Sine-Wave Sh
Nonlinear-amplification meth
For various input values,
values can be calculated
Transfer curve can be o
V
RC _ vO
(Sine w
vi Q1 R
(Triangular wave)
I
Prof. Tai-Haur Kuo - VE
12
haper (Cont.)
hod
their corresponding output
obtained and is similar to
VCC
O RC
wave)
Q2
R
I
VEE Electronics(3), 2012
- 51
Sine-Wave Sh
Breakpoint method
Piecewise linear transferc
Low-valued R is assumed
V1 Vin V1 Vout Vin
V1 Vin V2 D2 is on (volta
V0 V1 VD (Vin VD V
V2 Vin D1 is on limi
Prof. Tai-Haur Kuo 12
haper (Cont.)
curve
d V1 and V2 are constant
age drop VD )
V1 ) R5
R5 R
4
it V0 to V2 VD
- 52 Electronics(3), 2012
Sine-Wave Sh
V
D1 R1
D2 R5 V2
In R 4 R2 V
V1 V
R3 V
V
D3 R5 R3
D4 V1 12
R3
out V2
R1
V
Prof. Tai-Haur Kuo
haper (Cont.)
In
out
15
V2
V1 2 4
V1 0
V2
3
- 53 Electronics(3), 2012
Precision Rec
Precision half-wave rectifier
" Superdiode "
Vi
_ VA
VO
R
An alternate circuit
R1 D2 R2
Vi
_ D1 VO
Prof. Tai-Haur Kuo 12
ctifier Circuits
--- “superdiode”
VO
1
1
0 Vi
VO
1 0 Vi
1
Electronics(3), 2012
- 54
Precision Rectifie
Application:Measure AC
R2
D2
R1 _ D1
Vi
A 1
Average V1 VP R2 ;whe
π R1 amp
sinu
Prof. Tai-Haur Kuo 12
er Circuits (Cont.)
C voltages
C
R4 VO
R3 _
A2
V1
ere Vp is the peak
plitude of an input
usoid
- 55 Electronics(3), 2012
Precision Rectifie
If 1 ωmin ;ωmin
R4C freq
V2 VP R2 R4
π R1 R3
Prof. Tai-Haur Kuo 12
er Circuits (Cont.)
n is the lowest expected
quency of the input sine wave
- 56 Electronics(3), 2012
Precision Full-W
A DA A
1 B DB B
RL
C
Prof. Tai-Haur Kuo 12
Wave Rectifiers
or
- 57 Electronics(3), 2012
Precision Full-Wave
Vi A _ D1 C
A2
R1 E
R2
_ D2
A1
F
R
Prof. Tai-Haur Kuo 12
e Rectifiers (Cont.)
C VO
P Vi
VO
RL
- 58 Electronics(3), 2012
With load Peak R
Super diode
vi
-
_
buffered R
D2
_ D
v- i A1 12
Prof. Tai-Haur Kuo
Rectifier
RL
C v O
-
R
_
D1 A2 v
- O
C
- 59 Electronics(3), 2012