Diodes, Triodes, Thermistors, Opto
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Transcript Diodes, Triodes, Thermistors, Opto
Diodes, Triodes,
Thermistors, Opto-isolators,
& Phototransistors
ME 6405 – Spring 2005
Danny Nguyen
Wei Tan
Qiulin Xie
Presentation Outline
Diodes – Danny
Triacs & Thermistors – Qiulin
Opto-isolators & Phototransistors – Wei
Diodes: Overview
Meet the Diode
Junction Diodes
Analysis and Applications
Zener Diodes and Applications
What is a Diode?
Simplest semiconductor device
Allows current to flow in one direction but
not the other
Symbols:
Schematic
+ VD −
Internal View
Anode
Cathode
p
ID
n
Junction Diodes
Start out with Silicon or Germanium
(Group IV elements)
P-type - doping with Group III elements
Boron, Aluminum,
Gallium
Adds positive ‘holes’ to the region
N-type - Group V doping
Phosphorous, Arsenic
Add
electrons to the region
+
+
+
p
+
+
+
−
+
−
+
−
−
n
−
−
−
−
Junction Diodes
Due to thermal energy, some electrons
diffuse into the p-type region, creating a
depletion region
+
+
+
+
−
p
n
+
−
−
−
−
Depletion Region
No current flows through the diode at this
point
Junction Diodes
Forward Bias
Depletion
region decreases
Current flow when voltage is high enough
(0.6-0.7 Volts)
Current sustained by majority carriers
VD
ID
+
+
+
+
p
+
+ −
+ −
+ −
−
n
−
−
−
−
Junction Diodes
Reverse Bias
Depletion
region increases
Small leakage current by minority carriers
Reverse saturation current (I0)
On the order of 10-9 to 10-15 A
VD
+ +
+ p
+ +
− −
n −
− −
Analysis of Diodes
Mathematical Model
qVD ¡
I
=
I
[exp(
) 1]
D
0
kT
Ideal Model
·0
V
=
0;
I
>
0
I
=
0;
V
D
D
D
On:
Off: D
ID
Constant Voltage Drop Model
VD = Von ; ID > 0
On:
·V
Ideal
CVD
I
=
0;
V
D
D
on
Off:
» 0:7V
VD
V
=
0:6
on
V
Diode Eq.
on
Analysis and Applications
Half-wave rectifier
+ VD −
Vi = 5VAC
ID
1kΩ
Vo
Von = 0.7V
CVD Analysis:
On:
Replace diode with Von voltage source
Off: Replace diode with open circuit
Analysis and Applications
Half-wave rectifier
Von
Vi = 5VAC
ID
1kΩ
Vo
Von = 0.7V
CVD Analysis:
! V = V ¡ 0:7V
V
>
0:7V;
I
>
0
D
o
i
On: i
Off:
Analysis and Applications
Half-wave rectifier
Vi = 5VAC
1kΩ
Vo
CVD Analysis:
! V = V ¡ 0:7V
V
>
0:7V;
I
>
0
D
o
i
On: i
· 0:7V; I = 0 ! V = 0V
V
i
D
o
Off:
Analysis and Applications
Full-wave bridge rectifier
Vi
Vo
Peak Detector
Vi
Vo
Zener Diodes
Operated by reverse bias instead of
forward bias
All diodes have a breakdown region –
point where the diode can not handle
anymore negative voltage
Voltage remains nearly constant in the
breakdown region (Vz: Zener Voltage)
under widely varying current for Zeners
Zener Diodes: I-V Graph
Slope = 1/Rz
Schematic
− VZ +
+ VD −
IZ
ID
Reverse Breakdown
Model
VZ
RZ
IZ
Zener Diodes: Applications
Ability to maintain a constant voltage
allows it to act as a voltage regulator
R
Vi
Iz
Vo = Vz
RL
Vz = 6:2V; R = 1k ; RL = 10k ; Vi = 7 » 11V
Zener Diodes: Specifications
VZ (Zener Voltage): Common range is
between 3.3V and 75V
Tolerance: Commonly 5 to 10%
Power Handling: ¼, ½, 1, 5, 10, 50 W
Contents
Shockley Diode
Silicon-Controlled Rectifier (SCR)
Triac
Thermistor
Shockley Diode
Shockley diode after its
inventor, William
Shockley
four-layer diode, also
known as a PNPN
on if applying sufficient
voltage between anode
and cathode
Off if reducing to a much
lower voltage
Silicon-Controlled Rectifier (SCR)
Shockley diode becomes SCR if gate addition to
PNPN
it behaves exactly as a Shockley diode If an SCR's
gate is left disconnected.
gate terminal may be used as an alternative means
to latch the SCR
SCRs are unidirectional (one-way) current devices,
making them useful for controlling DC only
Triode AC Switch (Triac)
A triac can be regarded as a "bidirectional (AC) SCR” because it conducts in
both directions.
•
5 layer device
•
Region between MT1 and MT2 are parallel switches (PNPN and NPNP)
•
Allows for positive or negative gate triggering
Triggering Quadrant
Triac Characteristic Curve
Triac Characteristic Curve
VDRM refers to the maximum peak forward voltage which may be continuously
applied to the main terminals and the highest voltage that can be blocked
IDRM is the leakage current of the Triac when VDRM is applied to MT1 and MT2 ,
which is several orders of magnitude smaller than the “on” rating
VRRM: Peak Repetitive Reverse Voltage
Maximum peak reverse voltage that may be continuously applied to the main
terminals
IGT Gate trigger current
VGT Gate trigger voltage
Latching Current: the value of on-state current required to maintain conduction
at the instant when the gate current is removed
Holding current :Value of on-state current required to maintain conduction once
the device has fully turned on and the gate current has been removed. The onstate current is equal to or lower in value than the latching current
Triac Advantages and Applications
Advantages
Controllable trigger
Four quadrant device
Triacs provide the lowest cost
and simplest route to reliable,
interference-free switching
and power control.
Application
Light dimmer control
Motor speed control (a phasecontrol circuit is used to vary
the power to brush motors.)
Reason
Trigger pulse can control any
percentage of half cycle
Thermistor
Thermistor - Temperature sensitive resistor
Their change in electrical resistance is very large and
precise when subjected to a change in temperature.
Thermistors exhibit larger parameter change with
temperature than thermocouples and Resistance
Temperature Detectors (RTD’s).
Thermistor - sensitive
Thermocouple - versatile
RTD – stable
Generally composed of semiconductor materials.
Very fragile and are susceptible to permanent
decalibration.
Thermistor Probe
One of many available probe assemblies
Thermistor Characteristics
Most thermistors have a negative temperature
coefficient (NTC); that is, their resistance
decreases with increasing temperature.
Positive temperature coefficient (PTC)
thermistors also exist with directly proportional R
vs. T.
Extremely non-linear devices (high sensitivity)
Common temperature ranges are –100 °F (~-75
°C) to +300 °F (~150 °C)
Some can reach up to 600 °F
Thermistor R-T Curve
An individual thermistor curve can be very
closely approximated by using the SteinhartHart equation:
T = Degrees Kelvin
1
T
= A
B ln( R)
3
C ln( R)
R = Resistance of
the thermistor
A,B,C = Curve-fitting
constants
V or R
• Typical Graph
Thermistor (sensible)
RTD (stable)
T
Thermocouple
(versatile)
Thermistor Applications
Temperature Control
variable resistor
for setting
desired
temperature
relay
thermistor
high gain
amplifier
•Resistor is set to a desired
temperature (bridge
unbalance occurs)
•Unbalance is fed into an
amplifier, which actuates a
relay to provide a source of
heat or cold.
•When the thermistor
senses the desired
temperature, the bridge is
balanced, opening the relay
and turning off the heat or
cold.
Phototransistor
Introduction
Package and Scheme
Operation
Advantages
Example and applications
Phototransistor Introduction
A transistor which is sensitive to the input
light intensity
Operation similar to traditional transistors;
Have collector, emitter, and base
Phototransistor base is a light-sensitive
collector-base junction
Dark Current: Small collector can emit
leakage current when transistor is
switched off.
Phototransistor Packages
Phototransistor Scheme
Photocurrent: The electrons are amplified by the
transistor and appear as a current in the collector/emitter
circuit.
The base is internally left open and is at the focus of a
plastic lens.
Phototransistor Operation
The phototransistor must be
properly biased
A light sensitive collector base
p-n junction controls current
flow between the emitter and
collector
As light intensity increases,
resistance decreases, creating
more emitter-base current
The small base current
controls the larger emittercollector current
Collector current depends on
the light intensity and the DC
current gain of the
phototransistor
Why Use Phototransistors?
More sensitive than photodiodes of
comparably sized area
Available with gains form 100 to over 1500
Moderately fast response times
Available in a wide range of packages
Usable with almost any visible or near
infrared light source such as IREDs, lasers,
sunlight, and etc
Same general electrical characteristics as
familiar signal transistors
Application Example: Avoiding
Obstacles
Automated
Cart
LED
Baffle
Phototransistor
Obstacle
Phototransistor Applications
Computer/Business Equipment
protect control – floppy driver
Margin controls – printers
Write
Industrial
light source – light pens
Security systems
LED
Consumer
Coin
counters
Lottery card readers
Optoisolator
Introduction
Scheme and Package
Optocoupler Interrupter Example
Advantages and applications
Optoisolator Introduction
A device that uses a short
optical transmission path
to accomplish electrical
isolation between
elements of a circuit.
Note 1: The optical path may be air or a dielectric
waveguide;
Note 2: The transmitting and receiving elements may
be contained within a single compact module.
Optoisolator Scheme
The light emitted form the LED is detected by a
photodetector which sits across from the LED inside the
chip, and output a current.
Since the input signal is passed from the LED to the
photodetector, and cannot be passed form the
photodetector to the LED, the input device is optically
isolated from the circuit connected to the output side.
Optoisolator Package
An IRED is typically a controllable light source
and a phototransistor employs as the detector
element.
The
input and output sides have separate grounds
Optoisolators sensitive to input voltages.
Optocoupler Interrupter Example
Integrated emitter and detector pair
Setup Similar to Lab L3
Used to calculate speed or distance
Optoisolator Advantages & Applications
Advantages
Output
signals have no effect on input
High reliability and high efficiency
Noise isolation
Small size
Applications
Optical
switch
Signal transmission devices
Used to control motors, solenoids, etc.
Questions?
References
“Introduction to Mechatronics and Measurement
Systems, 2nd Ed.” by D.G. Alciatore and M.B.
Histand
http://www.semiconductors.philips.com
http://www.omega.com
“Microelectronic Circuit Design, 1st Ed.” by
Richard C. Jaeger
Fall 2000 Slides