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Signals and Spectra

The document covers key concepts in signals and spectra within communication systems, including sinusoidal signals, phasor representation, and Fourier series. It discusses power calculations, decibel measurements, and the power spectral density (PSD) for both deterministic and periodic waveforms. Additionally, it addresses signal transmission through linear systems and various definitions of bandwidth.

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0% found this document useful (0 votes)
24 views9 pages

Signals and Spectra

The document covers key concepts in signals and spectra within communication systems, including sinusoidal signals, phasor representation, and Fourier series. It discusses power calculations, decibel measurements, and the power spectral density (PSD) for both deterministic and periodic waveforms. Additionally, it addresses signal transmission through linear systems and various definitions of bandwidth.

Uploaded by

tai.diep21
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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Signals and Spectra

Chapter 2: Signals and Spectra


in Communication Systems  A generic sinusoidal
signal
v(t )  A cos(0t   ); 0  2f 0
 Phasor representation

January 2024
Lectured by Prof. Dr. Thuong Le-Tien  Frequency domain
representation

Amplitude
 Rotating phasors A
 Frequency plots f0
Slides with references from HUT Finland, La Hore uni.,  Amplitude A f0 f
Mc. Graw Hill Co., A.B. Carlson’s “Communication  Phase 0t   

Phase
Systems”, and Leon W.Couch “Digital and Analog
Communication Systems” books f0 f
1 2

 Two sided spectra can be seen from


Periodic Signals
 This represents two rotating phasors
 Amplitude and phase spectrum (two sided)  A signal x p(t ) is periodic if there exists T
such that x p(t) = x p(t + T)
 Smallest such T is called fundamental
period T0
 Any integer multiple of T0 is also a period

T0

3 4
Normalized Power
Average signal and Power  In the concept of normalized power, R is
assumed to be 1Ω, although it may be another
 Average signal value in the actual circuit.
 Another way of expressing this concept is to say
that the power is given on a per-ohm basis.
 It can also be realized that the square root of the
normalized power is the rms value.
 For periodic signals
Definition. The average normalized power is given by:
Where s(t) is the voltage or current waveform
 Average power T /2
1
P  s (t )  lim 
2
s 2 (t )dt
T  T
T / 2
5 6

Decibel Decibel Gain


 A base 10 logarithmic measure of power ratios.
 The ratio of the power level at the output of a circuit
compared with that at the input is often specified by
 If resistive loads are involved,
the decibel gain instead of the actual ratio.
 Decibel measure can be defined in 3 ways
 Decibel Gain
 Decibel signal-to-noise ratio (SNR in dB) Definition of dB may be reduced to,
 Mili-watt Decibel or dBm
 Definition: Decibel Gain
The decibel gain of a circuit is:
or

7 8
Decibel signal-to-noise ratio (SNR) Decibel with mili watt reference (dBm)
 Definition. The decibel power level with respect to 1 mW
 Definition. The decibel signal-to-noise ratio
(SNR) is:

= 30 + 10 log (Actual Power Level (watts)


Where, Signal Power (S) =  Here the “m” in the dBm denotes a milliwatt reference.
 When a 1-W reference level is used, the decibel level is
denoted dBW;
And, Noise Power (N) =  when a 1-kW reference level is used, the decibel level
is denoted dBk.
E.g.: If an antenna receives a signal power of 0.3W, what is the
received power level in dBm?
dBm = 30 + 10xlog(0.3) = 30 + 10x(-0.523)3 = 24.77 dBm

9 10

Fourier Series
Fourier Series Representation
 Projection of periodic signals onto basis
functions
 Periodic signal is a weighted sum of these basis
functions
 Exponentials are used as basis functions for DC component:
writing Fourier series
Any periodic signal can be expressed as a
1
 f0= T0 (fundamental frequency)
sum of infinite number of exponentials (or Line spectra at frequencies that are integer
sinusoids for real signals) multiple of fundamental frequency

11 12
Fourier series example: Fourier Series: Example

13 14

Three major properties of V(f)

Fourier Transform
 Back to the Fourier series:

15 16
Rectangular pulse spectrum
V(ƒ) = A sinc ƒ

17 18

Convolution
 The convolution of a waveform w1(t) with a waveform
w2(t) to produce a third waveform w3(t) which is

Evaluation of the integral involves 3 steps.


• Time reversal of w2 to obtain w2(-λ),
• Time shifting of w2 by t seconds to obtain w2(-(λ-t)),
and
• Multiplying this result by w1 to form the integrand
w1(λ)w2(-(λ-t)).

Note: we denote a signal s(t) as a waveform w(t)


19 20
Example for Convolution Power Spectral Density (PSD)
 T 
t 2   We define the truncated version of the waveform by:
w1 (t )    
 T 
 
t
-
w 2 (t)=e T u (t )

For 0< t < T • The average normalized power:

For t > T
• Using Parseval’s theorem to calculate power from the
frequency domain

21 22

Autocorrelation Function
 Definition: The Power Spectral Density (PSD) for a  Definition: The autocorrelation of a real (physical)
deterministic power waveform is waveform is

• Wiener-Khintchine Theorem: PSD and the autocorrelation function are Fourier


• where wT(t) ↔ WT(f) and Pw(f) has units of watts per hertz. transform pairs;

• The PSD is always a real nonnegative function of frequency.


The PSD can be evaluated by either of the following two methods:
• PSD is not sensitive to the phase spectrum of w(t) 1. Direct method: by using the definition,
• The normalized average power is 2. Indirect method: by first evaluating the autocorrelation function and
then taking the Fourier transform:

Pw(f)= ℑ [Rw(τ) ]
• This means the area under the PSD function is the normalized
• The average power can be obtained by any of the four techniques.
average power.

23 24
Normalized Power Power Spectral Density for Periodic Waveforms
Theorem: For a periodic waveform, the power spectral
Theorem: For a periodic waveform w(t), the
density (PSD) is given by
normalized power is given by:

where T0 = 1/f0 is the period of the waveform and


where the {cn} are the complex Fourier coefficients for the waveform. {cn} are the corresponding Fourier coefficients for the waveform.

Proof: For periodic w(t), the Fourier series representation is valid over all time
and one may evaluate the normalized power:

PSD is the FT of the


Autocorrelation
function

25 26

Power Spectral Density for a Square Wave Noise in communication systems


• The PSD for the periodic square wave will be found.  Thermal noise is described by a zero-mean Gaussian random
• Because the waveform is periodic, FS coefficients can be used to process, n(t).
evaluate the PSD. Consequently this problem becomes one of  Its PSD is flat, hence, it is called white noise.
evaluating the FS coefficients.
[w/Hz]

Power spectral
density

Autocorrelation
function

Probability density function

27 28
Signal transmission through linear systems  Ideal filters:

Input Output
Non-causal!
Linear system Low-pass

 Deterministic signals:
 Random signals:
Band-pass High-pass

 Ideal distortion less transmission:

All the frequency components of the signal not


 Realizable filters:
only arrive with an identical time delay, but also
RC filters Butterworth filter
are amplified or attenuated equally.

29 30

Bandwidth of signal Bandwidth of signal …


 Different definition of bandwidth:
 Baseband versus bandpass: a) Half-power bandwidth a) Fractional power containment bandwidth
b) Noise equivalent bandwidth b) Bounded power spectral density
Baseband Bandpass c) Null-to-null bandwidth c) Absolute bandwidth
signal signal
Local oscillator

(a)
 Bandwidth dilemma: (b)
 Bandlimited signals are not realizable! (c)
(d)
 Realizable signals have infinite bandwidth!
(e)50dB
31 32
Power Transfer Function
 Derive the relationship between the power spectral density
(PSD) at the input, Px(f), and that at the output, Py(f) , of a linear
time-invariant network.
Using the definition of PSD

PSD of the output is

Using transfer function


in a formal sense, we obtain

Thus, the power transfer


function of the network is

33

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