lecture 38 oscillators amit kumar mishra ece, iit g
TRANSCRIPT
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Lecture 38Oscillators
Amit Kumar Mishra
ECE, IIT G
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Amplitude Stabilization
Loop gain of oscillator changes due to power supply voltage, component value or temperature changes.
If loop gain is too small, desired oscillation decays and if it is too large, waveform is distorted.
Amplitude stabilization or gain control is used to automatically control loop gain and place poles exactly on jw axis.
At power on, loop gain is larger than that required for oscillation.As oscillation builds up, gain is reduced to minimum required to sustain oscillations.
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Amplitude Stabilization in RC Oscillators: Method 1
R1 is replaced by a lamp. Small-signal resistance of lamp depends on temperature of bulb filament.If amplitude is large, current is large, resistance of lamp increases, gain is reduced. If amplitude is small, lamp cools, resistance decreases, loop gain increases. Thermal time constant of bulb averages signal current and amplitude is stabilized.
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Active LC oscillator
Higher range Higher Q factor (=> ??)
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Hartely (b) and Colpitt (a) oscillators
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LC Oscillators: Colpitts Oscillator
)/(1 orSRG GS
CCC 23
L
CC
sL
Gmg
GCGCGDCsCC
GDCCCs
s
s
GmgCCs
sC
mgCs
sLGDCCs
)31
(3
)3
()31
(31
2
)(sV
)(gV
)31
(3
)3
(
/1)3
(
0
0
=0, collect real and imaginary parts and set them to zero.
TCLCo
131
31CC
CCGDC
TCC
At 0
13CC
Rmg
Generally more gain is used to ensure oscillation with amplitude stabilization.
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LC Oscillators: Hartley Oscillator
2
1
1
1
212
1
2
)(sV
)(gV
)2
/1()1
/1(2
/1
)2
/1(2
/1
0
0
LLC
LLssLmg
ogmgsC
s
s
ogmgsLsL
sL
mgsL
sLsC
=0, collect real and imaginary parts and set them to zero.
)21
(1LLCo
At 0
21LL
f
Generally more gain is used to ensure oscillation with amplitude stabilization.
G-S and G-D capacitances are neglected, assume no mutual coupling between inductors.
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Another practical Colpitt Osc.
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Crystal oscillator
In its heart is a piezoelectric crystal Pizo crystal have opposite faces plated with
electrodes. 3 major advantages:
Very high Q (10s to 100s of thousands) Stable with temp. and time Can give freq. upto several MHz
Q and res. Freq. depends on the size, orientation of faces, and mount
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Crystal Oscillators
Crystal: A piezoelectric device that vibrates is response to electrical stimulus, can be modeled electrically by a very high Q (>100,000) resonant circuit.
L, CS, R represent intrinsic series resonance path through crystal. CP is package capacitance. Equivalent impedance has series resonance where CS resonates with L and parallel resonance where L resonates with series combination of CS and CP.
SC
PC
SCPC
TC
TLCL
RssS
LCLRss
PsC
SZ
PZ
SZPZ
CZ
12
12
1
Below S and above P, crystal appears capacitive, between S and P it exhibits inductive reactance.
Used to replace L in Colpitt
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Crystal
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Crystal Oscillators: Example Problem: Find equivalent circuit elements for crystal with given parameters. Given data: fS=5 MHz, Q=20,000 R =50 W, CP =5 pF
Analysis:
5.02MHz
fF)6.31mH)(8.31(21
2
1
fF8.31
)0318.0(2710
12
1
mH8.31)6105(2
)000,20(50
SC
PC
SCPC
LPf
LS
SC
S
RQL
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Pierce crystal oscillator configuration
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Crystal Oscillators: Topologies
Colpitts Crystal Oscillator Crystal Oscillator using BJT
Crystal Oscillator using JFET
Crystal Oscillator using CMOS inverter as gain element.
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The classic 555 timer circuit
Since 1972 (by Signetics Co.) called “IC Time Machine”!
Numerous clones available Low-cost, accurate and easy to design with
(>1B units per year) ~23 Transistors; 2 diodes; ~16 resistors (DIP-
8) Can work in monostable, astable and bistable
configurations
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From the SE555 datasheet
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Schemtics
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Block diagram
S=R=0; Q=Q’ S=1;R=0; Q=1 S=0; R=1; Q=0 Vcc ~ 5V Vth = 2/3Vcc Vtl = 1/3Vcc Why 555? Transistor ~ switch
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Monostable configuration
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Astable configuration
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Many Thanks