am modulator ( method #1 - hawa.work am.pdf · •a given am (dsb-lc) broadcast station transmits...
TRANSCRIPT
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Lecture 10: Amplitude Modulation (Double Sideband Large Carrier,
DSB-LC or AM)
Dr. Mohammed HawaElectrical Engineering Department
University of Jordan
EE421: Communications I. For more information read Chapter 4 in your textbook or visit http://wikipedia.org/.
Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
AM Modulator (Method #1)
• Three possibilities (based on the value of A):
– Under modulation; m < 1
– Critical modulation; m = 1
– Over modulation; m > 1
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan 3
m(t)
t ω0
γ|M(ω)|
2πB−2πB0 V
c(t)
t
π
ω0
π
|C(ω)|
ωc−ωc0 V
0 V
x(t)
t
γ/2
ω0
γ/2
|X(ω)|
ωc−ωc
180°
180°
ωc + 2πBωc − 2πB
Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
<< Under modulation
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Ac(t)
t
π A
ω0
π A
|AC(ω)|
ωc−ωc0 V
0 V
x(t)
t
γ/2
ω0
γ/2
|X(ω)|
ωc−ωc
180°
180°
ωc + 2πBωc − 2πB
0 V
ϕ(t)
t
γ/2
ω0
γ/2
|Φ(ω)|
ωc−ωc
0°
ωc + 2πBωc − 2πB
0°
πAπA
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
AM Modulator (Method #2)
• Three possibilities (based on the value of A):
– Under modulation; m < 1
– Critical modulation; m = 1
– Over modulation; m > 1
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan 6
m(t)
t ω0
γ|M(ω)|
2πB−2πB0 V
t ω0
2πA
|FA|
0 V
A
m(t)+A
tω0
γ
|M(ω)+FA|
2πB−2πB0 V
2πA
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
<< Under modulation
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0 V
c(t)
t
π
ω0
π
|C(ω)|
ωc−ωc
ϕ(t)
t
γ/2
ω0
γ/2
|Φ(ω)|
ωc−ωc
0 V
0°
ωc + 2πBωc − 2πB
m(t)+A
tω0
γ
|M(ω)+FA|
2πB−2πB0 V
2πA
0°
πAπA
Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan 8
m(t)
t ω0
γ|M(ω)|
2πB−2πB0 V
t ω0
2πA
|FA|
0 V
A
m(t)+A
t ω0
γ
|M(ω)+FA|
2πB−2πB0 V
2πA
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
<< Over modulation
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0 V
c(t)
t
π
ω0
π
|C(ω)|
ωc−ωc
ϕ(t)
t
γ/2
ω0
γ/2
|Φ(ω)|
ωc−ωc
0 V
180°
ωc + 2πBωc − 2πB
m(t)+A
t ω0
γ
|M(ω)+FA|
2πB−2πB0 V
2πA
180°
πAπA
Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan 10
m(t)
t ω0
γ|M(ω)|
2πB−2πB0 V
t ω0
2πA
|FA|
0 V
A
m(t)+A
t ω0
γ
|M(ω)+FA|
2πB−2πB0 V
2πA
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
<< Critical modulation
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0 V
c(t)
t
π
ω0
π
|C(ω)|
ωc−ωc
ϕ(t)
t
γ/2
ω0
γ/2
|Φ(ω)|
ωc−ωc
0 V
ωc + 2πBωc − 2πB
m(t)+A
t ω0
γ
|M(ω)+FA|
2πB−2πB0 V
2πA
πAπA
Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
Homework
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If we perform AM modulation on the following baseband message signal using m = 0.5, 1, 2, ∞:
• Sketch the modulated signal in time domain ϕAM(t)
• Sketch the frequency domain Fourier Transform ΦAM(ω)
• Determine the modulated signal bandwidth.
−2
2
m(t)
t (seconds)31 50 0.5−0.5
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
AM Modulation Index, m
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≜
m > 1
m = 1
m < 1
m = ∞
Only synchronous (coherent) receivers
can demodulate. Such RX requires using a
PLL (Expensive)
Asynchronous (incoherent) receivers
can demodulate (Very simple and very inexpensive)
More power needed from transmitter
(Larger A)
Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
Example
Sketch the AM modulated signal in time domain ϕAM(t) and frequency domain ΦAM(ω), then calculate the modulated signal bandwidth, average power, power efficiency. Assume the case of tone modulation, and:
– m = 0.5
– m = 1
– m = 2
– m = ∞
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
= . . . + .
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
Notice the Difference!
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
AM Average Power
= 2 = lim#→∞1# ' 2
#
2 = ( cos,- + cos,- .2
2 = 2 cos2,- + 2 cos2,- + 2 cos2,-
2 = 2 cos2,- + 2 cos2,- + 2 cos2,-
2 = 12 2 + 2
2 + = / + - + 0
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
AM Power Efficiency
1 = 2/34 6789#74 6789 = /
= /
/ + -
1 =12 2
12 2 + 2
2 94
1 = 22 + 2 7 747
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
Homework #1
• A given AM (DSB-LC) broadcast station transmits an average carrier power, Pc , of 40 kW and uses a modulation index, m, of 0.707 for tone modulation. Assuming the antenna is represented by a 50 Ω resistive load, calculate:– The transmission efficiency (η).– The total average power output (Pt).– The extra carrier amplitude (A).– The peak amplitude of the output signal.– Answers: 20%; 50 kW; 2000 V; 3414 V.
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
Homework #2
• The baseband signal m(t) shown is passed through the following modulator. Assume the power efficiency is 90%, T = 60 µs and fc = 40 MHz. Determine:
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
Homework #2
• Type of the modulated signal φ(t)?
• Bandwidth of the modulated signal?
• Average power in the sidebands Ps?
• Average power in the extra carrier Pc?
• Modulation index of the modulated signal?
• Magnitude spectrum density of the modulated signal |Φ(ω)| at ω=ωc−2π/T?
• Answers: AM; 166.67 kHz; 18 W; 2 W; 1.5;2π×1.403 δ(ω-ωc+2π/T);
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
AM vs. DSB-SC
• Both require the same transmission bandwidth (equal to 2B).
• DSB-SC allows for a more efficient transmitter (power savings).
• AM allows for a cheaper receiver(asynchronous demodulator), while DSB-SC only works with synchronous detection.
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Copyright © Dr. Mohammed Hawa Electrical Engineering Department, University of Jordan
AM vs. QAM
• Advantages of QAM:– QAM is more bandwidth efficient than AM,
allowing us to send two signals on the same channel (of bandwidth 2B).
– QAM allows for more power efficiency at the transmitter.
• Disadvantages of QAM:– AM can be demodulated using cheap
asynchronous demodulators, but QAM only works with synchronous detection (because of orthogonality).
– There is NO such thing as QAM-LC.
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