Title: September 28th 2004
1Transistors
- Student Lecture by
- Giangiacomo Groppi
- Joel Cassell
- Pierre Berthelot
2Lecture outline
- Historical introduction
- Semiconductor devices overview
- Bipolar Junction Transistor (BJT)
- Field Effect Transistors (FET)
- Power Transistors
3Transistor History
- Invention 1947,at Bell Laboratories.
- John Bardeen, Walter Brattain, and William
Schockly developed the first model of transistor
(a Three Points transistor, made with Germanium) - They received Nobel Prize in Physics in 1956 "for
their researches on semiconductors and their
discovery of the transistor effect" - First application replacing vacuum tubes (big
inefficient). - Today millions of Transistors are built on a
single silicon wafer in most common electronic
devices
First model of Transistor
4What is a transistor ?
- The Transistor is a three-terminal, semiconductor
device. - Its possible to control electric current or
voltage between two of the terminals (by applying
an electric current or voltage to the third
terminal). The transistor is an active component.
- With the Transistor we can make amplification
devices or electric switch. Configuration of
circuit determines whether the transistor will
work as switch or amplifier - As a miniature electronic switch, it has two
operating positions on and off. This switching
capability allows binary functionality and
permits to process information in a
microprocessor.
5Semiconductors
- Most used semiconductor
- Silicon
- Basic building material of most integrated
circuits - Has four valence electrons, in its lattice there
are 4 covalent bonds. - Silicon crystal itself is an insulator no free
electrons - Intrinsic concentration (ni) of charge carriers
function of Temperature (at room temp. 300K ni
1010 /cm3)
6Semiconductors 2
- Electric conductibility in the Silicon crystal is
increased by rising the temperature (not useful
for our scope) and by doping. - Doping consists in adding small amounts of
neighbor elements.
7Semiconductors 3 Doping
- Two Dopant Types
- N-type (Negative)
- Donor impurities (from Group V) added to the Si
crystal lattice. - Dominant mobile charge carrier negative
electrons. - Group V elements such as Phosphorous, Arsenic,
and Antimony. - P-type (Positive)
- Acceptor impurities (from Group III) added to the
Si crystal lattice. - Dominant mobile charge carrier positive holes.
- Group III elements such as Boron, Aluminum, and
Gallium.
8The simplest example p-n junction
- Its also called Junction Diode
- Allows current to flow from P to N only.
- Because of the density gradient, electrons
diffuse to the p region, holes to the n region. - Because of the recombination, the region near the
junction is depleted of mobile charges. - Two types of behavior Forward and Reverse biased.
9Forward bias
- Forward biasing
- The external Voltage lowers the potential barrier
at the junction. - The p-n junction drives holes (from the p-type
material) and electrons (from the n-type
material) to the junction. - A current of electrons to the left and a current
of holes to the right the total current is the
sum of these two currents.
10Reverse bias
- Reverse biasing
- Reverse voltage increases the potential barrier
at the junction. - There will be a transient current to flow as both
electrons and holes are pulled away from the
junction. - When the potential formed by the widened
depletion region equals the applied voltage, the
current will cease except for the small thermal
current. Its called reverse saturation current
and is due to hole-electrons pairs generated by
thermal energy.
11Diode characteristics
- Forward biased (on)- Current flows
- It needs about 0.7 V to start conduction (Vd )
- Reversed biased (off)- Diode blocks current
- Ideal Current flow 0
- Real Iflow 10-6 Amps (reverse saturation
current)
12BJT
13Bipolar Junction Transistor (BJT)
- 3 adjacent regions of doped Si (each connected to
a lead) - Base. (thin layer,less doped).
- Collector.
- Emitter.
- 2 types of BJT
- npn.
- pnp.
- Most common npn (focus on it).
Developed by Shockley (1949)
14BJT npn Transistor
- 1 thin layer of p-type, sandwiched between 2
layers of n-type. - N-type of emitter more heavily doped than
collector. - With VCgtVBgtVE
- Base-Emitter junction forward biased,
Base-Collector reverse biased. - Electrons diffuse from Emitter to Base (from n to
p). - Theres a depletion layer on the Base-Collector
junction ?no flow of e- allowed. - BUT the Base is thin and Emitter region is n
(heavily doped) ? electrons have enough momentum
to cross the Base into the Collector. - The small base current IB controls a large
current IC
15BJT characteristics
- Current Gain
- a is the fraction of electrons that diffuse
across the narrow Base region - 1- a is the fraction of electrons that recombine
with holes in the Base region to create base
current - The current Gain is expressed in terms of the ß
(beta) of the transistor (often called hfe by
manufacturers). - ß (beta) is Temperature and Voltage dependent.
- It can vary a lot among transistors (common
values for signal BJT 20 - 200).
16npn Common Emitter circuit
- Emitter is grounded.
- Base-Emitter starts to conduct with VBE0.6V,IC
flows and its ICbIB. - Increasing IB, VBE slowly increases to 0.7V but
IC rises exponentially. - As IC rises ,voltage drop across RC increases and
VCE drops toward ground. (transistor in
saturation, no more linear relation between IC
and IB)
17Common Emitter characteristics
Collector current controlled by the collector
circuit. (Switch behavior) In full saturation
VCE0.2V.
Collector current proportional to Base current
The avalanche multiplication of current through
collector junction occurs to be avoided
No current flows
18BJT as Switch
- Vin(Low ) lt 0.7 V
- BE junction not forward biased
- Cutoff region
- No current flows
- Vout VCE Vcc
- Vout High
- Vin(High)
- BE junction forward biased (VBE0.7V)
- Saturation region
- VCE small (0.2 V for saturated BJT)
- Vout small
- IB (Vin-VB)/RB
- Vout Low
19BJT as Switch 2
- Basis of digital logic circuits
- Input to transistor gate can be analog or digital
- Building blocks for TTL Transistor Transistor
Logic - Guidelines for designing a transistor switch
- VCgtVBgtVE
- VBE 0.7 V
- IC independent from IB (in saturation).
- Min. IB estimated from by (IBmin IC/b).
- Input resistance? such that IB gt 5-10 times IBmin
because b varies among components, with
temperature and voltage and RB may change when
current flows. - Calculate the max IC and IB not to overcome
device specifications.
20Operation point of BJT
- Every IB has a corresponding I-V curve.
- Selecting IB and VCE, we can find the operating
point, or Q point. - Applying Kirchoff laws around the base-emitter
and collector circuits, we have - IB (VBB-VBE)/RB
- VCE Vcc ICRC
21Operation point of BJT 2
Load-line curve
Q
22BJT as amplifier
- Common emitter mode
- Linear Active Region
- Significant current Gain
- Example
- Let Gain, b 100
- Assume to be in active region -gt VBE0.7V
- Find if its in active region
23BJT as amplifier 2
VCBgt0 so the BJT is in active region
24Operation region summary
25FET
26Field Effect Transistors
- 1955 the first Field effect transistor works
- Increasingly important in mechatronics.
- Similar to the BJT
- Three terminals,
- Control the output current
27Field Effect Transistors
- Three Types of Field Effect Transistors
- MOSFET (metal-oxide-semiconductor field-effect
transistors) - Enhancement mode
- Depletion mode
- JFET (Junction Field-effect transistors)
- Each in p-channel or n-channel
- The more used one is the n-channel enhancement
mode MOSFET, also called NMOS
28MOSFET (enhancement mode n-channel)
The arrow head indicates the direction of the pn
substrate-channel junction
- N-channel gt Source and Drain are n type
- Enhancement mode gt
- Increase VGS to make the travel from D to S
easier for the electrons
29NMOS Behavior
VGS gt Vth 0 lt VDS lt VPinch off
Depletion mode (or active region), gate holes are
repelled. ? variable resistor (controled
by VGS)
VDS gt VPinch off Inversion mode (or saturation
region), IDS constant.
VDS gt VBreakdown IDS increases quickly Should be
avoided
30NMOS Characteristic
31NMOS Vs PMOS
32NMOS Vs PMOS
VGS lt Vth 0 lt VDS lt VPinch off
Depletion mode (or active region), gate holes are
repelled. ? variable resistor (controled
by VGS)
VDS gt VPinch off Inversion mode (or saturation
region), IDS constant.
Analogous to the pnp BJT
VDS gt VBreakdown IDS increases quickly Should be
avoided
33NMOS uses
- High-current voltage-controlled switches
- Analog switches
- Drive DC and stepper motor
- Current sources
- Chips and Microprocessors
- CMOS Complementary fabrication
34NMOS Example
35JFET overview
36JFET Behavior
Can be used with VG0
37JFET Behavior
Can be used with VG lt 0
38JFET Behavior
VGS lt Vth 0 lt VDS lt VPinch off
Depletion mode (or active region), gate holes are
repelled. ? variable resistor (controled
by VGS)
VDS gt VPinch off Inversion mode (or saturation
region), IDS constant.
Analogous to the pnp BJT
VDS gt VBreakdown IDS increases quickly Should be
avoided
39JFET uses
- Small Signal Amplifier
- Voltage Controlled Resistor
- Switch
40FET Summary
- General
- Signal Amplifiers
- Switches
JFET For Small signals Low noise
signals Behind a high impedence system
Inside a good Op-Ampl.
MOSFET Quick Voltage Controlled
Resistors RDS can be really low 10 mOhms
41Power Transistors
- In General
- Fabrication is different in order to
- Dissipate more heat
- Avoid breakdown
- So Lower gain than signal transistors
- BJT
- essentially the same as a signal level BJT
- Power BJT cannot be driven directly by HC11
- MOSFET
- base (flyback) diode
- Large current requirements
42References
- Introduction to Mechatronics and Measurement
Systems by D.G. Alciatore, McGraw-Hill - Microelectronics by J. Millman, McGraw-Hill
- Several Images from Internet some websites are
- http//www.engr.colostate.edu/dga/mechatronics/fi
gures/ - http//www.ecse.rpi.edu/schubert/Course-ECSE-6290
SDM-2/ - http//hyperphysics.phy-astr.gsu.edu/hbase/solids/
diod.html