the Dirac functions are infinitely narrow, the sampled signal  $x_{\rm A}(t)$  also contains arbitrary high-frequency components.
• Accordingly, the spectral function  $X_{\rm A}(f)$  of the sampled signal is extended to infinity.

Signal reconstruction

Signal sampling is not an end in itself in a digital transmission system; it must be reversed at some point. Consider, for example, the following system:

Sampling and Reconstruction of a Signal

• The analogue signal  $x(t)$  with bandwidth  $B_{\rm NF}$  is sampled as described above.
• At the output of an ideal transmission system, the likewise time-discrete signal  $y_{\rm A}(t) = x_{\rm A}(t)$  is present.
• The question now is how the block  signal reconstruction  is to be designed so that also  $y(t) = x(t)$  applies.

The solution is relatively simple if one considers the spectral functions:   One obtains from  $Y_{\rm A}(f)$  the spectrum  $Y(f) = X(f)$  by a low-pass with the  Frequency Response  $H(f)$, which 

Frequency Domain Representation of the Signal Reconstruction Process

• passes the low frequencies unaltered:

$$H(f) = 1 \hspace{0.3cm}{\rm{f\ddot{u}r}} \hspace{0.3cm} |f| \le B_{\rm NF}\hspace{0.05cm},$$

• suppresses the high frequencies completely:

$$H(f) = 0 \hspace{0.3cm}{\rm{f\ddot{u}r}} \hspace{0.3cm} |f| \ge f_{\rm A} - B_{\rm NF}\hspace{0.05cm}.$$

Further it can be seen from the graph that the frequency response  $H(f)$  in the range of  $B_{\rm NF}$  to  $f_{\rm A}-B_{\rm NF}$  can be arbitrarily shaped,

• for example, linearly sloping (dashed line)
• or also rectangular,

as long as both of the above conditions are met.

Sampling theorem

The complete reconstruction of the analogue signal  $y(t)$  from the sampled signal  $y_{\rm A}(t) = x_{\rm A}(t)$  is only possible if the sampling rate  $f_{\rm A}$  corresponding to the bandwidth  $B_{\rm NF}$  of the message signal has been chosen correctly.

From the graph of the  last page , it can be seen that the following condition must be fulfilled:

$$f_{\rm A} - B_{\rm NF} > B_{\rm NF} \hspace{0.3cm}\Rightarrow \hspace{0.3cm}f_{\rm A} > 2 \cdot B_{\rm NF}\hspace{0.05cm}.$$

$\text{Sampling Theorem:}$  If an analogue signal  $x(t)$  has spectral components in the range  $\vert f \vert < B_{\rm NF}$, it can only be completely reconstructed from its sampled signal if the sampling rate is sufficiently large:

$$f_{\rm A} ≥ 2 \cdot B_{\rm NF}.$$

Accordingly, the following must apply to the distance between two samples:

$$T_{\rm A} \le \frac{1}{ 2 \cdot B_{\rm NF} }\hspace{0.05cm}.$$

If the largest possible value   ⇒   $T_{\rm A} = 1/(2B_{\rm NF})$  is used for sampling,

• then, in order to reconstruct the analogue signal from its sampled values,
• one must use an ideal, rectangular low-pass filter with cut-off frequency  $f_{\rm G} = f_{\rm A}/2 = 1/(2T_{\rm A})$ .

$\text{Example 3:}$  The graph above shows the spectrum  $\pm\text{ 5 kHz}$  of an analogue signal limited to  $X(f)$  below the spectrum  $X_{\rm A}(f)$  of the signal sampled at distance  $T_{\rm A} =\,\text{ 100 µs}$  ⇒   $f_{\rm A}=\,\text{ 10 kHz}$.

Sampling Theorem in the Frequency Domain

Additionally drawn is the frequency response  $H(f)$  of the low-pass filter for signal reconstruction, whose cut-off frequency must be   $f_{\rm G} = f_{\rm A}/2 = 5\,\text{ kHz}$ .

• With any other  $f_{\rm G}$ value, the result would be  $Y(f) \neq X(f)$.
• For  $f_{\rm G} < 5\,\text{ kHz}$  the upper  $X(f)$ portions are missing.
• At  $f_{\rm G} > 5\,\text{ kHz}$  there are unwanted spectral components in  $Y(f)$ due to convolution operations.

If the sampling at the transmitter had been done with a sampling rate  $f_{\rm A} < 10\,\text{ kHz}$    ⇒   $T_{\rm A} >100 \,{\rm µ s}$, the analogue signal  $y(t) = x(t)$  would not be reconstructible from the samples  $y_{\rm A}(t)$  in any case.

Note:   There is an interactive applet on the topic covered here:   Sampling of Analogue Signals and Signal Reconstruction

Exercises For the Chapter

Exercise 5.1: Sampling Theorem

Exercise 5.1Z: Sampling of Harmonic Oscillations