Continuous-time Signals. (AKA analog signals)

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Continuous-time Signals (AKA analog signals)

I. Analog* Signals review Goals: - Common test signals used in system analysis - Signal operations and properties: scaling, shifting, periodicity, energy and power *Analog = the argument t (time) of the signal g(t) is continuous (CT). Also known as CT signals.

The Unit Step function u( t) =! 1, t > 0 # " 1 / 2, t = 0 # $ 0, t < 0 Precise Graph Commonly-Used Graph Note: The signal is discontinuous at zero but is an analog signal Note: The product signal g(t)u(t) for any g(t) can be thought of as the signal g(t) turned on at time t = 0. Used to check how a system responds to a sudden input

The Signum Function sgn( t) = " 1, t > 0& $ $ # 0, t = 0 ' $ % 1, t < 0 $ ( = 2u( t) 1 Precise Graph Commonly-Used Graph

rect ( t) = The Unit Rectangle function! 1, t < 1 / 2 % # # " 1 / 2, t = 1 / 2& # $ 0, t > 1 / 2 # ' = u( t +1 / 2) u( t 1 / 2) The product g(t)rect(t) can be understood as the signal turned on at and turned off at t = 1 2 t = 1 2 5

The Unit Ramp function ramp t " ( ) = t, t > 0 t % # & = u( λ)dλ $ 0, t 0 = t u t ' ( ) The Unit Ramp function is unbounded with time

Unit Triangle function tri t # ( ) = 1 t, t < 1 ' $ ( %& 0, t 1)& The triangle signal is related to the rectangle through an operation called convolution (to be introduced later ) 7

The Impulse function The impulse function is not a function in the ordinary sense because its value at zero is not a real value δ(0) =, δ(t) = 0, t 0 It is represented by a vertical arrow The impulse function is unbounded and discontinuous

Creating an Impulse An impulse can be defined as the limit of the rectangle function with unit area as a goes to zero " δ a ( t) = # 1 / a, t < a / 2 $% 0, t > a / 2 Other approximations are possible for example, we can use a triangle function

The Unit Sinc function The unit sinc function is related to the unit rectangle function through the Fourier Transform sinc( t) = sin ( πt ) πt It is used for noise removal in signals lim sinc t t 0 ( ) = lim t 0 d dt ( sin ( πt) ) d ( dt πt) = lim π cos ( πt ) t 0 π = 1

Real exponentials red blue black e 0.5t e t e 2t red blue black e 0.5t e t e 2t

Sinusoids (and Cosinusoids) red blue black red black sin(5t) sin(3t) sin(7t) sin(5t) cos(5t) for cos(ωt + θ) = cos(2πft + θ) radian frequency: (rad/s) cyclic frequency: f (cycles/s) wavelength or period: 1/ f amplitude: phase: θ 1 ω

Real and complex sinusoids Recall that a complex number is defined as (here and ) Re(z) = a Im(z) = b j = 1 z = a + jb A complex sinusoid is expressed as A graphical example for ω = 2π : e jωt = cos(ωt) + j sin(ωt) Relation between complex and real sinusoids: cos(ωt) = e jωt + e jωt 2 sin(ωt) = e jωt e jωt 2 j

Goals: Analog signals review - Common test signals used in system analysis - Signal operations and properties: shifting, scaling, periodicity, energy and power 14

Signal operations: shifting and scaling Amplitude scaling g( t) Ag( t) Expansion/contraction of signal along Y axis Rotation about X axis for negative A

Signal operations: shifting and scaling Time shifting Time shifting t t t 0

Signal operations: shifting and scaling Time scaling t t / a Expansion/contraction of signal along X axis Rotation about Y axis for negative a

Example: Doppler effect Sound heard by firefighters: g(t) Sound we hear when truck comes: A(t) g(at), A increasing, a>1 Sound we hear when truck goes: B(t) g(bt), B decreasing, b<1 Checkout the website: http://www.lon-capa.org/~mmp/applist/doppler/d.htm

Signal operations: shifting and scaling A signal may be expressed by means of basic test signals that have been time-scaled and amplified

Signal operations: shifting and scaling Caution! The impulse satisfies special properties Time-scaling property Sampling property δ ( a( t t 0 )) = 1 a δ ( t t 0 ) g( t)δ ( t t 0 )dt = g t 0 ( ) The impulse function is not a function in the ordinary sense

Signal properties: periodic signals Periodic signals repeat x(t + kt ) = x(t) Cycle time is the period T Here about 1 second 2 seconds is also a period We only need define the signal over one period and we know everything about it Sinusoids and constant are clearly periodic signals Other examples include periodic pulses (rectangular and triangular pulses)

Signal properties: periodic signals The sum of two periodic signals x(t) = x 1 (t) + x 2 (t) T 1 T 2 with periods and is: T 1 T 1 = a 1 T 2 = a 2 - periodic when is rational. If, T 2 b 1 then the period is T = LCM(a 1,a 2 ) GCD(b 1,b 2 ) b 2 - not periodic when is irrational T 1 T 2

Signal energy and power Quantifying the size of a signal is important in many applications: How much electricity can be used in a defibrillator? How much energy should an audio signal have to be heard? The energy of the signal x(t) is E x = x t ( ) 2 dt

Signal energy and power Some signals have infinite energy. In that case, we may use the concept of average signal power For a periodic signal, x(t), with period T, the average signal power is P x = 1 T T x( t) 2 dt If the signal is not periodic, then 1 P x = lim T T T /2 T /2 x( t) 2 dt

We have seen: Analog signals summary -Signals can be seen as inputs/outputs to systems -Analog signals can be represented as functions of continuous time -The unit step, impulse, ramp and rectangle functions are examples of test signals to systems -A general signal can be expressed as a combination of some basic test signals by using scaling/shifting operations -Properties of signals include periodicity, even/odd, continuity, differentiability, etc -Power and energy are concepts that measure signal size