General Description

From LNTwww


In this chapter  periodic signals  are considered and described mathematically in the time and frequency domain.

This chapter contains in detail:

  • Some basic terms like  "period duration", "basic frequency"  and  "circular frequency",
  • the properties of a  "DC signal"  as a boundary case of a periodic signal,
  • the definition and interpretation of the  "Dirac function",
  • the spectral representation of a DC signal or a DC signal component,
  • the time and frequency representation of  "harmonic oscillations", and finally
  • the application of  "Fourier series"  for spectral analysis of periodic signals.

Features and applications

Periodic signals are of great importance for communications engineering:

  • They belong to the class of deterministic signals, whose time function can be specified in analytical form.
  • Their signal path is thus known for all times  $t$  and can be clearly predicted for the future.
  • They are therefore never information-carrying signals.

Nevertheless, periodic signals are often also required in communications engineering, for example

  • for modulation and demodulation in carrier frequency systems,
  • for synchronization and clock regeneration in digital systems,
  • as test and verification signals during system implementation.

Oscilloscope image of cosine and triangular signals

$\text{Example 1:}$  The oscilloscope image shows two typical representatives of periodic signals:

  • above a cosine signal,
  • below a triangular signal.

As can be seen from the displayed settings, the period duration of both signals is one millisecond and the amplitude one volt.

Definition and parameters

Before we turn to the signal parameters of a periodic signal, the term  "periodicity"  shall be clearly defined:

$\text{Definition:}$  A  $\text{periodic signal}$  $x(t)$  is present if for all arbitrary values of  $t$  and all integer values of  $i$  with an appropriate  $T_{0}$  applies:

$$x(t+i\cdot T_{0}) = x(t).$$

This results in the following parameters:

  • The  $\text{period duration}$  $T_{0}$  indicates the smallest possible value, which satisfies the above equation.
  • The  $\text{basic frequency}$  $f_{0} = 1/T_{0}$  describes the number of periods per time unit (mostly per second).
  • The unit  "1/s"  is also called  "Hz", named after the German physicist   Heinrich Hertz.
  • The  $\text{basic circular frequency}$  $\omega_{0}$  represents the angular rotation per second, usually given in radians.
  • In contrast to the basic frequency, the unit  "Hz"  is not common here, but  "1/s".  The following equation applies:
$$\omega_{0}=2\pi f_{0} = {2\pi}/{T_{0}}.$$

Given signal and period duration

$\text{Example 2:}$  Here, a periodic time signal is shown:

  • The period duration is  $T_{0} = 2.5 \ \rm ms$.
  • From this the basic frequency   $f_0 = 400 \ \rm Hz$ is calculated.
  • The basic circular frequency results to  $\omega_{0}=2513 \ \rm 1/s.$

Resulting period duration

If a signal  $x(t)$  consists of the sum of two periodic signals  $x_{1}(t)$  and  $x_{2}(t)$  with the period durations  $T_{1}$  or   $T_{2}$, the resulting period duration of the sum signal is the smallest common multiple of  $T_{1}$  and  $T_{2}$.

  • This statement applies independently of the amplitude and phase relations.
  • On the other hand, if   $T_{1}$  and  $T_{2}$  don't have a rational common multiple  $($Example:   $T_{2} = \pi \cdot T_{1})$,
    then the sum signal  $x(t)$  is in contrast to its two components  $x_{1}(t)$  and  $x_{2}(t)$  not periodic.

$\text{Example 3:}$  Here, a cosinusoidal signal  $x_{1}(t)$  with period duration  $T_{1} = 2\; {\rm ms}$  (blue signal course) is added with a sinusoidal signal  $x_{2}(t)$  with period duration  $T_{2} = 5\; {\rm ms}$  and twice the amplitude (green curve).

Resulting period duration of the sum of cosine and sine signal
  • The (red) sum signal  $x(t) = x_{1}(t) + x_{2}(t)$  then shows the resulting period duration  $T_{0} = 10\; {\rm ms}$   ⇒   basic frequency  $f_{0} = 100\; {\rm Hz}$.
  • The frequency  $f_{0}$  itself is not contained in  $x(t)$  only integer multiples of it, namely 
$f_{1} = 500\; {\rm Hz}$  and  $f_{2} = 200\; {\rm Hz}$.

With the interactive applet  Period Duration of Periodic Signals  the resulting period of two harmonic oscillations can be determined.

Exercises for the chapter

Exercise 2.1: Rectification

Exercise 2.1Z: Sum Signal