ECE 1100: Introduction to Electrical and Computer Engineering Sinusoidal Signals Waves t v(t)v(t) Wanda Wosik Associate Professor, ECE Dept. Spring 2011.

Slides:



Advertisements
Similar presentations
Electromagnetic Waves (Optional Unit)
Advertisements

Prof. Ji Chen Notes 15 Plane Waves ECE Spring 2014 z x E ocean.
PH0101 UNIT 2 LECTURE 31 PH0101 Unit 2 Lecture 3  Maxwell’s equations in free space  Plane electromagnetic wave equation  Characteristic impedance 
Maxwell’s Equations and Electromagnetic Waves
Chapter 22 Electromagnetic Waves. Units of Chapter 22 Changing Electric Fields Produce Magnetic Fields; Maxwell’s Equations Production of Electromagnetic.
My Chapter 22 Lecture.
Module 1-1 Continued Nature and Properties of Light.
Technician License Course Chapter 2 Lesson Plan Module 2 – Radio Waves & Signals.
Light as a Wave: Part 1 SNC2D. What is a wave? A wave is a disturbance which carries energy from one location to another. The material the disturbance.
ECE 4321 Computer Networks Chapter 4 Transmission Media: Wireless.
Physics 1402: Lecture 26 Today’s Agenda Announcements: Midterm 2: NOT Nov. 6 –About Monday Nov. 16 … Homework 07: due Friday this weekHomework 07: due.
3.1 Chapter 3 Data and Signals Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Antennas. Free Charge  A free charge has a constant electric field and no magnetic field.  No waves are produced. No radiationNo radiation  A charge.
08/28/2013PHY Lecture 011 Light is electromagnetic radiation! = Electric Field = Magnetic Field Assume linear, isotropic, homogeneous media.
Basic radio frequency communications - 1 Session 1.
- sound in air - AC electricity in a wire -an earthquake in rock -ocean waves in water radio waves - light - infrared radiation - X-rays - gamma rays -microwaves.
AERIALS AND RADIO FREQUENCY PROPAGATION By Farhan Saeed.
ECE 1100: Introduction to Electrical and Computer Engineering Notes 23 Power in AC Circuits and RMS Spring 2008 David R. Jackson Professor, ECE Dept.
Waves.
Energy and Waves.
Dr. Jie ZouPHY Chapter 25 Electromagnetic Waves.
Electromagnetism. Last Time Electromagnetic induction: The process by which current is generated by moving a conductor through a magnetic field or a magnetic.
Chapter 34 Electromagnetic Waves. Currents produce B Change in E produces B Currents produce B Change in E produces B Change in B produces an E charges.
Lecture 38: FRI 24 APR Ch.33 Electromagnetic Waves Heinrich Hertz (1857–1894) Physics 2113 Jonathan Dowling.
ECE 1100: Introduction to Electrical and Computer Engineering David R. Jackson Professor, ECE Dept. Notes 12 Antennas Spring 2008.
Electromagnetic Waves Chapter 35. Electromagnetic (EM) Waves Can travel through space Radio, Microwaves, IR, Light, UV, X-rays, Gamma Rays All on the.
Year 10 Physics Rotation Version What are waves? A wave is a means of transferring energy and momentum from one point to another without there being.
Chapter 4 Electromagnetic Waves. 1. Introduction: Maxwell’s equations  Electricity and magnetism were originally thought to be unrelated  in 1865, James.
4.4.1Describe a wave pulse and a continuous progressive (traveling) wave State that progressive (traveling) waves transfer energy Describe.
WAVES Wave motion allows a transfer of energy without a transfer of matter.
UPenn NROTC Unit, dtd Fall 2004 Naval Weapons Systems Energy Fundamentals.
ECE 1100: Introduction to Electrical and Computer Engineering Notes 11 Crystal Radio Principles Spring 2011 Wanda Wosik Associate Professor, ECE Dept.
ECE 3317 Prof. David R. Jackson Notes 15 Plane Waves [Chapter 3]
Electromagnetic Waves and Their Propagation Through the Atmosphere
ECE 1100: Introduction to Electrical and Computer Engineering Notes 10 Antennas Transmission and Reception of waves Wanda Wosik Associate Professor, ECE.
ECE 1100: Introduction to Electrical and Computer Engineering David R. Jackson Professor, ECE Dept. Spring 2008 Notes 9 Sinusoidal Signals t v(t)v(t)
Physics 1202: Lecture 18 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, etc.
Waves Basics. Expectations Upon completion of this unit you will be able to: Define waves and wave pulses. Identify the two types of wave pulses. Define.
Polarization of Light.
Copyright © 2009 Pearson Education, Inc. Energy in EM Waves: The Poynting Vector.
Waves and Sound Chapter The Nature of Waves A Wave: 1.Traveling disturbance 2.Carries energy from place to place Two Different Types: 1.Transverse.
What is a wave? Wave – a disturbance or oscillation that travels from one place to another.
Fundamentals of Transmission channels
Physics 102: Lecture 14, Slide 1 Electromagnetic Waves Physics 102: Lecture 14.
Wave Motion Types waves –mechanical waves require a medium to propagate –sound wave, water wave –electromagnetic waves not require a medium to propagate.
Lecture 37: FRI 19 NOV Ch.33 Electromagnetic Waves I Heinrich Hertz (1857–1894) Physics 2113 Jonathan Dowling.
Waves. What are waves? A wave is a transfer of energy from one place to another. Waves take many forms. Wave Characteristics include: –Amplitude –Wavelength.
General Physics 2Induction1 Introduction to Waves A wave is a disturbance that moves through a medium while the medium remains essentially at rest Examples.
Unit 12: Waves Waves.
17. Electromagnetic waves
Electromagnetic Waves
Unit 12: Waves Waves.
Waves Unit 8.
A.D.Patel institute of technology
Unit 11: Waves Waves.
EM Waves, & Their Speed Derived from Maxwell’s Equations
Electromagnetic waves
(Based on medium) 2. Mechanical Waves
Phys102 Lecture 20 Electromagnetic Waves * (skipped)
What are waves? A wave is a transfer of energy from one place to another. Waves take many forms. Wave Characteristics include: Amplitude Wavelength Frequency.
What we will do today: Carry out calculations involving the relationship between speed, wavelength and frequency for waves.
Waves & Sound Waves.
Unit 11: Waves Waves.
Light as a Wave: Part 1 SNC2D.
Waves.
Waves.
WAVES.
Lecture 33: FRI 03 APR Ch.33.1–3,5: E&M Waves
Electromagnetic Waves
TECHNICIAN BANDS RADIO AND SIGNAL FUNDAMENTALS
Presentation transcript:

ECE 1100: Introduction to Electrical and Computer Engineering Sinusoidal Signals Waves t v(t)v(t) Wanda Wosik Associate Professor, ECE Dept. Spring 2011 Slides developed by Dr. Jackson

Basic Facts Sinusoidal waveforms (waves that vary sinusoidally in time) are the most important types of waveforms encountered in physics and engineering.  Most natural sources of radiation (the sun, etc.) emit sinusoidal waveforms.  Most human-made systems produce sinusoidal waveforms (AC generators, microwave oscillators, etc.)  Most communications is done via sinusoidal waveforms that have been modulated, either in an analog fashion (such as AM or FM) or digitally.

General Sinusoidal Waveform A = amplitude of sinusoidal waveform  = “radian frequency” of sinusoidal waveform [radians/s]  = phase of sinusoidal signal [radians] t v (t)v (t) A -A 

Period of Sinusoidal Wave T = period (cycle) of wave [s] = time it takes for the waveform to repeat itself. In this example, T = 0.5 [ s ]. t [s] v (t)v (t) T

Frequency of Sinusoidal Wave f = frequency = # cycles (periods) / s Units: Hz = cycle/s In this example, f = 2 Hz f = 1/T [Hz] cycles/s = 1 / (s/cycle) t [s] v (t)v (t) [s] 1.5

Radian Frequency Since the cosine function repeats after 2 , we have t v (t)v (t) T  = 2  f [rad/s] Hence: or  Rotation with angular frequency 

Summary t v(t)v(t) A -A  = 2  f [rad/s] f = 1/T [Hz]

Waves Waves in nature (and engineering) are usually sinusoidal in shape, and they move outward from the source with a velocity.

Waves (cont.) We focus attention on a particular direction, called z. h (z) = height of wave at a fixed time t = 0. This is a “snapshot” of the wave at a fixed time t = 0. z

z [m] h (z)h (z) crest trough v = velocityWavenumber Assumed form of wave: k is “wavenumber” of wave. Wavelength z [m] h(z)h(z) The wavelength is the distance it takes for the waveform to repeat (for a fixed time).

Wave at Fixed Observation Point Next question: what is the velocity that the observer will feel? z [m] h (z)h (z) v = velocity observer zz Point on crest µ 0 =4  x10 -7 H/m  0 =8.85x F/m c=2.997x10 8 m/s v = velocity

Wave at Fixed Observation Point Next question: what would the height as a function of time look like, for an observer at a fixed value of z = z 0 ? z [m] h (z)h (z) v = velocity observer We can pretend that the wave is fixed and the observer is moving backwards at velocity v.

Wave at Fixed Observation Point (cont.) z [m] h (z)h (z) v = velocity observer

Wave at Fixed Observation Point (cont.) z [m] h (z)h (z) v = velocity observer

Define Wave at Fixed Observation Point (cont.) The observed amplitude varies sinusoidally in time!

General Form of Wave z [m] h (t, z)h (t, z) v = velocity Allowing for both t and z to be arbitrary, we have.

General Form of Wave (cont.) For the velocity we can also write

E H Electromagnetic Waves Wave propagation with speed of light c

Electromagnetic Wave There are two types of fields in nature: electric and magnetic. An electromagnetic wave has both fields, perpendicular to each other, and it travels (propagates) at the speed of light. You will learn much more about EM waves in ECE velocity = c (speed of light) The power flows in the direction E  H

Electromagnetic Wave (cont.) z c = speed of light electric field vector magnetic field vector The amplitudes of the electric and magnetic fields vary sinusoidal in space (just like the amplitude of a water wave).

Electromagnetic Wave (cont.) z earth x power flow ( z direction) The electric field vector is in the direction of the transmitting antenna.

Transmitting Antenna AM Radio: 550 kHz < f < 1610 kHz ExEx Electric field is vertically polarized z earth x

Transmitting Antenna (cont.) FM Radio: 88 MHz < f < 108 MHz Electric field is horizontally polarized z EyEy earth x VHF TV: MHz < f < 216 MHz UHF TV: 470 MHz < f < 806 MHz

Equation for Electric Field z c = speed of light electric field vector x Note: It is the electric field that would be received by a wire antenna.

Value of k From Maxwell’s equations, it can be shown that: (permeability of free space) (permittivity of free space)

Velocity of Wave (cont.) velocity = v = c =  /k Note: all frequencies travel the same speed. From previous notes on waves (propagation in vacuum): Hence we have c =  10 8 [m/s] (exact defined quantity)

Summary of Wave Formulas k = 2  / c = f c =  10 8 [m/s]  = ck  = 2  f [rad/s] f = 1/T [Hz] = m f m vacuum media vacuum  medium

Example KFCC 1270 AM (1270 [kHz]) Calculate all of the parameters and write down an expression for the electric field of this wave.