Chapter 2 One Dimensional Continuous Time System.

Slides:



Advertisements
Similar presentations
Previous Lectures Source free RL and RC Circuits.
Advertisements

Differential Equations
Signals and Systems – Chapter 2
Lecture 7: Basis Functions & Fourier Series
Experiment 17 A Differentiator Circuit
Characteristics of a Linear System 2.7. Topics Memory Invertibility Inverse of a System Causality Stability Time Invariance Linearity.
ENTC 3320 Absolute Value.
Fundamentals of Electric Circuits Chapter 10 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Description of Systems M. J. Roberts - All Rights Reserved. Edited by Dr. Robert Akl 1.
A second order ordinary differential equation has the general form
2nd Order Circuits Lecture 16.
Lecture 181 Second-Order Circuits (6.3) Prof. Phillips April 7, 2003.
Feb 23, 2007 EEE393 Basic Electrical Engineering K.A.Peker Signals and Systems Introduction EEE393 Basic Electrical Engineering.
Measurements &Testing (1)a CSE 323a 1. Grading Scheme 50Semester work 50Lab exam 50Final exam 150Total Course webpage
ES250: Electrical Science
A Differentiator Circuit.  All of the diagrams use a uA741 op amp. ◦ You are to construct your circuits using an LM 356 op amp.  There is a statement.
Digital Signals and Systems
Overview of ENGR 220 Circuits 1 Fall 2005 Harding University Jonathan White.
Sinusoidal Steady-state Analysis Complex number reviews Phasors and ordinary differential equations Complete response and sinusoidal steady-state response.
ES250: Electrical Science
1 Chapter 1 Fundamental Concepts. 2 signalpattern of variation of a physical quantity,A signal is a pattern of variation of a physical quantity, often.
Differential Amplifier
Time Domain Representation of Linear Time Invariant (LTI).
Time-Domain Representations of LTI Systems
Dr. Hatim Dirar Department of Physics, College of Science Imam Mohamad Ibn Saud Islamic University.
CISE315 SaS, L171/16 Lecture 8: Basis Functions & Fourier Series 3. Basis functions: Concept of basis function. Fourier series representation of time functions.
Module 2 SPECTRAL ANALYSIS OF COMMUNICATION SIGNAL.
1 Chapter 1 Fundamental Concepts. 2 signalpattern of variation of a physical quantity,A signal is a pattern of variation of a physical quantity, often.
BYST CPE200 - W2003: LTI System 79 CPE200 Signals and Systems Chapter 2: Linear Time-Invariant Systems.
COSC 3451: Signals and Systems Instructor: Dr. Amir Asif
1 Lecture 1: February 20, 2007 Topic: 1. Discrete-Time Signals and Systems.
Week 6 Second Order Transient Response. Topics Second Order Definition Dampening Parallel LC Forced and homogeneous solutions.
Input Function x(t) Output Function y(t) T[ ]. Consider The following Input/Output relations.
Fundamentals of Electric Circuits Chapter 10 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
1 G. Baribaud/AB-BDI Digital Signal Processing March 2003 DISP-2003 The Laplace transform  The linear system concept  The definition and the properties.
Net work analysis Dr. Sumrit Hungsasutra Text : Basic Circuit Theory, Charles A. Desoer & Kuh, McGrawHill.
Signals and Systems 1 Lecture 7 Dr. Ali. A. Jalali September 4, 2002
Chapter 7 The Laplace Transform
EE 207 Dr. Adil Balghonaim Chapter 4 The Fourier Transform.
1 Chapter 3 Linear Ordinary Differential Equations in The Time Domain.
Signals and Systems Analysis NET 351 Instructor: Dr. Amer El-Khairy د. عامر الخيري.
Dr. Tamer Samy Gaafar Lec. 2 Transfer Functions & Block Diagrams.
1 Fourier Representation of Signals and LTI Systems. CHAPTER 3 UniMAP.
A sinusoidal current source (independent or dependent) produces a current That varies sinusoidally with time.
Series-Parallel Circuits. Most practical circuits have both series and parallel components. Components that are connected in series will share a common.
Eeng360 1 Chapter 2 Linear Systems Topics:  Review of Linear Systems Linear Time-Invariant Systems Impulse Response Transfer Functions Distortionless.
Description and Analysis of Systems Chapter 3. 03/06/06M. J. Roberts - All Rights Reserved2 Systems Systems have inputs and outputs Systems accept excitation.
Chapter 2. Signals and Linear Systems
Eeng Chapter4 Bandpass Signalling  Bandpass Filtering and Linear Distortion  Bandpass Sampling Theorem  Bandpass Dimensionality Theorem  Amplifiers.
Circuit Theorems 1.  Introduction  Linearity property  Superposition  Source transformations  Thevenin’s theorem  Norton’s theorem  Maximum power.
Math for CS Fourier Transforms
Eeng Chapter4 Bandpass Signalling  Bandpass Filtering and Linear Distortion  Bandpass Sampling Theorem  Bandpass Dimensionality Theorem  Amplifiers.
Chapter 2. Signals and Linear Systems
Absolute Value.
What is System? Systems process input signals to produce output signals A system is combination of elements that manipulates one or more signals to accomplish.
Automatic Control Theory CSE 322
Signal Processing First
Mathematical Modeling of Control Systems
Description and Analysis of Systems
Mathematical Descriptions of Systems
Chapter4 Bandpass Signalling Bandpass Filtering and Linear Distortion
Chapter 1 Fundamental Concepts
§1-2 State-Space Description
2. 2 The V-I Relationship for a Resistor Let the current through the resistor be a sinusoidal given as Is also sinusoidal with amplitude amplitude.
8.3 Frequency- Dependent Impedance
§1—2 State-Variable Description The concept of state
Chapter4 Bandpass Signalling Bandpass Filtering and Linear Distortion
Signals and Systems Lecture 2
Mathematical Models of Control Systems
SIGNALS & SYSTEMS (ENT 281)
Presentation transcript:

Chapter 2 One Dimensional Continuous Time System

2.2 One Dimensional Continuous Time System Definition 1: An one dimensional analog system or continuous time system can be defined as a mapping function T which maps a real-valued analog signal f(t) to another real-valued g(t) such that

T f(t)T[f(t)] input system output

Definition 2: The mapping T is linear if it satisfies the following equations T[af 1 (t) + bf 2 (t)] = aT[f 1 (t)] + bT[f 2 (t)] (additivity) T[af(t)] = aT[f(t)] (homogeneity) for any If a system is not linear it is called a nonlinear system.

Example 1: A multiplier system is defined as The multiplier is an amplifier that converts a very small audio signal into a large audio to drive the speaker. The multiplier is a transformer that convert a low voltage sinusoidal wave into a high voltage sinusoidal wave or vice versa.

Example 2: A differentiator is defined as

Example 3: An integrator is defined as

Example 4: A delay system is defined as where D > 0 is a time delay.

Example 5: The following square wave if with the period 2  can be approximated by

f N (t) is the superposition (linear combination) of sine waves. It is easy to know that

Figure2.1: (a) N = 1 (b) N=3 (c) N = 5 (d) N = 10 (e) N=50 (f) N = 100

Figure 2.1 shows f 1 (t), f 3 (t), f 5 (t), f10(t), f 50 (t) and f 100 (t). As N increase There are overshoot and undershoot also increases at t = 0. the following MATLAB program show the plot of f 100 (t)

% % f(wc) = -1, -pi < wc < 0 % = 1, 0 <= wc < pi wc = 0.5 * pi; ws = 0.01* pi;

N = pi /ws; Nc = wc/ws; f = zeros(1, 2*N-1); f(1:N-1) = -1 * ones(1,N-1); f(N:2*N-1) = ones(1, N);

Nop = 100; w = (-pi + ws) : ws : (pi -ws); s = zeros(size(w) ); for i = 1:1:Nop s = s + 2/pi * (1 - (-1)^i )/i * sin(i*w); end; plot(w, f, w,s);

Example 6: Figure 2.2(a) shows f(t) = cos(200  t) cos(1000  t)). It is easy to know that

Figure 2.2(b) shows the analog signal Obviously the differentiation system attenuates low frequency signal and magnifies high frequency. It is a high pass system.

Figure 2.2: (a) f(t) = cos(200  t) cos(1000  t) (b) (c) (a)(b)(c)

Figure 2.2(c) show the analog signal The integration system attenuates high frequency and magnifies low frequency. it is a low pass system. Also, if f(t) is processed by an integration system then

Example 7: A square system is defined as

Example 8: A exponential system is defined as

Example 9: A natural logarithm system is defined as

Definition 3: The system T is linear time- invariant if

Example 10: The system g(t)  g(t  D) = f(t) is a linear time invariant system. Let h ’ (t) = T(  (t  a), is the output when  (t  a) Thus,

Assume that the system is linear time invariant.It is known that the output of the system is the impulse response h(t) when the input is  (t). At time t  a if the input is f(t  a) =  (t  a) then the output is

From the above two equations we can easily obtain The equality holds if Therefore, the system is time invariant.

Example 11: The system g(t)  tg(t  D) = f(t) is a time varying system Let h ’ (t) be the output when the input applies to the system. Thus, At time t  a we obtain

Assume that the system is linear time invariant. It is known that the output of the system is the impulse response h(t) when the input is d(t  a). Therefore, From the two previous equations we can easily obtain which implies

Thus, If the system is time invariant which is contraction to Equation h(t  a  D) = 0, Therefore,and the impulse response of the system is time varying.

Theorem 1: If h(t) is the impulse response of a linear invariant system and f(t) is the input of the system then the output is

h(t) f(t)

Definition 4: A system T is called causal if its present output does not depend on its future input

Definition 5: A system T is call BIBO stable if its input and output is bounded. That is, if then

Theorem 2: If the impulse response h(t) of the system is absolute integrable the system is BIBO stable.

Assume that the input f(t) is bounded. There exist a real number M 1 such that Since h(t) is absolute integrable there exists a real number M 2 such that

Then, the absolute output is The output g(t) is bounded.

Example 12: A multiplier system is defined as where k is a constant and is called the gain of the system.The system is an all pass filter.

Example 13: A time delay system is defined as where T is called the delay time. It can be easily that the system is linear time invariant. The system is casual since the impulse response h(t) =  (t  T) = 0 for t < 0. The output depends on its past input but does not depends on the future input.

is linear time invariant. However, it is not causal because the current output g(t) depends on future input f(t + T). In fact, its impulse response for t < 0. Note that the system

Example 14: A differentiation system is defined as It is a high pass filter. If f(t) = e j  t then g(t) =j  e j  t. For small , |g(t)| is very small while for large , |g(t)| is very large. It is a high pass filer.

Example 15: An integration system is defined as It is a low pass filter. If For small , |g(t)| is very large while for large , |g(t)| is very small. It is a low pass filter. The integration filter is linear time invariant.

Example 16: A fall-wave rectifier is defined as

Example 17: A half-wave rectifier is defined as if otherwise. Both the full wave rectifier and the half wave rectifier are nonlinear system.

Definition 6: the modulation of a signal f(t) is defined as where m(t) is called the modulating signal.

2.3 Linear Differential Equations Definition 7: an ordinary differential equation is an equation that has derivatives with respect to an independent variable only. If the equations has the derivatives with respect to at least two variables it is called an partial differential equation.

Definition 8: The ordinary differential equation is a linear differential equation of order N. If a differential equation can not be written as above equation it is nonlinear.

ak(t) ak(t) equation is said to be non- homogeneous; other- wise it it said to be homogeneous. If the initial conditions are given the differential equation is called the initial-value problem. Each Coefficient depends on on the variable t. If the

In practical systems, is usually assumed to be constant so that the system is LTI.

Example 18: The following equations are ordinary differential equations.

Example 19: The following equations are partial differential equations

Example 21: The following ordinary differential equations are linear.

Example 22: The following ordinary differential equations are nonlinear.

R +- Voltage across the resistor

L +- Voltage across the inductor

C +- Voltage across the capacitor

The Kirchhoff’s Current Law The sum of the currents at a node in a circuit is zero.

The Kirchhoff’s Voltage Law The sum of the voltages around a loop in a circuit is zero.

= 0

Example 23: A R-L series circuit shown in Figure 2.5 R L V +  i(t)i(t) Figure 2.5: The R-L series circuit.

The current i(t) that satisfies where V(t) is the input voltage. It is a first order differential equation.

Example 24: Figure 2.6(a) show a circuit where R and C in series. R C V +  i(t)i(t) Figure 2.6(a): The R-C series circuit.

The current flows in the circuit is i(t). The voltage across the capacitor is and the voltage across the resistor is Ri(t). Thus, The equation can be also written as where q(t) is the charge across the capacitor.

Example 25: A series R-L-C circuit shown in Figure 2.7 R L V(t) i(t)i(t) Figure 2.7: A R-L-C series circuit. C q(t)q(t)

The input voltage V(t) satisfies where q(t) denotes the charge in the capacitor and i(t) denotes the current of the circuit. It is a linear second differential equation.

The R, L, and C values in the circuit can change with time. However, they are assumed to be constant for analysis.