Transcript Slide 1

ME 6405 Mechatronics
In Order of Presentation:
Jonathan Jobe
David Malphurs
Isaac Penny
October 11, 2005
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Contents
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Brief History
Properties of Transistors
Types of Transistors
Characteristics and Applications
Engineering Selection
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History
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Vacuum Tube
1879
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Edison Invents Light Bulb
1883
Edison found that he could detect electrons
flowing through the vacuum from the lighted filament to a
metal plate mounted inside the bulb. “Edison Effect”
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John Fleming implements Edison Effect as first diode.
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1906
Lee DeForest introduced a third electrode
called the grid into the vacuum tube. The resulting triode
could be used as both an amplifier and a switch.
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Predecessors
Diode
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Triode
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First Transistors
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Bell Labs
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1947 Invented First Transistor
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Application: replace vacuum tubes
Smaller, more durable, no warm up
Made of Germanium
Current Transistors
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Silicon based
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Doped with phosphorus (n-type)
Doped with boron (p-type)
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The PN Junction
 Forward Biasing
 The external Voltage
lowers the potential barrier at
the junction, allowing the
electrons to flow.
 Reverse Biasing
 The external voltage raises
the potential barrier at the
junction, preventing electrons
from flowing.
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Transistor Types
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BJT
Bipolar Junction Transistor
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FET
Field Effect Transistor
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JFET
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MOSFET (Metal Oxide Semiconducting FET)
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(Junction FET)
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BJTs
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2 types
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NPN
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(most common)
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When IB≠0, VCE
forward biased & VBC
NPN bipolar junction transistor
reverse biased
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PNP
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When IB≠0, VCE
reverse biased & VBC
forward biased
PNP bipolar junction transistor
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npn-B J T Voltage Characteristic
Cutoff: Base-Emitter starts to conduct with VBE=0.6V
Saturation: Increasing IB causes IC to rise exponentially.
Active:
IC    I B
Breakdown: Ic approaches infinity due to breakdown at both junctions
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B J T Operational Characteristics
Operation IB or VCE
Region
Char.
Cutoff
IB = Very
small
Saturation VCE = Small
Active
Linear
Breakdown
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VCE & VBE
Junctions
Reverse &
Reverse
Forward &
Forward
VCE =
Reverse &
Moderate
Forward
VCE = Large Beyond
Limits
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Mode
Open
Switch
Closed
Switch
Linear
Amplifier
Overload
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Equations of npn-B J T s
Definitions
VBE  VB  VE
VCE  VC  VE
Kirchoff’s Current Law
IE  IB  Ic
In Active region
IC    IB
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Common values for
ß are 20 to 200
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Point of Operation
The existence of RC means that
IC and VCE are no longer
independent.
VCE = Vcc – IC*RC
After solving for IC,
VCC VCE
IC 

RC RC
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Point of Operation
Load-line constraint
IC 
VCC VCE
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RC RC
Selecting VBB and VCC, we
can find the operating
point, or Q point.
IB = (VBB-VBE)/RB
Q point for IB=100μA
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B J T resistor sizing
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ß and IC,max are specified by the catalog
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We need to choose Values for RB and RC to keep IC
and IB within specifications
IB 
IC
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VCC
RC 
IC
VBB VBB 
RB 
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IB
IC
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Field Effect Transistors (FET)
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Three Types of Field Effect Transistors
 MOSFET (metal-oxide-semiconductor field-effect transistors)
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Enhancement mode IDS α VGS
Depletion mode IDS α 1/VGS
JFET (Junction Field-effect transistors)
Available in n or p Channel
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n-Channel activated by VGS > 0 for MOSFET and VGS < 0 for JFET
p-Channel activated by VGS < 0 for MOSFET and VGS > 0 for JFET
Most Common Types
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n-Channel Enhancement Mode MOSFET (NMOS)
n-Channel JFET
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FET Architecture
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Enhanced MOSFET
Conducting
Region
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Depleted MOSFET
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JFET
Nonconducting
Region
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Analogous BJT Terminals
Nonconducting
Region
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BJT
FET
Base
Gate
Collector
Drain
Emitter
Source
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NMOS Voltage Characteristic
VDS = Constant
VGS < Vth
IDS=0
I DS  I DSSHORT
VGS > Vth :
0 < VDS < VPinch off
 VGS
1 
 VTH
Active Region
IDS controlled by VGS
VDS > VPinch off
Saturation Region
IDS constant
Active
Region
Saturation
Region
VDS > VBreakdown
IDS approaches IDSShort
Should be avoided
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VPinchoff
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2
Junction Field Effect Transistor
Difference
from NMOS
VGS > Vth
IDS=0
I DS  I DSSHORT
VGS < -Vth :
0 < VDS < VPinch off
Active Region
IDS controlled by
VGS
Active
Region
 VGS
1 
 VTH
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2
Saturation
Region
VDS > VPinch off
Saturation Region
IDS constant
VDS > VBreakdown
IDSShort
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IDS approaches
Should be
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Transistor Selection
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Applications of Transistors
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Switch
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Voltage Amplifier
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Current Amplifier
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Transistor as a Switch
Many times you just need to switch a
signal on or off
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Ex. Digital Logic, LED’s, PWM
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Relays can perform this same function
They can usually handle higher currents
than can transistors
Not Solid State, so shorter life and less
durable
Slower activation time
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Transistor as a Voltage Amplifier
Other times you want to
amplify an analog signal
Ex. Sensor input, audio,
Op-amps can perform the same
function
Higher gains
Can’t handle nearly as much
current.
Thus Op-amps are better for
signal amplification, while
Transistors are better for power
amplification.
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Transistor as a Current Amplifier
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Other times you want to
amplify an analog signal
Ex. Sensor input, audio,
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Op-amps can perform the
same function
Higher gains
Can’t handle nearly as much
current.
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Thus Op-amps are better for
signal amplification, while
Transistors are better for
power amplification.
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Example Problem
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Refer to your first handout
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Questions
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Refer to your second handout
Candy!!
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