Chapter 2: Amplitude Modulation Transmission EET-223: RF - - PowerPoint PPT Presentation

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Chapter 2: Amplitude Modulation Transmission EET-223: RF - - PowerPoint PPT Presentation

Chapter 2: Amplitude Modulation Transmission EET-223: RF Communication Circuits Walter Lara Introduction As see before, modulation is needed to: Avoid interference since intelligence signals are at approximately the same frequency


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SLIDE 1

Chapter 2: Amplitude Modulation Transmission

EET-223: RF Communication Circuits Walter Lara

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SLIDE 2

Introduction

  • As see before, modulation is needed to:

– Avoid interference since intelligence signals are at approximately the same frequency – Avoid impractical large antennas since intelligence signals have low frequencies

  • Problem: how to put intelligence signal onto a

carrier (high frequency) signal for transmission

  • Simplest solution: put intelligence into carrier’s

amplitude

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SLIDE 3

AM Fundamentals

  • Combining (“mixing”) the intelligence and carrier

signals can be done:

– Using linear device (e.g. resistor) – simple addition, but not suitable for transmission (receiver cannot detect intelligence) – Non-linear device (e.g., BJT or OpAmp) – method used in practice

  • Non-linear mixing results on:

– DC Component – Components at original frequencies (intelligence & carrier) – Components at sum & difference of original frequencies – Harmonics of original frequencies

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SLIDE 4

AM Fundamentals – Cont’d

  • Only the following components resulting from non-

linear mixing are used on an AM waveform:

– Carrier frequency (fc) – Lower-side frequency (fc - fi) – Upper-side frequency (fc + fi)

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SLIDE 5

Figure 2-1 Linear addition of two sine waves.

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SLIDE 6

Figure 2-2 Nonlinear mixing.

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SLIDE 7

AM Waveforms

  • An AM modulated signal can be expressed as:

e(t) = (Ec + Ei sin wit) sin wct where: Ec = peak value of carrier signal Ei =peak value of intelligence signal wc= angular frequency of carrier signal wi= angular frequency of intelligence signal

  • It can be demonstrated that:

e(t)= Ec sin wct + (Ei/2)cos (wc - wi)t - (Ei/2)cos (wc + wi)t

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SLIDE 8

Figure 2-3 AM waveform under varying intelligence signal (ei) conditions.

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SLIDE 9

Figure 2-4 Carrier and side-frequency components result in AM waveform.

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SLIDE 10

Figure 2-5 Modulation by a band of intelligence frequencies.

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SLIDE 11

Figure 2-6 Solution for Example 2-1.

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SLIDE 12

Percentage Modulation

  • Aka Modulation Index or Modulation Factor
  • Measure of extend to which carrier voltage is varied

by intelligence

  • Defined as: %m = Ei / Ec * 100

– Ei: Peak value of intelligence signal – Ec: Peak value of carrier signal

  • Can also be computed using the peak-to-peak value
  • f the AM waveform (see Fig. 2-8)

– Convenient in graphical (oscilloscope) solutions.

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SLIDE 13

Figure 2-8 Percentage modulation determination.

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SLIDE 14

Overmodulation

  • Overmodulation is a condition that occurs when an

excessive intelligence signal overdrives an AM modulator making %m > 100% (because Ei> Ec)

  • Modulated carrier amplitude reach value greater than

double of unmodulated value

  • It produces a distortion known as sideband splatter,

which results on transmission at frequencies outside the allocated range

  • It is unacceptable because it causes severe interference

with other stations and causes a loud splattering sound to be heard at the receiver.

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SLIDE 15

Figure 2-9 Overmodulation.

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SLIDE 16

AM Analysis

  • Recall:

e(t) = (Ec + Ei sin wit) sin wct = Ec sin wct + (Ei/2)cos (wc - wi)t + (Ei/2)cos (wc + wi)t

  • Since Ei = m Ec , then:

e(t) = Ec sin wct + (mEc/2) cos (wc - wi)t + (mEc/2) cos (wc + wi)t

  • Therefore, the side-frequency amplitude is:

ESF = mEc/2

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SLIDE 17

Why is important to use a high %m?

  • The higher m, the more transmitted power gets to
  • ur sidebands, which contain the intelligence.
  • The total power can be computed as:

PT = PC + 2PSF = PC (1 + m2 / 2) Where: PC : carrier power PSF : single sideband power

  • The total current can be computed as:

IT = Ic 𝟐 + 𝒏𝟑/𝟑

  • The power efficiency can be computed as:

Efficiency = 2PSF / PT = m2 / (2 + m2)

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SLIDE 18

AM Transmitter System

  • Refer to block diagram at Fig. 2-18 (next slide).
  • Main components are:

– Oscillator: generates carrier signal at high accuracy (crystal- controlled) – Buffer Amplifier: provides high impedance load to oscillator to minimize drift – Intelligence Amplifier: amplifies the signal from input transducer – Modulated Amplifier (aka Modulator): generates modulated/mixed signal – Linear Power Amplifier: amplifies modulated signal on high- power (commercial) systems

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SLIDE 19

Figure 2-18 Simple AM transmitter block diagram.

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SLIDE 20

Trapezoidal Patterns

  • Method to check proper modulation of AM signal

– More revealing than viewing signal on scope

  • Procedure:

– Put scope in XY Mode – Put AM signal on vertical – Put intelligence signal on horizontal (through RC phase-shift network

  • Possible Results (see Fig 2-23):

– Top & bottom straight lines: proper modulation – Single vertical line: no intelligence (carrier only) – Concave curvature: poor linearity on modulation stage – Convex curvature: improper bias or low carrier signal – Half oval with inner Y : improper phase relationships

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SLIDE 21

Figure 2-23 Trapezoidal pattern connection scheme and displays.

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SLIDE 22

Spectrum Analyzers

  • Show plot of amplitude vs frequency
  • Swept-tuned (superhetereodyne) Analyzer – uses

analog frequency sweep, can go up to GHz range

  • Fourier Analyzer – digitizes waveform and uses FFT
  • algorithms. Limited to ~40 MHz (EET Labs)
  • Vector Signal Analyzer (VSA) – uses analog front-

end and digitizes after down-convertion.

– Best of both worlds, but expensive – Can measure Total Harmonic Distortion (THD)

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SLIDE 23

Figure 2-24 Spectrum analysis of AM waveforms.

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SLIDE 24

Figure 2-25 Spectrum analyzer and typical display. (Courtesy of Tektronix, Inc.)

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SLIDE 25

Figure 2-25 (continued) Spectrum analyzer and typical display. (Courtesy of Tektronix, Inc.)

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SLIDE 26

Relative Harmonic Distortion (RHD)

  • Ratio of fundamental with respect to the largest

undesired harmonic

– The greater, the better

  • Can be computed (in dB) as:

RHD = 𝟑𝟏 𝒎𝒑𝒉 𝑾𝟐/𝑾𝟑 Where: V1: desired component (fundamental frequency) V2: largest undesired harmonic component

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SLIDE 27

Figure 2-26 Relative harmonic distortion.

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SLIDE 28

Total Harmonic Distortion (THD)

  • Ratio of power from unwanted harmonics to

desired frequency components

– The greater, the worst

– More descriptive distortion spec than RHD

  • Occurs in amplifiers and non-linear devices
  • Can be computed as:

THD = (𝑾𝟑

𝟑 + 𝑾𝟒 𝟑 + 𝑾𝟓 𝟑 + … )/𝑾𝟐 𝟑

Where: V1: desired component (fundamental frequency) V2, V3, … : undesired harmonic components