Electronics I

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Transcript Electronics I

CO2005: Electronics I
Diode Circuits
張大中
中央大學 通訊工程系
[email protected]
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Rectifier Circuits
 A diode rectifier forms the first stage of a dc power supply. Rectification is the process of
converting an alternating (ac) voltage into one that is limited to one polarity.
 Rectification: half-wave rectification and full-wave rectification
half-wave
rectification
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full-wave
rectification
Electronics I, Neamen 3th Ed.
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Half-Wave Rectification
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Q-point Analysis of Half-Wave Rectification
 Load line Concept for Q-point
 Battery Charger
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Full-Wave Center- Tapped Transformer Rectification
 The full-wave rectifier inverts the negative portions of the sine wave so that a unipolar
output signal is generated during both halves of the input sinusoid.
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Full-Wave Bridge Rectifier
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Electronics I, Neamen 3th Ed.
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Full-Wave Bridge Rectifier
 Full-wave bridge rectifier circuit to produce negative output voltages
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Filter Circuit for Diode Rectifier
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Analysis of Filter Circuit for Diode Rectifier
After theoutputhas reached thepeak value, vo (t )  VM et '/ RC
VL  VM eT '/ RC
 T 
Vr  VM  VL  VM (1  eT  / RC )  VM 

RC


 Tp 
 T 
As RC  T , T   Tp , andVr  VM 

V

 M 
RC
RC




1
V
Tp 
, Vr  M
2f
2 fRC
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Current in the Filter Circuit for Diode Rectifier
iD  iC  iR
iD  C
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dvo vo

dt R
Electronics I, Neamen 3th Ed.
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Detectors
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Electronics I, Neamen 3th Ed.
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Voltage Doubler Circuit
 There are also voltage tripler and voltage quadrupler circuits. These circuits provides a
means by which multiple dc voltage can be generated from a single ac source and power
transformer.
+
-
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+
Electronics I, Neamen 3th Ed.
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Zener Diode Circuits
 Zener Voltage Reference Circuit
I Z maximum: VPS maximumand I L minimum
Ri 
VPS (max) VZ
I Z (max) I L (min)
[VPS (min) VZ ]  [ I Z (max) I L (min)]
I Z minimum: VPS minimumand I L maximum
Ri 
 [VPS (max) VZ ]  [ I Z (min) I L (max)]
VPS (min) VZ
I Z (min) I L (max)
ChooseI Z (min) 0.1I Z (max),we have
I Z (max)
I L (max)[VPS (max) VZ ]  I L (min)[VPS (min) VZ ]
VPS (min) 0.9VZ  0.1VPS (max)
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Electronics I, Neamen 3th Ed.
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Electronics I, Neamen 3th Ed.
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Zener Resistance and Percentage Regulation
 Because of the Zener resistance, the output voltage will not remain constant.
 Source regulation: a measure of the change in output voltage with a change in source
voltage.
Source regulation(%) 
vL
 100%
vPS
 Load regulation: a measure of the change in output voltage with a change in load current.
vL,no load  vL,full load
Load regulation(%) 
 100%
vL, full load
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Electronics I, Neamen 3th Ed.
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Ri  15.3
I L  0 ~ 100m A
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Electronics I, Neamen 3th Ed.
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Electronics I, Neamen 3th Ed.
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Clipper Circuits
 Clipper circuits are used to eliminate portions of a signal that are above or/and below a
specified level.
 Transfer characteristics of a limiter circuits
 Single diode clipper
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Parallel-Based Clipper
if VB  V  VI
then VO  VB  V
if VI  V  VB
then VO  V  VB
if  VB  V  VI
then VO  VB  V
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Parallel-Based Clipper
if VI  V  VB1
then VO  V  VB1
and if  VB 2  V  VI
then VO  VB 2  V
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Electronics I, Neamen 3th Ed.
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Series-Based Clipper
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Clampers
 Clamping shifts the entire signal voltage by a dc level. The distinguishing feature of a
clamper is that it adjusts the dc level without needing to know the exact waveform.
vo (t )  vC  vI  (VM  V )  VM sin t
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Clampers
 Clamping Circuit Including an Independent Voltage Source
vo (t )  vC  vI  (VM  VB  V )  VM sin t
 VB  V  VM (sin t  1)
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Electronics I, Neamen 3th Ed.
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Analysis of Single Diode Circuits
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Electronics I, Neamen 3th Ed.
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Analysis of Two-Diode Circuit
Diode St at es:
(1) D1 off,D 2 off
(2) D1 off,D 2 on
(3) D1 on,D 2 on
(4) D1 on,D 2 off
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Analysis of Two-Diode Circuit (1)
 D1: off, D2: on
Let V   V   V .
If D1 is off, thenD2 is always on.
D2 on : V   V   V ,
iR 1 
V   V  V 
R1  R2
, vo  V   iR1  R1
D1 off : vI  v  V ,
vo
v '  V   iR 2  R2 , iR 2  iD 2  iR1
V   iR1  R1
v'V
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
vI
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Analysis of Two-Diode Circuit (2)
 D1: on, D2: on
D1 on : vI  v'V ,
v'  vI  V , iR 2 
vI  V  V 
R2
D2 on : V   v'V  vI ,
V   vI
vo  vI , iR1 
R1
vo
V
v'V
v'V
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
V
vI
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Analysis of Two-Diode Circuit (3)
 D1: on, D2: off
D1 on : vI  V  V  ,
v'  vI  V , iR 2 
vI  V  V 
R2
D2 off : V   v'V  vI ,
vo  V  , iR1  0
V

vo
V
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
vI
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Diode Logic Circuits
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Photodiode Circuit
 If the photon intensity is zero, the only current through the diode is the reverse-saturation
current, which is normally very small.
 Photons striking the diode create excess electrons and holes in the depletion region. The
electric field separates these excess carriers and sweeps them out of the depletion region,
thus creating a photocurrent in the reverse-bias direction.
I ph  eA
 : quantum efficiency, e : electroniccharge
 : photonflux density, A : junctionarea
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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Light-Emitting Diode (LED) Circuits
中央大學通訊系 張大中
Electronics I, Neamen 3th Ed.
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