73559_Chapter 5 part2 2010
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Transcript of 73559_Chapter 5 part2 2010
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8/15/2019 73559_Chapter 5 part2 2010
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1
Non Sinusoidal
Oscillator (Part II)
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2
Non sinusoidal oscillator
Known as relaxation oscillator
Typically use RC circuit or integrator and schmitt
comparator The capacitor charge and discharge. The comparator
compare the capacitor voltage with a reference voltage and
switch between high and low voltage
Lecture will covers
Suare wave generator Triangular wave generator
Sawtooth wave generator
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!
Square wave generator
Composed of 2 components Bistable multivibrator (or Schmitt trigger) "enerate output voltage vo # or $ depending
on vd
RC circuit Charge towards %&' voltage
and %(' voltage depending on
vo
satV +
satV −
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)
*on +nverting Schmitt trigger ,d - v& ( v(
if vd / v0 - &,sat
if vd 1 ( v0 - (,sat
Schmitt trigger will becovered in more detail
in chapter
δ
(
&,sat
On oscillator circuit
V is connected to RC
networ! and com"ared to a
re#erence voltage
V$ is used as Vre#
δ
δ
3or simplicity we
assume -0 in
the analysis
δ
δ
δ
(,sat
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4
Circuit O"eration
The circuit operation can be visuali5ed by loo6ing at the chainreaction in the circuit.
The comparator compare the capacitor voltage with thereference voltage and switch between #&,sat and (,sat$
3irst assume that ,o initial value is high #&,sat$ then analyses theeffect of this setting on the threshold #reference voltage$ and thecomparator output
7xplanation will be based on the notes
vC
vo
(,th
&,th
&,sat
(,sat
t
+nitial operation
Steady(state operation
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Revision% Ste" Res"onse o# &
RC Circuit (#rom circuit theor')
The detail derivation for the oscillation freuency f is
given in the note
+nitially at time t-08 ,0 - v#0$
The current through theresistor R is eual to current
flowing through the capacitor
ic - #,s 9 v$: R - C dv:dt
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erivation o# the voltage vc(t)
(when ca"acitor is charging)*ote that in the oscillator circuit8 the out"ut voltage
Vo is used to charge the capacitor
Charging starts when ,o - &,sat is applied
,s - ,o and ,#t$ - ,c#t$ ,#0&$- ,0 - (,th
( ) ( ) RC t c eV V V t v −
+−=∴thsatsat
,o
Vc
,#0&$
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<
Oscillation requenc' # * + ,-
3irst find t= #the charging time of the
capacitor$
The detail derivation for f is given in the note
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>
Com"uting the ca"acitor
charging time t+
?ssume currently at "oint
+ and moving to "oint .
@sing
?pplied voltage is &,sat 8
,#t$ - ,c#t$
,#0&$- ,0 - (,th
vC
vo
Vth
&,th
$Vsat
Vsat
t
+nitial operation
Steady(state operation
t=t2 +
.
( ) ( )
RC t
c eV V V t v −
+−=∴thsatsat
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=0
Com"uting the ca"acitor
charging time t+
vC
vo
Vth
&,th
$Vsat
Vsat
t
+nitial operation
Steady(state operation
t=t2
+
.
?t point 2 8 t - t=
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==
Square /ave Oscillation
requenc'
+n the circuit t= - t2
121 2t t t T =+=
+= F
F
R
R R RC 1
2ln2
+= F R R
RC
12
1ln2
+
==
F
o
R R RC T
f
121ln2
11
1164.1 R R
F
≈
RC
f o2
1=
.
I# ln(+ $ .R+ ,R
) * +
8
.
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=2
-riangular /ave 0enerator Consist of comparator ?= and integrator ?2
Comparator continuously compares the non(inverting
input at point A with the inverting input #- 0,$.
+f ,& / 0 ,o' - &,sat
+f ,& 1 0 ,o' - (,sat
The integrator
integrate the
suare wave to
produce atriangular wave at
,o
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=!
-ransient voltage current
relationshi" in a ca"acitor
c
cc
dt
dvC i =
,/0
)(
)0(
∫ ∫ ==
t
c
t v
t vc
c dt C idV c
∫ =− +t
ccc d ivt v0
)0()( τ
,c#t$
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=)
Integrator
3rom chapter = notes8 ,c - ,o
-
?s value of t increases8 the area under ,i increases Thus integrating a rectangle wave give a linear increasing negative
value
∫ −
=t
i
F
o d V C R
t V 01
)(1
)( τ τ
C3
(
&
,i
,o
R=
,(
,&
∫ −
=− +t
i
F
oo d V C R
V t V 01
)(1
)0()( τ τ
t
,i
?rea
under
curve
,i
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=4
Com"arator out"ut Vo1 switch between $Vsat and 2
Vsat de"ending on oscillator out"ut Vo
,o is connected to ,& through resistor R=8 Bhen ,o is more negative than 9,th /// the
comparator output will switch to 9,sat Bhen ,o is more positive than &,th /// the
comparator output will switch to &,sat
vo
vo1
Vth
$Vth
$Vsat
Vsat
t
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=
Circuit O"eration ?ssume that when the
supply voltage areswitched on8 ,& slightly above 0 , 8
,c#t-0$ - 0 , ,o' - &,sat
etail description is
given in the note Knowing ,o' we can
derive ,o which turns outto be alternating
negative:positive ramp
vo
vo1
Vth
$Vth
$Vsat
Vsat
t=
=
2
!
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eriving the oscillation #requenc' Be are interested to find the time it
ta6es for the capacitor to chargefrom an initial voltage
,c - (,th to ,c - &,th Considering point 2 !
?ssume at point 28 t-08 at point ! t-t=-T:2 ic - C d,c:dt 8 ic - (iR - (,o':R - &,sat :R
,o - ,c -
,o - ,sat :RC$ t & ,c#t-0$
,0 - ,sat :RC$ t ( ,th
vo
vo1
Vth
$Vth
$V sat
Vsat
t=
2
!
t*3
)0(/0=+
∫ t V dt C i
c
t
c
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=<
eriving the oscillation #requenc' ,o - ,sat :RC$ t ( ,th
?t half period8 t-t= - T:28
T - period8
vo
vo1
Vth
$Vth
$V sat
Vsat
t=
2
!
t-0
( ) th1
V t t vc ==
th1sat V t
RC
V −=
th
sat
2V
T
RC
V −
=
satsat
th 44V RC
V RCV T == ( )sat
1 V R R
F
+
F R
RCRT 1
4=
( )1t t vc =
#=$
#2$
#=$ - #2$
#requenc' o# oscillation4 == 1411
R R
RC T f F o
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=>
Sawtooth(wave "enerator
? sawtooth wave#orm has uneual rise and
fall times.
The rise time tr may be longer than the fall
time tf or vice versa.
tr tf
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Sawtooth(wave "enerator
Circuit The triangular(wave generator can be
converted to a sawtooth generator by adding
a variable dc voltage to the noninverting
terminal of the op(amp.
,ref acts as a reference signal for the
integrator(,sat 1 ,ref 1 ,sat
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2=
Circuit O"eration
+n the triangle oscillator ,= - 0,
Dy changing ,= to ,ref 8 we can change the slope
for the decreasing and increasing ramp function.
That is the main idea of the circuit.
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eriving the out"ut voltage Vo
ecreasing ram" #unction Vo(t) * (Vre# Vsat ) t,RC $ Vth
Increasing ram" #unction
Vo(t) * (Vre# $Vsat ) t,RC Vth
Alease see the
note for detail
explanation
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2!
Oscillation requenc' # * +,-
Escillation period T - tf & tr
ref sat
th2
V V
RCV t f −
=ref sat
th2
V V
RCV t r +
=
ref sat
th
ref sat
th 22
V V
RCV
V V
RCV t t T r f
+
+
−
=+=
2
ref
2
sat
satth4V V V RCV
−=
+==
sat
ref 12
1/
V
V T t cycleduty f
(,sat 1 ,ref 1 ,sat
Alease see the
note for detail
explanation