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From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1
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From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Dec 17, 2015

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Page 1: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

From Continuous Time System to Discrete Time System

ES400Jack Ou, Ph.D.

Chapter 1

Page 2: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Outline

• Modeling –Signal–System

• Continuous Time System• ADC• Discrete Time System

Page 3: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Signals

• Signals are divided into two natural categories–Continuous time signal: Discrete

time signal: defined at only defined for all values of time–Discrete Time Signal: Only defined

at certain instants of time.

Page 4: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Example of a Continuous Time Signal

Criterion: The signal defined for all values of timeTechniques: Fourier series, Fourier transform, Laplace transform

Page 5: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Example of a Discrete Time Signal

Criterion: The signal is defined for at only certain instants of time Technique: Z transform, DFT, FFT

Page 6: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Tinkering

Page 7: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Mathematical Modeling of a Physical System

Page 8: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Mathematical Solutions of Physical Problems

1. Formulate a math model for physical signal and system involved.2. Equations are solved for typical excitation function. 3. Compare math solution with the response of the physical system4. Iterate the process until close correlation between the measuredand model is achieved.

Page 9: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Continuous Time Example

Page 10: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Mathematical Modeling of Elementary Circuits

Page 11: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Use KVL to formulate the mathematical representation of a physical system

• KVL: The algebraic sum of Voltages around any closed loop in an electric circuit is zero.

Page 12: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Describe the input signal mathematically

Page 13: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Represent Input Voltage Source using Laplace Transform

Page 14: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Solve the problem in the Laplace Domain

• Laplace transform the KVL expression

• Solve the variable of interest• Inverse Laplace Transform

Page 15: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Not All Systems Can Be Represented Using a Continuous Time Representation

Page 16: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Convert a Signal From Continuous Time System to Discrete Time System

• Operational Amplifier• Digital to Analog Converter• Comparator• Counter-Ramp Analog to Digital

Converter

Page 17: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Operational Amplifier

If used in a feedback configuration, V+=V-.

Large input impedance!

Page 18: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

A Simple Voltage Amplifier

Page 19: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Digital-to-analog Converter

Purpose: Convert a binary number to a voltage.

Page 20: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

A Simple Digital to Analog Converter

Assume “1”=5V, “0”=0VD0=“1”, D1=“0”, D2=“0”What is Vout?

Page 21: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Comparator

If Vi>Vr, then Vo=“1”Else zero.

Page 22: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

A Simple Op-Amp Based Comparator

Page 23: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

A Analog-to-digital Converter

(Inverter)

(NAND)

EOC: End of ConversionA binary output approximately equal to Vx will be when EOC=1

Page 24: From Continuous Time System to Discrete Time System ES400 Jack Ou, Ph.D. Chapter 1.

Sampling in Telephone Systems