Technical Aspects-5 - Semiconductors

Download Report

Transcript Technical Aspects-5 - Semiconductors

Chelmsford Amateur Radio Society
Advanced Course
Technical Aspects
Part-5 - Semiconductors
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
1
Solid State Devices
• Semiconductors form the basis of all modern solid state
devices - diodes, transistors, analogue and digital
integrated circuits etc
• Common Semiconductors are Silicon and Germanium
• Advance Course requires a knowledge of
– Semiconductor theory
– Diodes, including Zeners and Varicaps
– Bipolar & FET Transistors
– Amplifiers - Circuits, Classes, Efficiency
Note: RF Amps inc. Valves covered in Transmitter Course
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
2
Origins of Semiconductors
• Silicon and
Germanium are in
Group-IV where each
atom has 4 electrons
in its outer shell
Group IV
Si
Silicon
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
3
Semiconductors
• In pure (intrinsic) Silicon and Germanium all four outer electrons
pair with neighbours in the crystal lattice leaving none free - making
them insulators
• By doping these materials with very small amounts of impurities,
Electron-rich (N-type) or Electron-poor versions (P-type) can be
created
• N-type dopants have one extra electron and come from Group-V
– Phosphorous, Arsenic, Antimony
• P-Type dopants have one less electron and come from Group-III
– Boron, Aluminium, Indium
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
4
N-type and P-type
• Example shown is
Silicon with n-type
doping by Arsenic
• Arsenic has an extra
electron not used for
pairing up in covalent
bonds, and is free to
move under bias
• In p-type - a positive
‘hole’ is left due to a
shortage which behaves
similar to a real electron
‘Spare’
Electron
As
Si
n-type doping
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
5
P-N Junction - The Diode
• A junction between P-type an N-type material will have a charge
across it - a potential barrier
• Near the junction some electrons fill the holes nearby, making the
region devoid of charge, the depletion layer, which is an insulator
• If bias is applied, the depletion layer narrows until electrons will flow
easily from N to P
• If reverse bias is applies the depletion region will widen and stop flow
Junction
N
- -
+
+
P
+
+
Depletion Region
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
6
Diodes
• Standard Diodes act as rectifiers
• Forward threshold Vf is: Silicon ~0.6v, Germanium ~0.4v
• Reverse Breakdown, Vr usually many volts
+I
Ge
Si
Vr
Vf
-I
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
7
Varicap Diodes
• When Diodes are reverse biased the depletion layer acts as the
insulating layer of a capacitor
• Varicap Diodes also known as Varactors exploit this
• Higher reverse voltages widen the depletion layer, driving the
capacitive plates apart, lowering the capacitor value
• Typical values are of the order of pF
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
8
Zener Diodes
• In normal diodes, little current flows when reverse biased up to the
point of catastrophic breakdown
• Zener Diodes have a well defined reverse breakdown voltage which
can act as a voltage reference for PSU regulators
• Current in the diode must be limited to avoid excess heat dissipation
+VE
+5.1V
0V
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
9
Bipolar Transistors
• Ordinary transistors are known as bipolars - two P-N junctions
• Apply ‘bias’ current in the base to control Collector-Emitter current
• Small Signal Gain or ‘Beta’ is the ratio of IC/IB
IC = ß x I B
Collector
Collector
IC
- N-
+
P
+
- - N-
Emitter
Chelmsford Amateur Radio Society
Advanced Licence Course
NPN
IE
Base
IB
Emitter
Base
NB: IE = IC + IB
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
10
Bipolar Transistors
• Two types - NPN and PNP
Collector
• Base-Emitter similar to Diode characteristic
Base
• ‘Bias’ current in the base controls
Collector-Emitter current
• PNP has negative current in the Base for bias
40µA
1 mA
mA
Emitter
IB = 60µA
IC
IC
NPN
20µA
E
B
C
PNP
0.5 V
VBE
Chelmsford Amateur Radio Society
Advanced Licence Course
12 V
Murray Niman G6JYB
VCE
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
11
Bias Issues
• Bias determines the operating point of a transistor
• Transistors are temperature dependent and have variable gain
• Circuits need to be designed to be relatively independent of this
and give stable operation
• This issue is known as bias stability
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
12
FETs
d
p-type
• FETs are a semiconductor device similar to a Valve
Depletion
Layer
g
• Operates by a field effect due to Voltage
(as opposed to Current in a Bipolar)
• GDS Terminology refers to Electron flow
s
• n-Channel and p-Channel variants exist
n-Channel
• Insulated Gate FETS give NMOS, PMOS,
and CMOS - which are all static sensitive
Drain
G
Gate
D
G2
S
G1
d
g
Depletion
Layer
about to
pinch off
channel
Source
n-Channel
Chelmsford Amateur Radio Society
Advanced Licence Course
p-Channel
Dual Gate
Insulated FET
Murray Niman G6JYB
s
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
13
Common Emitter
• Three circuit configurations are
possible:-
+V
Common Emitter,
Common Collector and
Common Base
Output
• Common Emitter refers to Emitter
being Common to Input & Output
• A rise in the input voltage turns on
the device harder lowering the
voltage on the collector and output
Input
Low Zin
~1K
Medium Zout
~ 5K
• Thus the circuit inverts, or is said
to give 180° phase change
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
14
Common Collector
• Common Collector is
also popularly called
Emitter Follower
+V
• Output Voltage is similar
to input but can supply
much more current
Input
• So no Voltage gain, but
used for current buffering
• Collector is Common,
as at AC the PSU rails
have zero potential
Chelmsford Amateur Radio Society
Advanced Licence Course
High Zin
50k-2M
Murray Niman G6JYB
Output
Low Zout
10-500 Ohms
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
15
Common Base
• Base is common to
input and output
- thus Common Base
• A positive input voltage will
decrease VBE and reduce IC;
causing the Collector voltage
to rise, so output is in phase
with input
• Mainly used for RF
frequencies
- eg in IF Amplifier chains
+V
High Zout
50k
Input
Low Zin
50 Ohms
Output
Capacitor
ensures no
signal on
the base
• Common base amps amplify
voltage - not current
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
16
Amplifier Class & Bias
• Class-A, B, AB and C are defined by the
bias and operating region of the
transistor
• Higher Classes aim to reduce wasted
Output Current and improve efficiency
IC
IC
Distorted
Output
Output
VBE
Input signal
normal bias voltage
Chelmsford Amateur Radio Society
Advanced Licence Course
VBE
Input signal
low bias voltage
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
17
Amplifier Classes
• Class-A
Biased well on for high fidelity but also results in low efficiency and
high heat dissipation in poweramps
• Class-B
Gives only only half the waveform, so usually used in Push-Pull
configurations. Fairly efficient, but can give crossover distortion
• Class-AB
A variation of above with transistor biased to conduct for more than
half a cycle for better fidelity, but modest dissipation
• Class-C
Nonlinear but efficient - high distortion needs filtering
- Useful for constant amplitudes such as FM and GSM mobile phones
• Other Classes exist but are out of scope: D, E, F, G, H, S etc
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
18
Class-B Push-Pull
+15 V
• Class-B only gives half a
sine wave
TR1
• In Push-Pull:TR1 gives positive half,
TR2 give negative half
0.5 Ohms
• Need to keep Bases at
0.7V else crossover
distortion occurs.
Output
bias adjust
0.5 Ohms
• Using diodes to do this
gives a degree of tracking
vs temperature
TR2
Input
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
-15 V
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
19
Amplifier Efficiency, 
• Principal efficiency definition, usually expressed as a
percentage.
Collector/Drain/Anode Efficiency:
 = PRFout / PDCin
• For info, other definitions are:
• Power Added Efficiency:
Pae = (PRFout - PRFin) / PDCin
• Overall Efficiency:
Overall = PRFout / (PDCin+PRFin)
– a good criterion (esp for a multistage amp) but not often quoted
Chelmsford Amateur Radio Society
Advanced Licence Course
Murray Niman G6JYB
Slide Set 5: v1.2, 26-Oct-2006
(3) Technical Aspects - Semiconductors
20