Frequency Domain Analysis of Signals and Systems ELEN 3024 - - - PowerPoint PPT Presentation

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Frequency Domain Analysis of Signals and Systems ELEN 3024 - - - PowerPoint PPT Presentation

Frequency Domain Analysis of Signals and Systems ELEN 3024 - Communication Fundamentals School of Electrical and Information Engineering, University of the Witwatersrand July 15, 2013 Amplitude Modulation Proakis and Salehi, Communication


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Frequency Domain Analysis of Signals and Systems

ELEN 3024 - Communication Fundamentals

School of Electrical and Information Engineering, University of the Witwatersrand

July 15, 2013

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Amplitude Modulation

Proakis and Salehi, “Communication Systems Engineering” (2nd Ed.), Chapter 3

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Overview

Power content of various AM modulation schemes

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SLIDE 4

3.2.1.2 Double-Sideband Supressed Carrier AM

u(t) = Acm(t) cos(2πfct + φ) Assume phase of signal set to zero → power in signal is independent of phase

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3.2.1.2 Double-Sideband Supressed Carrier AM

time-average autocorrelation function of u(t) Ru(τ) = lim

T→∞

1 T

  • T

2

− T

2

u(t)u(t − τ)dt

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3.2.1.2 Double-Sideband Supressed Carrier AM

time-average autocorrelation function of u(t) Ru(τ) = lim

T→∞

1 T

  • T

2

− T

2

u(t)u(t − τ)dt = lim

T→∞

1 T

  • T

2

− T

2

A2

cm(t)m(t − τ)×

cos(2πfct) cos(2πfc(t − τ))dt =

A2

c

2

lim

T→∞

1 T

  • T

2

− T

2

m(t)m(t − τ)× [cos(4πfct − 2πfcτ) + cos(2πfcτ)] dt =

A2

c

2 Rm(τ) cos(2πfcτ)

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SLIDE 7

3.2.1.2 Double-Sideband Supressed Carrier AM

Used the fact that: lim

T→∞

  • T

2

− T

2

m(t)m(t − τ) cos(4πfct − 2πfcτ)dt = 0 Because ∞

−∞ m(t)m(t − τ) cos(4πfct − 2πfcτ)dt

= ∞

−∞ F [m(t − τ)] {F [m(t) cos(4πfct − 2πfcτ)]}∗ df

= ∞

−∞ e−j2πf τM(f )

  • M(f −2fc)e−j2πfc t

2

+ M(f +2fc)ej2πfc t

2

∗ df = 0

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SLIDE 8

3.2.1.2 Double-Sideband Supressed Carrier AM

−∞

e−j2πf τM(f ) M(f − 2fc)e−j2πfct 2 + M(f + 2fc)ej2πfct 2 ∗ df = 0 Why?

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3.2.1.2 Double-Sideband Supressed Carrier AM

−∞

e−j2πf τM(f ) M(f − 2fc)e−j2πfct 2 + M(f + 2fc)ej2πfct 2 ∗ df = 0 Why? M(f ) limited to the frequency band [−W , W ] and W ≪ fc, therefore no frequency overlap between M(f ) and M(f ± 2fc)

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3.2.1.2 Double-Sideband Supressed Carrier AM

Fourier transform on both sides of: F(Ru(τ)) = F( A2

c

2 Rm(τ) cos(2πfcτ))

Su(f ) =

A2

c

4 [Sm(f − fc) + Sm(f + fc)]

⇒ power-spectral density of DSB-SC signal is the power-spectral density of the message shifted upward and downward by fc and scaled by A2

c/4.

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3.2.1.2 Double-Sideband Supressed Carrier AM

To obtain total power in modulated signal

  • Substitute τ = 0 in time-average autocorrelation function
  • integrate power-spectral density of modulated signal

Pu =

A2

c

2 Rm(τ) cos(2πfcτ)|τ=0

=

A2

c

2 Rm(0)

=

A2

c

2 Pm

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3.2.1.2 Double-Sideband Supressed Carrier AM

Example 3.2.2

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3.2.2.2 Conventional Amplitude Modulation

Conventional AM signal similar to DSB when m(t) is substituted with 1 + amn(t) Pu = A2

c

2 Pm Pm power in the message signal.

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3.2.2.2 Conventional Amplitude Modulation

For AM DSB FC: Pm = lim

T→∞

1 T

  • T

2

− T

2

(1 + amn(t))2dt lim

T→∞

1 T

  • T

2

− T

2

(1 + a2m2

n(t))dt

Assuming average of mn(t) = 0. Pm = 1 + a2Pmn

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3.2.2.2 Conventional Amplitude Modulation

Hence Pu = A2

c

2 + A2

c

2 a2Pmn First component → carrier Second component → information carrying component.