Properties of Angle Modulation

Properties of Angle Modulation

Properties of Angle Modulation
Properties of Angle Modulation

Reference:

Sections 4.2 and 4.3 of
Professor Deepa Kundur

S. Haykin and M. Moher, Introduction to Analog & Digital Communications, 2nd ed., John Wiley & Sons, Inc., 2007. ISBN-13 978-0-471-43222-7.

University of Toronto

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

1 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

2 / 25

Angle Modulation

carrier

I

Phase Modulation (PM):

  • θi (t)
  • =
  • 2πfc t + kpm(t)

1 dθi (t)

kp dm(t)

message

  • fi (t)
  • =

=
= fc +

2π dt

Ac cos[2πfc t + kpm(t)]

2π dt

sPM (t)

amplitude modulation

I

Frequency Modulation (FM):

Z

t

θi (t) fi (t)
===
2πfc t + 2πkf

m(τ)dτ

0

phase modulation

1 dθi (t)
= fc + kf m(t)

2π dt

  • ꢀ
  • ꢁ

Z

t

sFM (t)

Ac cos 2πfc t + 2πkf

m(τ)dτ

frequency modulation

0

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

3 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

4 / 25

carrier

carrier

message

message

amplitude modulation

amplitude modulation

phase modulation

phase modulation

frequency modulation

frequency modulation

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

5 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

6 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Constancy of Transmitted Power
  • Constancy of Transmitted Power: AM

1

f0

I

Consider a sinusoid g(t) = Ac cos(2πf0t + φ) where T0 = or T0f0 = 1.

I

The power of g(t) (over a 1 ohm resister) is defined as:

ZZ
Z

T

/2

T

/2

  • 0
  • 0

  • 1
  • 1

P

===

g2(t)dt =

A2c cos2(2πf0t + φ)dt

  • T0
  • T0

−T /2 T
−T /2

  • 0
  • 0

/2

Ac2

T0

1

0

[1 + cos(4πf0t + 2φ)] dt
2

−T /2

0

ꢂꢂꢂꢂ

  • ꢀ
  • ꢁ

T

/2

Ac2

sin(4πf0t + 2φ)

0

t +

2T0

4f0

−T /2

0

  • ꢀꢃ
  • ꢄ
  • ꢃ
  • ꢄꢁ

Ac2

2T0

Ac2

  • T0
  • −T0

sin(4πf0T0/2 + 2φ) − sin(−4πf0T0/2 + 2φ)
=

=

−

+

  • 2
  • 2

4πf0

  • ꢀ
  • ꢁ

sin(2π + 2φ) − sin(−2π + 2φ)

Ac2

T0

  • +
  • =

2T0

4πf0

2

I

Therefore, the power of a sinusoid is NOT dependent on f0, just its envelop

Ac .

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

7 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

8 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Constancy of Transmitted Power: PM
  • Constancy of Transmitted Power: FM

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

9 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

10 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Constancy of Transmitted Power
  • Nonlinearity of Angle Modulation

Consider PM (proof also holds for FM).

I

Suppose

s1(t)

==
Ac cos [2πfc t + kpm1(t)]

s2(t)

Ac cos [2πfc t + kpm2(t)]

Therefore, angle modulated signals exhibit constancy of transmitted

power.

I

Let m3(t) = m1(t) + m2(t).

s3(t)

==
Ac cos [2πfc t + kp(m1(t) + m2(t))]

s1(t) + s2(t)

∵ cos(2πfc t + A + B) = cos(2πfc t + A) + cos(2πfc t + B)

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

11 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

12 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Nonlinearity of Angle Modulation
  • Irregularity of Zero-Crossings

I

Zero-crossing: instants of time at which waveform changes amplitude from positive to negative or vice versa.
Therefore, angle modulation is nonlinear.

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

13 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

14 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Zero-Crossings: AM
  • Zero-Crossings: PM

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

15 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

16 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Zero-Crossings: FM
  • Irregularity of Zero-Crossings

Therefore angle modulated signals exhibit irregular zero-crossings

because they contain information about the message (which is irregular in general).

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

17 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

18 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Visualization Difficulty of Message
  • Visualization: AM

I

Visualization of a message refers to the ability to glean insights about the shape of m(t) from the modulated signal s(t).

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

19 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

20 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Visualization: PM
  • Visualization: FM

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

21 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

22 / 25

  • 4.2 Properties of Angle Modulation
  • 4.2 Properties of Angle Modulation

  • Visualization Difficulty of Message
  • Bandwidth vs. Noise Trade-Off

I

Noise affects the message signal piggy-backed as amplitude modulation more than it does when piggy-backed as angle

modulation.

Therefore it is difficult to visualize the message in angle modulated

signals due to the nonlinear nature of the modulation process.

I

The more bandwidth that the angle modulated signal takes, typically the more robust it is to noise.

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

23 / 25

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

24 / 25

4.2 Properties of Angle Modulation

carrier message amplitude modulation

phase modulation

frequency modulation

Professor Deepa Kundur (University of Toronto)

Properties of Angle Modulation

25 / 25

ꢀ

View Full Text

Details

  • File Type
    pdf
  • Upload Time
    -
  • Content Languages
    English
  • Upload User
    Anonymous/Not logged-in
  • File Pages
    7 Page
  • File Size
    -

Download

Channel Download Status
Express Download Enable

Copyright

We respect the copyrights and intellectual property rights of all users. All uploaded documents are either original works of the uploader or authorized works of the rightful owners.

  • Not to be reproduced or distributed without explicit permission.
  • Not used for commercial purposes outside of approved use cases.
  • Not used to infringe on the rights of the original creators.
  • If you believe any content infringes your copyright, please contact us immediately.

Support

For help with questions, suggestions, or problems, please contact us