data communication, lecture5 - sharif
TRANSCRIPT
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1 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
Data Communication, Lecture5
Some Analog Systems
Data Communication, Lecture 5
2 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
Analog Carrier Wave SystemsCarrier wave techniques form a bases for telecommunication systemsMultiplexing techniques
• Frequency Division Multiplexing (FDM)• Quadrature-carrier multiplexing
– Phase-locked loop (PLL)• FM-demodulator• frequency synthesis
Data Communication, Lecture 5
3 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
Frequency-division multiplexing (FDM)
Data Communication, Lecture 5
4 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
FDM receiver
First the FDM wave is demodulated. Then each subcarrieris detected by using separate bandpass filters anddetectors.
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Data Communication, Lecture 5
5 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
Advanced FDM: xDSL with OFDMConventional FDM:– Each channel occupies accurately certain frequency band– Bandwidth efficiency increased by using SSB modulation– Usage of guard bands wastes resources– A lot of filtering functions (complex circuitry)
Modern FDM: OFDM (orthogonal frequency division multiplexing) and DMT (discrete multitone modulation) yield increased spectral adaptation. Applied in xDSL (digital subscriber line techniques).
DMT with cable attenuation only
DMT with cable attenuation, interferenceand cross-talk
rejected sub-band
Data Communication, Lecture 5
6 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
Phase-locked loops (PLLs)
Phase-locked loop is a feedback arrangement capable to synchronize itself to a noisy external referenceThe output signals of the loop can be used to produce for instance multitude of locked frequenciesPLL application areas include...– modulators– demodulators– frequency synthesis– multiplexers– signal processors
Data Communication, Lecture 5
7 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
The PLL principle
The PLL circuit consists of– phase comparator (in the figure below the multiplier)– lowpass filter– feedback amplifier– VCO (voltage controlled oscillator), whose output
frequency is linearly proportional to input amplitudePrinciple: phase difference of Xc(t) and v(t) adjusts VCO
Phase comparator output iscomparable to phase difference of input signals
Data Communication, Lecture 5
8 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
PLL phase comparator realizationsCircuits: (a) analog and (b) digital phase comparator circuitNote that for (a) output is proportional to– input signal phase difference– input signal amplitudes (unintended AM thus harmful)
In (b) AM effects are compensated and response is more linear
XOR-circuit 1 1sin( cos( ) sin( ) sin( )2 2a β α β α β) = − + +
ideal
pulse ratio: 50/50
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Data Communication, Lecture 5
9 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
FM detection by PLL
( ) 2 ( )tv vt K y t dtφ π ∫=
time domain
phase domain
frequency domain
( )( )
( ) ( )
v
t
v
d ttdt
t d
φω
φ ω α α−∞∫
⎧ =⎪⎨⎪ =⎩ 1 1( ) ( ) (0) ( )22
t
v d V f V fj f
λ λ δπ−∞
⇔ +∫
sin ( ) ( ) ( ) ( )ε ε φ φ≈ = − vt t t t
Data Communication, Lecture 5
10 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
PLL FM-demodulator: the feedback analysis
1
1 2
( )( ) ( )1 ( ) ( )
H fY f X fH f H f
=+
( )( ) ( )1 ( ) /1 ( ) ( )
( )( )
a
a v
v
a v
K H fY f fK H f K jf
jfKH f fK jf KH f
K K K
= Φ+
= Φ+
=
Solve transfer function with feedback:
This is applied to the linearized PLL yielding relationship between the input phase and output voltage:
( )2 1( ) ( ) ( ) ( ) ( )Y f X f H f Y f H f= −
1 2 1( ) ( ) ( ) ( ) ( ) ( )Y f H f H f Y f X f H f+ =( )Y f
Data Communication, Lecture 5
11 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
Applying the FM signal to the linearized PLL model
Remember the FM wave:
where the modulating signal is denoted by x(t). The input FM phase to the system is thus
This is in frequency domain:
assuming no DC component or V(0) = 0, or
( ) / 2 ( )d t dt f x tφ π ∆=
( ) 2 ( )t
t f x dφ π λ λ∆ ∫=
( ) 2 ( ) /( )f f X f j fπ π∆Φ = 2
0
1 1( ) ( ) (0) ( )22tv d V f V f
j fλ λ δ
π=
∫ ⇔ +1 44 2 4 43
Data Communication, Lecture 5
12 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
Applying FM signal to the detector... (cont.)
Thus the input is and the output is
where the loop equivalent transfer function is
Assume that the first order LP function is used or
( ) ( ) /( )f f X f jf∆Φ =1 ( ) ( )( ) ( ) ( )
( ) L
v v
jfKH f f X fY f f H fK jf KH f K
∆= Φ =+
( )( )( ) ( / )L
H fH fH f j f K
=+
1( )1 ( / )LH f
j f K=
+( )( ) ( ), 1
1 ( / )v v
f fX f WY f X fK j f K K K
∆ ∆⇒ ≈ ≈ <<+
( ) ( )v
fy t x tK
∆⇒ ≈
Y(f)
a vK K K=
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Data Communication, Lecture 5
13 Helsinki University of Technology,Communications Laboratory, Timo O. Korhonen
PLL based frequency synthesizer
VCOVCO
Filt.Filt.PhasedetectorPhase
detector
Divide by10
Divide by10
10out inf f=
inf
By adjusting thedivider differentfrequencies can be producedwhose phase is locked into fin
Reference signal finis locked for instanceto the fundamental frequency of a crystal oscillator