Analogue Electrical Design
Basics R R-
-
the toner Diode
R ,"
-
-
.
R ,
= REV
R' R2
Potential Ven
t
Dividers
Designed for the operation the
°
in reverse -
brakedown
y
✓out Rr Zener diode has bracedown voltage
region
=
r. a
•
R, Rz Extrinsic Silicon
.
+ •
-
Add
to the
equal output Voltage -
to make
PI Rz impurities a
↳
R =
2- Rz
A material semi
conducting
-
run
Cathode
&
type type
t
n
p
- -
vz Brauedown
7¥
-
°
NO movement " "age h h
of charge These materials have
mostly
Vo Load
hole (positive ) VD
through carriers or
.
a
ph junction at
-
cnegan.ve ,
an.ae
demon came,
voyage , cons,.am,
equi,;w,um ,
region Region
Biasing
pn junction
a - : known as a diode ; The current cannot
barrier
Amplifier Modelling
flow from p to n unless the inbuilt
potential
external circuit
is overcome
by the .
-
- - - -
- - -
. . -
. .
,
Rs
.
'
Rout s
keIhfNan?÷ ) VflnµanN÷)
I
'
y
Ubi
'
O H
- -
- -
- - i t .
A l l
Output Vs
'
Rin
±
Axvin
'
Toad
Input ' l
Pot
gal '
Output Axinput
.
i
vin
Thermal Voltage
, - -
-
,
,
-0A
'
. -
÷
kIq
!
-
VT
-
-
Room
-
25mV Temp
- - - -
-
at
- - -
-
-
=
Vent
Voltage Gain Av
•
, : -
-
Vin
•
Reverse Brake down Reverse voltage : to reach °
Power Gain :
Ap -
-
a certain value , avalanches and makes
•
Current Gain :
A;
huge current .
Only limited
by external circuit .
Feedback V
E ous
A
t
7 ,
Forward Bias
i .Vin
DC
:
voltage positive terminal connected
Negative Feedback System
.
B s
to the and Gets
p region negative to the n
region
to
vous
-
-
t
Vo Alvin sprout )
.
E A 7 ,
-
-
-
O FV and then Vin
around current
flows
-
-
#p
.
=
s s
Diode Characteristic TV curve . n
anode cathode
im f
-
-
Feedback Fraction •
Positive Feedback leads to
)
+
(Vin flout ) A
-
Reverse saturation VD Vo -
-
-
oscillation
current
Is =
Reverse Saturation Current
¥ ,¥p
b
loop Vt = Thermal voltage =
Eat:{Id -
- Acn
"T
, " .
(
"" ^
"
Wh " ✓ " ° '
" "
"
"
Oscillators
iii. Is
(÷) a) -
With positive feedback P will
R
.
frequency be a
selective network at low
frequencies only need
Vss Rip
-
-
-
+ Vp
Aeuljwl VI z.f-p-g.co,
+
capacitive circuits
Qa
-
(
-
1) TV
-
-
Vd
.
.
Vss -
vs, = RI, e
-
,
•
Sinusoidal Oscillators -
The Barkerhauser Criterion
The diodes have to have a resistor to limit the current or it
)
Loopgain LGW AB Gw) At
-
-
-
the
destroy itself
•
phase loop
-
will . wo
loop gain
'
% must be zero
At specific frequency
•
a
Plot Either the TD
-
-
O
VFR and the
magnitude of
loop gain (Ap )
the load lines
°
diode
'
→
to the
behaves like aractaistic loop gain must be
unity
a short circuit or an ACL will tend to
infinity "
open circuit .
.
If it behave, as a
conman ya , .nu," .am sustain man"IEp%7%:::
short circuit the current is ¥ Exide
oscillations of
no input
applied '
•
If it behaves as circuit
frequency w
°
To sustain oscillation AB
-
I
an
open vans -
,
in O
Apljw) I
-
)
Lcjw
-
will not be sinusoidal
two is = =
current AB >1 oscillations
no
flows .
Apc 1 oscillations will die out .
°
Diode not
conducting and not
forward biased
The
=
'
frequency of oscillation Wo is determined
Soley by the phase
effectively open circuit
only reverse currentflows .
characteristics of the feedback loop .
The loop oscillates at the
Diode frequency which the phase is zero
conducting
°
is it conducts
assume
perfectly
.
V silicon 20.7
-
-
.
Basics R R-
-
the toner Diode
R ,"
-
-
.
R ,
= REV
R' R2
Potential Ven
t
Dividers
Designed for the operation the
°
in reverse -
brakedown
y
✓out Rr Zener diode has bracedown voltage
region
=
r. a
•
R, Rz Extrinsic Silicon
.
+ •
-
Add
to the
equal output Voltage -
to make
PI Rz impurities a
↳
R =
2- Rz
A material semi
conducting
-
run
Cathode
&
type type
t
n
p
- -
vz Brauedown
7¥
-
°
NO movement " "age h h
of charge These materials have
mostly
Vo Load
hole (positive ) VD
through carriers or
.
a
ph junction at
-
cnegan.ve ,
an.ae
demon came,
voyage , cons,.am,
equi,;w,um ,
region Region
Biasing
pn junction
a - : known as a diode ; The current cannot
barrier
Amplifier Modelling
flow from p to n unless the inbuilt
potential
external circuit
is overcome
by the .
-
- - - -
- - -
. . -
. .
,
Rs
.
'
Rout s
keIhfNan?÷ ) VflnµanN÷)
I
'
y
Ubi
'
O H
- -
- -
- - i t .
A l l
Output Vs
'
Rin
±
Axvin
'
Toad
Input ' l
Pot
gal '
Output Axinput
.
i
vin
Thermal Voltage
, - -
-
,
,
-0A
'
. -
÷
kIq
!
-
VT
-
-
Room
-
25mV Temp
- - - -
-
at
- - -
-
-
=
Vent
Voltage Gain Av
•
, : -
-
Vin
•
Reverse Brake down Reverse voltage : to reach °
Power Gain :
Ap -
-
a certain value , avalanches and makes
•
Current Gain :
A;
huge current .
Only limited
by external circuit .
Feedback V
E ous
A
t
7 ,
Forward Bias
i .Vin
DC
:
voltage positive terminal connected
Negative Feedback System
.
B s
to the and Gets
p region negative to the n
region
to
vous
-
-
t
Vo Alvin sprout )
.
E A 7 ,
-
-
-
O FV and then Vin
around current
flows
-
-
#p
.
=
s s
Diode Characteristic TV curve . n
anode cathode
im f
-
-
Feedback Fraction •
Positive Feedback leads to
)
+
(Vin flout ) A
-
Reverse saturation VD Vo -
-
-
oscillation
current
Is =
Reverse Saturation Current
¥ ,¥p
b
loop Vt = Thermal voltage =
Eat:{Id -
- Acn
"T
, " .
(
"" ^
"
Wh " ✓ " ° '
" "
"
"
Oscillators
iii. Is
(÷) a) -
With positive feedback P will
R
.
frequency be a
selective network at low
frequencies only need
Vss Rip
-
-
-
+ Vp
Aeuljwl VI z.f-p-g.co,
+
capacitive circuits
Qa
-
(
-
1) TV
-
-
Vd
.
.
Vss -
vs, = RI, e
-
,
•
Sinusoidal Oscillators -
The Barkerhauser Criterion
The diodes have to have a resistor to limit the current or it
)
Loopgain LGW AB Gw) At
-
-
-
the
destroy itself
•
phase loop
-
will . wo
loop gain
'
% must be zero
At specific frequency
•
a
Plot Either the TD
-
-
O
VFR and the
magnitude of
loop gain (Ap )
the load lines
°
diode
'
→
to the
behaves like aractaistic loop gain must be
unity
a short circuit or an ACL will tend to
infinity "
open circuit .
.
If it behave, as a
conman ya , .nu," .am sustain man"IEp%7%:::
short circuit the current is ¥ Exide
oscillations of
no input
applied '
•
If it behaves as circuit
frequency w
°
To sustain oscillation AB
-
I
an
open vans -
,
in O
Apljw) I
-
)
Lcjw
-
will not be sinusoidal
two is = =
current AB >1 oscillations
no
flows .
Apc 1 oscillations will die out .
°
Diode not
conducting and not
forward biased
The
=
'
frequency of oscillation Wo is determined
Soley by the phase
effectively open circuit
only reverse currentflows .
characteristics of the feedback loop .
The loop oscillates at the
Diode frequency which the phase is zero
conducting
°
is it conducts
assume
perfectly
.
V silicon 20.7
-
-
.