Title: Lecture 2 Probability Review and Random Process
1Lecture 2Probability Review and Random Process
2Review of last lecture
- The point worth noting are
- The source coding algorithm plays an important
role in higher code rate (compressing data) - The channel encoder introduce redundancy in data
- The modulation scheme plays important role in
deciding the data rate and immunity of signal
towards the errors introduced by the channel - Channel can introduce many types of errors due to
thermal noise etc. - The demodulator and decoder should provide high
Bit Error Rate (BER).
3ReviewLayering of Source Coding
- Source coding includes
- Sampling
- Quantization
- Symbols to bits
- Compression
- Decoding includes
- Decompression
- Bits to symbols
- Symbols to sequence of numbers
- Sequence to waveform (Reconstruction)
4ReviewLayering of Source Coding
5ReviewLayering of Channel Coding
- Channel Coding is divided into
- Discrete encoder\Decoder
- Used to correct channel Errors
- Modulation\Demodulation
- Used to map bits to waveform for transmission
6ReviewLayering of Channel Coding
7ReviewResources of a Communication System
- Transmitted Power
- Average power of the transmitted signal
- Bandwidth (spectrum)
- Band of frequencies allocated for the signal
- Type of Communication system
- Power limited System
- Space communication links
- Band limited Systems
- Telephone systems
8ReviewDigital communication system
- Important features of a DCS
- Transmitter sends a waveform from a finite set of
possible waveforms during a limited time - Channel distorts, attenuates the transmitted
signal and adds noise to it. - Receiver decides which waveform was transmitted
from the noisy received signal - Probability of erroneous decision is an important
measure for the system performance
9Review of Probability
10Sample Space and Probability
- Random experiment its outcome, for some reason,
cannot be predicted with certainty. - Examples throwing a die, flipping a coin and
drawing a card from a deck. - Sample space the set of all possible outcomes,
denoted by S. Outcomes are denoted by Es and
each E lies in S, i.e., E ? S. - A sample space can be discrete or continuous.
- Events are subsets of the sample space for which
measures of their occurrences, called
probabilities, can be defined or determined.
11Three Axioms of Probability
- For a discrete sample space S, define a
probability measure P on as a set function that
assigns nonnegative values to all events, denoted
by E, in such that the following conditions are
satisfied - Axiom 1 0 P(E) 1 for all E ? S
- Axiom 2 P(S) 1 (when an experiment is
conducted there has to be an outcome). - Axiom 3 For mutually exclusive events E1, E2,
E3,. . . we have
12Conditional Probability
- We observe or are told that event E1 has occurred
but are actually interested in event E2
Knowledge that of E1 has occurred changes the
probability of E2 occurring. - If it was P(E2) before, it now becomes P(E2E1),
the probability of E2 occurring given that event
E1 has occurred. - This conditional probability is given by
- If P(E2E1) P(E2), or P(E2 n E1) P(E1)P(E2),
then E1 and E2 are said to be statistically
independent. - Bayes rule
- P(E2E1) P(E1E2)P(E2)/P(E1)
13Mathematical Model for Signals
- Mathematical models for representing signals
- Deterministic
- Stochastic
- Deterministic signal No uncertainty with respect
to the signal value at any time. - Deterministic signals or waveforms are modeled by
explicit mathematical expressions, such as - x(t) 5 cos(10t).
- Inappropriate for real-world problems???
- Stochastic/Random signal Some degree of
uncertainty in signal values before it actually
occurs. - For a random waveform it is not possible to write
such an explicit expression. - Random waveform/ random process, may exhibit
certain regularities that can be described in
terms of probabilities and statistical averages. - e.g. thermal noise in electronic circuits due to
the random movement of electrons
14Energy and Power Signals
- The performance of a communication system depends
on the received signal energy higher energy
signals are detected more reliably (with fewer
errors) than are lower energy signals. - An electrical signal can be represented as a
voltage v(t) or a current i(t) with instantaneous
power p(t) across a resistor defined by - OR
15Energy and Power Signals
- In communication systems, power is often
normalized by assuming R to be 1. - The normalization convention allows us to express
the instantaneous power as - where x(t) is either a voltage or a current
signal. - The energy dissipated during the time interval
(-T/2, T/2) by a real signal with instantaneous
power expressed by Equation (1.4) can then be
written as - The average power dissipated by the signal during
the interval is
16Energy and Power Signals
- We classify x(t) as an energy signal if, and only
if, it has nonzero but finite energy (0 lt Ex lt 8)
for all time, where - An energy signal has finite energy but zero
average power - Signals that are both deterministic and
non-periodic are termed as Energy Signals
17Energy and Power Signals
- Power is the rate at which the energy is
delivered - We classify x(t) as an power signal if, and only
if, it has nonzero but finite energy (0 lt Px lt 8)
for all time, where - A power signal has finite power but infinite
energy - Signals that are random or periodic termed as
Power Signals
18Random Variable
- Functions whose domain is a sample space and
whose range is a some set of real numbers is
called random variables. - Type of RVs
- Discrete
- E.g. outcomes of flipping a coin etc
- Continuous
- E.g. amplitude of a noise voltage at a particular
instant of time
19Random Variables
- Random Variables
- All useful signals are random, i.e. the receiver
does not know a priori what wave form is going to
be sent by the transmitter - Let a random variable X(A) represent the
functional relationship between a random event A
and a real number. - The distribution function Fx(x) of the random
variable X is given by
20Random Variable
- A random variable is a mapping from the sample
space to the set of real numbers. - We shall denote random variables by boldface,
i.e., x, y, etc., while individual or specific
values of the mapping x are denoted by x(w).
21Random process
- A random process is a collection of time
functions, or signals, corresponding to various
outcomes of a random experiment. For each
outcome, there exists a deterministic function,
which is called a sample function or a
realization.
Random variables
Sample functions or realizations (deterministic
function)
22Random Process
- A mapping from a sample space to a set of time
functions.
23Random Process contd
- Ensemble The set of possible time functions that
one sees. - Denote this set by x(t), where the time functions
x1(t, w1), x2(t, w2), x3(t, w3), . . . are
specific members of the ensemble. - At any time instant, t tk, we have random
variable x(tk). - At any two time instants, say t1 and t2, we have
two different random variables x(t1) and x(t2). - Any realationship b/w any two random variables is
called Joint PDF
24Classification of Random Processes
- Based on whether its statistics change with time
the process is non-stationary or stationary. - Different levels of stationary
- Strictly stationary the joint pdf of any order
is independent of a shift in time. - Nth-order stationary the joint pdf does not
depend on the time shift, but depends on time
spacing
25Cumulative Distribution Function (cdf)
- cdf gives a complete description of the random
variable. It is defined as - FX(x) P(E ? S X(E) x) P(X x).
- The cdf has the following properties
- 0 FX(x) 1 (this follows from Axiom 1 of the
probability measure). - Fx(x) is non-decreasing Fx(x1) Fx(x2) if x1
x2 (this is because event x(E) x1 is contained
in event x(E) x2). - Fx(-8) 0 and Fx(8) 1 (x(E) -8 is the empty
set, hence an impossible event, while x(E) 8 is
the whole sample space, i.e., a certain event). - P(a lt x b) Fx(b) - Fx(a).
26Probability Density Function
- The pdf is defined as the derivative of the cdf
- fx(x) d/dx Fx(x)
- It follows that
- Note that, for all i, one has pi 0 and ?pi 1.
27Cumulative Joint PDF Joint PDF
- Often encountered when dealing with combined
experiments or repeated trials of a single
experiment. - Multiple random variables are basically
multidimensional functions defined on a sample
space of a combined experiment. - Experiment 1
- S1 x1, x2, ,xm
- Experiment 2
- S2 y1, y2 , , yn
- If we take any one element from S1 and S2
- 0 lt P(xi, yj) lt 1 (Joint Probability of two or
more outcomes) - Marginal probabilty distributions
- Sum all j P(xi, yj) P(xi)
- Sum all i P(xi, yj) P(yi)
28Expectation of Random Variables(Statistical
averages)
- Statistical averages, or moments, play an
important role in the characterization of the
random variable. - The first moment of the probability distribution
of a random variable X is called mean value mx or
expected value of a random variable X - The second moment of a probability distribution
is mean-square value of X - Central moments are the moments of the difference
between X and mx, and second central moment is
the variance of x. - Variance is equal to the difference between the
mean-square value and the square of the mean
29Contd
- The variance provides a measure of the variables
randomness. - The mean and variance of a random variable give a
partial description of its pdf.
30Time Averaging and Ergodicity
- A process where any member of the ensemble
exhibits the same statistical behavior as that of
the whole ensemble. - For an ergodic process To measure various
statistical averages, it is sufficient to look at
only one realization of the process and find the
corresponding time average. - For a process to be ergodic it must be
stationary. The converse is not true.
31Gaussian (or Normal) Random Variable (Process)
- A continuous random variable whose pdf is
- µ and are parameters. Usually denoted as
- N(µ, ) .
- Most important and frequently encountered random
variable in communications.
32Central Limit Theorem
- CLT provides justification for using Gaussian
Process as a model based if - The random variables are statistically
independent - The random variables have probability with same
mean and variance
33CLT
- The central limit theorem states that
- The probability distribution of Vn approaches a
normalized Gaussian Distribution N(0, 1) in the
limit as the number of random variables approach
infinity - At times when N is finite it may provide a poor
approximation of for the actual probability
distribution
34Autocorrelation
- Autocorrelation of Energy Signals
- Correlation is a matching process
autocorrelation refers to the matching of a
signal with a delayed version of itself - The autocorrelation function of a real-valued
energy signal x(t) is defined as - The autocorrelation function Rx(?) provides a
measure of how closely the signal matches a copy
of itself as the copy is shifted ? units in time. - Rx(?) is not a function of time it is only a
function of the time difference ? between the
waveform and its shifted copy.
35Autocorrelation
- symmetrical in ? about zero
- maximum value occurs at the origin
- autocorrelation and ESD form a Fourier transform
pair, as designated by the double-headed arrows - value at the origin is equal to the energy of the
signal
36AUTOCORRELATION OF A PERIODIC (POWER) SIGNAL
- The autocorrelation function of a real-valued
power signal x(t) is defined as - When the power signal x(t) is periodic with
period T0, the autocorrelation function can be
expressed as
37Autocorrelation of power signals
The autocorrelation function of a real-valued
periodic signal has properties similar to those
of an energy signal
- symmetrical in ? about zero
- maximum value occurs at the origin
- autocorrelation and PSD form a Fourier transform
pair, as designated by the double-headed arrows - value at the origin is equal to the average power
of the signal
38(No Transcript)
39(No Transcript)
40Spectral Density
41SPECTRAL DENSITY
- The spectral density of a signal characterizes
the distribution of the signals energy or power,
in the frequency domain - This concept is particularly important when
considering filtering in communication systems
while evaluating the signal and noise at the
filter output. - The energy spectral density (ESD) or the power
spectral density (PSD) is used in the evaluation. - Need to determine how the average power or energy
of the process is distributed in frequency.
42Spectral Density
- Taking the Fourier transform of the random
process does not work
43ENERGY SPECTRAL DENSITY
- Energy spectral density describes the energy per
unit bandwidth measured in joules/hertz - Represented as ?x(t), the squared magnitude
spectrum - ?x(t) x(f)2
- According to Parsevals Relation
- Therefore
- The Energy spectral density is symmetrical in
frequency about origin and total energy of the
signal x(t) can be expressed as
44Power Spectral Density
- The power spectral density (PSD) function Gx(f)
of the periodic signal x(t) is a real, even ad
nonnegative function of frequency that gives the
distribution of the power of x(t) in the
frequency domain. - PSD is represented as (Fourier Series)
- PSD of non-periodic signals
- Whereas the average power of a periodic signal
x(t) is represented as
45Noise
46Noise in the Communication System
- The term noise refers to unwanted electrical
signals that are always present in electrical
systems e.g. spark-plug ignition noise,
switching transients and other electro-magnetic
signals or atmosphere the sun and other galactic
sources - Can describe thermal noise as zero-mean Gaussian
random process - A Gaussian process n(t) is a random function
whose value n at any arbitrary time t is
statistically characterized by the Gaussian
probability density function
47WHITE NOISE
- The primary spectral characteristic of thermal
noise is that its power spectral density is the
same for all frequencies of interest in most
communication systems - A thermal noise source emanates an equal amount
of noise power per unit bandwidth at all
frequenciesfrom dc to about 1012 Hz. - Power spectral density G(f)
- Autocorrelation function of white noise is
- The average power P of white noise if infinite
48White Noise
49White Noise
- Since Rw( T) 0 for T 0, any two different
samples of white noise, no matter how close in
time they are taken, are uncorrelated. - Since the noise samples of white noise are
uncorrelated, if the noise is both white and
Gaussian (for example, thermal noise) then the
noise samples are also independent.
50Additive White Gaussian Noise (AWGN)
- The effect on the detection process of a channel
with Additive White Gaussian Noise (AWGN) is that
the noise affects each transmitted symbol
independently - Such a channel is called a memoryless channel
- The term additive means that the noise is
simply superimposed or added to the signalthat
there are no multiplicative mechanisms at work
51Random Processes and Linear Systems
- If a random process forms the input to a
time-invariant linear system, the output will
also be a random process
52Distortion less Transmission
- Remember linear and non-linear group delays in
DSP
53DISTORTION LESS TRANSMISSION
- What is required of a network for it to behave
like an ideal transmission line? - The output signal from an ideal transmission line
may have some time delay and different amplitude
as compared with the input - It must have no distortionit must have the same
shape as the input - For idea distortion less transmission
54Ideal Distortion Less Transmission
- The overall system response must have a constant
magnitude response - The phase shift must be linear with frequency
- All of the signals frequency components must
also arrive with identical time delay in order to
add up correctly - The time delay t0 is related to the phase shift
and the radian frequency ? 2?f by - A characteristic often used to measure delay
distortion of a signal is called envelope delay
or group delay, which is defined as
55BANDWIDTH OF DIGITAL DATA
- Baseband signals
- Signals containing frequencies ranging from 0 to
some frequency fs - Bandpass or Passband Signals
- Signals containing frequencies ranging from fs1
to some frequency fs2
56Note
- Chapters/Topics from different books
- Topics to be covered on your own
- Chapter 1 from Bernard Sklar
- Chapter 1 from Simon Haykin
- Appendix 1 from Digital Communication, Simon
Haykin for Probability
- Periodic, Non-periodic Signals
- Analog and Digital Signals
- Ideal Filters
- Realizable filters
57References
- Bernard Sklar
- University of Saskatchewan
- Communication System, Simon Haykin
- MIT open source lectures (Robert Gallager)