Class 3: The Fundamentals of Designing with Semiconductors
1. The World Leader in High Performance Signal Processing Solutions
THE FUNDAMENTALS OF DESIGNING WITH
SEMICONDUCTORS FOR SIGNAL
PROCESSING APPLICATIONS
Class 3 - BEYOND THE OP AMP
Presented by David Kress
2. Analog to Electronic signal processing
Sensor Amp Converter Digital Processor
(INPUT)
Actuator Amp Converter
(OUTPUT)
3. Analog to Electronic signal processing
Sensor Amp Converter Digital Processor
(INPUT)
Actuator Amp Converter
(OUTPUT)
4. Amplifiers and Operational Amplifiers
Amplifiers
Make a low-level, high-source impedance signal into a high-
level, low-source impedance signal
Op amps, power amps, RF amps, instrumentation amps, etc.
Most complex amplifiers built up from combinations of op
amps
Operational amplifiers
Three-terminal device (plus power supplies)
Amplify a small signal at the input terminals to a very, very
large one at the output terminal
5. Specialty Amplifiers
Specialty Amplifiers
Designed for a specific signal type
Extract and amplify only the signal of interest
Pick off a small differential signal from a large common-mode
voltage
Capture and demodulate a low-level AC signal
Compress a high-dynamic range signal
Provide automatic or controlled gain-changing
Send and receive precision signals
Provide high-speed low-impedance power output
Use the analog domain to its best advantage to prepare a clean
signal for the data converter
6. Specialty Amplifier Types
General Inst. Amps.
Differential Amps.
Current-sense Amps.
Programmable gain
Demodulating amps (AD630 and AD698)
Thermocouple amps
Logarithmic amps with time-gain-control
ADC drivers
Clamp amps
Funnel amplifier
Line drivers/receivers
Isolation amps
7. Single-ended vs. Differential Signals
Single-ended signals
Signalis measured referred to ground
When signals are bipolar (+ and-), negative supplies needed
AC signals are typically bipolar or need special ‘floating’, or
capacitive coupling
Ground often carries high noise from other signals or power,
compromising the signal
Differential signals
Both sides of the signal float ‘off ground’
Signals are separated from ground and other signals
High frequency and accuracy usually need differential handling
Common mode (average) can be set for single supply
Specialized differential/difference amplifiers are needed
8. Instrumentation, Difference and
Differential Amplifiers
Instrumentation amplifiers
Amplify differential inputs to a single-ended output
Normally both amplifier inputs are high impedance
Provide high gain (up to 10,000) and low noise
Normally handle low-level signals from sensors
Difference amplifiers
Amplify differential inputs from high common mode voltage levels
Often include input attenuator to allow operation outside supplies
High common model rejection even at high frequencies
Differential amplifiers
High frequency amplifiers with differential input and output
Handle higher-level signals at lower gains
Typically used for line driving/receiving and ADC driving
9. The Generic Instrumentation Amplifier
(In Amp)
RS/2 RS
RG
+
COMMON
MODE
VOLTAGE
~ VSIG +
_ 2
VCM
IN-AMP
GAIN = G
+
VSIG _ VOUT
VREF
~
~ _
2
~
RS/2
VCM
COMMON MODE ERROR (RTI) =
CMRR
10. Op Amp Subtractor or Difference Amplifier
R1 R2
V1
_
VOUT
R2
1+
R1
CMR = 20 log10
+ Kr
R1' R2' REF
V2 Where Kr = Total Fractional
Mismatch of R1/ R2 TO
R2 R1'/R2'
VOUT = (V2 – V1)
R1
R2 R2'
= CRITICAL FOR HIGH CMR
R1 R1'
EXTREMELY SENSITIVE TO SOURCE IMPEDANCE IMBALANCE
0.1% TOTAL MISMATCH YIELDS 66dB CMR FOR R1 = R2
11. The Three Op Amp In Amp
+
+ R2' R3'
VSIG
A1
~
2 _ _
_
VCM R1' VOUT
RG A3
R1
~ +
+ _
VSIG R2 R3
~ VREF
2 A2
_
2R1
+ VOUT = VSIG • R3 1 + + VREF
R2 RG
GAIN × 100 2R1
CMR 20log IF R2 = R3, G = 1 +
RG
% MISMATCH
12. GENERALIZED BRIDGE AMPLIFIER USING
AN IN-AMP
VB
R+R +VS
R–R R
VOUT = VB GAIN
R
-
RG IN AMP
REF VOUT
+
R–R
R+R -VS
13. AD620B Bridge Amplifier DC Error Budget
+10V 499 MAXIMUM ERROR CONTRIBUTION, +25°C
VCM = 5V FULLSCALE: VIN = 100mV, VOUT = 10V
RG
+ VOS 55µV ÷ 100mV 550ppm
AD620B IOS 350 × 0.5nA ÷ 100mV 1.8ppm
Gain Error 0.15% 1500ppm
– REF
Gain 40ppm 40ppm
G = 100
Nonlinearity
350100mV FS
LOAD CELL CMR Error 120dB
1ppm × 5V ÷ 100mV 50ppm
AD620B SPECS @ +25°C, ±15V 0.1Hz to 10Hz
280nV ÷ 100mV 2.8ppm
VOSI + VOSO/G = 55µV max 1/f Noise
IOS = 0.5nA max
Total
Gain Error = 0.15% Unadjusted 9 Bits Accurate 2145ppm
Gain Nonlinearity = 40ppm Error
0.1Hz to 10Hz Noise = 280nVp-p
Resolution 14 Bits Accurate 42.8ppm
CMR = 120dB @ 60Hz
Error
16. AD8251/53 Digitally Programmable Gain
Instrumentation Amplifier (PGIA)
AD8251 Fine Gain Setting of 1,2,4,8
AD8253 Coarse Gain Setting of 1,10,100,1000
Low noise and low offset with 10MHz bandwidth
+VS DGND WR A1 A0
2 6 5 4
-IN
LOGIC
–IN 1
A1
-
7 OUT
A1 Gain Logic A3 OUT
A2
+
+IN 10
A2
+IN
AD8253
06983-001
8 3 9
-VS REF +VS –VS REF
AD8251 AD8253
17. Demodulating Amplifiers
AC demodulation
Low-level low-frequency AC signal processing can be used for
capturing low-level signals
A modulated signal bypasses issues of offset and noise in
amplifiers
Useful for transformer-coupled position detectors
Lock-in amplifier can find narrow band signal 100db below the
interfering noise
18. IMPROVED LVDT OUTPUT SIGNAL
PROCESSING
ABSOLUTE
+ FILTER
VALUE
+ VOUT
AC
~ _
SOURCE
ABSOLUTE
_ FILTER
VALUE
LVDT
+ VOUT
_ POSITION +
_
19. Lock-in Amplifier
AD630 demodulates 400Hz signal 100dB below noise
CLIPPED
C
BAND-LIMITED
WHITENOISE AD630
B 16 5k
100R
15 10k
AD542
1 2.5k AD542
20 A 13 R
19
17 2.5k B
100dB 100R
ATTENUATION 14 10k
C OUTPUT
A
10 LOW-PASS
0.1Hz 9 FILTER
MODULATED
400Hz CARRIER
CARRIER PHASE
REFERENCE
20. Thermocouple Amplifiers
Cold junction compensation
Thermocouples use two different metals that develop a voltage
varying with temperature
The temperature effect also occurs at the point where the
thermocouple wires connect to the instrument
This ‘cold junction’ effect must be compensated for to get accurate
measurements
Various techniques have been used including ice baths
Modern thermocouple amplifiers include accurate compensation
circuitry
21. Using a Temperature Sensor for Cold-
Junction Compensations
V(OUT) TEMPERATURE
V(COMP) COMPENSATION
CIRCUIT
COPPER COPPER
METAL A SAME METAL A
TEMP TEMP
SENSOR
T1 V(T1) V(T2) T2
METAL B
V(COMP) = f(T2)
ISOTHERMAL BLOCK
V(OUT) = V(T1) – V(T2) + V(COMP)
IF V(COMP) = V(T2) – V(0°C), THEN
V(OUT) = V(T1) – V(0°C)
22. AD594/AD595 Monolithic Thermocouple
Amplifier with Cold-Junction Compensation
+5V
0.1µF BROKEN
4.7k THERMOCOUPLE VOUT
ALARM 10mV/°C
OVERLOAD
TYPE J: AD594 DETECT
TYPE K: AD595
THERMOCOUPLE AD594/AD595 +A
– – –TC
ICE
G + G POINT
+ + COMP
+TC
23. Log Amplifiers
Signal compression
Many applications must capture signals over a very wide dynamic
range
Radio antennas capturing broadcast signals
Photomultipliers and photodiodes capture light signals over a very
wide range
To process and use these signals, they need to be compressed to
a much smaller range
Logarithmic amplifiers
Log amplifiers compress signals over ranges of as much as 120db
– a million to one -- to a normal range of 1 to 10 volts
Accuracy is typically 0.1 to 0.5 dB -- 1 to 5%
24. Log Amp Transfer Function
VYLOG (VIN/VX)
IDEAL
ACTUAL
2VY
SLOPE = VY
VY VIN
VOUT = VY log10
VX
+
0
ACTUAL VIN=10VX VIN=100VX INPUT ON
VIN=VX
- IDEAL LOG SCALE
26. AD8307 six-decade RF power
measurement
TO
ANTENNA
100kΩ 0.1µF
1/2W VP
22Ω
51pF +5V
NC
8 7 6 5
VR1 LEAD-
INP VPS ENB INT THROUGH
2kΩ
AD8307 CAPACITORS,
INT ±3dB
1nF
50Ω INPUT INM COM OFS OUT
FROM P.A. 604Ω
1 2 3 4
1µW TO 2kΩ
1kW NC VOUT
51pF 1nF OUTPUT
NC = NO CONNECT
27. Time-gain-control with AD8335
Ultrasound processor changes AD8335 gain to account
for changes in signal strength with tissue depth
TX HV AMPs
TX BEAMFORMER BEAMFORMER
CENTRAL CONTROL
MULTICHANNEL
TGC USES MANY VGAs
HV
AD8335 VGAs
T/R Rx BEAMFORMER
MUX/ SWITCHES LNAs
DEMUX (B AND F MODES)
TRANSDUCER TGC
ARRAY TIME GAIN COMPENSATION
128, 256 ETC.
ELEMENTS CW (ANALOG)
BIDIRECTIONAL BEAMFORMER SPECTRAL IMAGE AND COLOR
CABLE DOPPLER MOTION DOPPLER (PW)
PROCESSING PROCESSING PROCESSING
MODE (B MODE) (F MODE)
AUDIO DISPLAY
OUTPUT
28. ADC driver amplifiers
High performance ADCs
Recent high performance ADCs have 16-bits and more at 200MSPS
and higher
Such performance requires a differential input signal
Differential amplifiers
Differential
or single-ended input converted to differential output
Low impedance output stage rejects ADC switching spikes
Common mode level set and gain setting allow optimum match to
ADC range
30. ADC Input Clamp Amplifiers
Imaging systems
Ultrasound and imaging systems often exhibit high-level
transients in practice
Input signals can easily exceed supply and ADC input range
Long recovery times can impair image stability
Clamp amplifiers
Clamp amplifiers capture and suppress input transients
Amplifier output does not exceed ADC range
Transient recovery takes a few nanoseconds
31. AD8036/AD8037 Clamp Amplifier Equivalent
Circuit
RF
14 0
-V IN +
A1 A2 VOUT
A - +1
+VIN +1
S1
VH B
+1
VL C S1 A B C
+1
V IN > V H 0 1 0
+
CH V L V IN V H 1 0 0
-
V IN < V L 0 0 1
+
CL
-
36. Video Difference Amplifier with Variable
Common
AD830 allows different input and output common mode
voltage for matching ADC input range
VP
0.1µF
V1 1 AD830 8
INPUT GM
SIGNAL VOUT
V2 2 7
INPUT A=1
COMMON
3 6
GM C 0.1µF
4 5
VN
V3
VOUT = V1 – V2 + V3 OUTPUT
COMMON
37. APPLICATIONS FOR ISOLATION
AMPLIFIERS
Sensor is at a High Potential Relative to Other
Circuitry
(or may become so under Fault Conditions)
Sensor May Not Carry Dangerous Voltages,
Irrespective of Faults in Other Circuitry
(e.g. Patient Monitoring and Intrinsically Safe
Equipment for use with Explosive Gases)
To Break Ground Loops
38. AD210 3-PORT ISOLATION AMPLIFIER
FB INPUT OUTPUT
T1
–IN _
DEMOD
_
MOD VO
+ FILTER +
+IN
ICOM OCOM
T2 POWER T3
+VISS INPUT OUTPUT +VOSS
POWER POWER
–VISS SUPPLY SUPPLY –VOSS
POWER
OSCILLATOR
PWR PWR COM
39. AD210 ISOLATION AMPLIFIER KEY
FEATURES
Transformer Coupled
High Common Mode Voltage Isolation:
2500V RMS Continuous
±3500V Peak Continuous
Wide Bandwidth: 20kHz (Full Power)
0.012% Maximum Linearity Error
Input Amplifier: Gain 1 to 100
Isolated Input and Output Power Supplies,
±15V, ±5mA
40. MOTOR CONTROL CURRENT SENSING
HIGH VOLAGE
AC INPUT < 2500V RMS
+15V FB INPUT OUTPUT
T1
+ –IN _ _ OUTPUT
DEMOD
MOD VO
+IN + FILTER
AD620 +
0.01 RG OCOM
REF ICOM
_
–15V
+VISS T2 POWER T3
INPUT OUTPUT +VOSS
–VISS POWER POWER
SUPPLY SUPPLY –VOSS
RG = 499 POWER
M FOR G = 100 AD210 OSCILLATOR
PWR PWR COM
+15V
41. Fundamentals Webcasts 2011
January Introduction and Fundamentals of Sensors
February The Op Amp
March Beyond the Op Amp
April Converters, Part 1, Understanding Sampled Data Systems
May Converters, Part 2, Digital-to-Analog Converters
June Converters, Part 3, Analog-to-Digital Converters
July Powering your circuit
August RF: Making your circuit mobile
September Fundamentals of DSP/Embedded System design
October Challenges in Industrial Design
November Tips and Tricks for laying out your PC board
December Final Exam, Ask Analog Devices
www.analog.com/webcast
42. Next webcasts
Challenges in Embedded Design for Motor Control systems
April 13th at Noon (EDT)
MEMs solutions for Instrumentation applications
May 18th at Noon (EDT)
Multi-Parameter Vital Signs Patient Monitors
June 22nd at Noon (EDT)
www.analog.com/webcast
43. The World Leader in High Performance Signal Processing Solutions
Thank You
Editor's Notes
In the first seminar, we discussed the issues of capturing physical variables, which are not electronic, into electronic format through sensors. Sensors provide weak, difficult to handle signals. Amplifiers pick those signals off the sensors and amplify them to make it easier to use them in the whole system.
In this session and the next, we will cover amplifiers. Today we will talk about op amps, the fundamental building block for most of analog circuitry. In the next session, we will build up these op amps into more complex amplifiers and other devices for processing signals in the analog domain. These amplifiers will prepare the signals for digitizing in the ADC stage.
As you increase the gain, the noise gain line moves up and the usable bandwidth goes down.
A series of thermocouple amplifiers is available from Analog Devices so you can find the right accuracy and operating temperature range for your needs. These products use very little power, less than 1mW, and are in a small MSOP package. Two of the important things to look at when using a thermocouple amplifier are the initial accuracy and the temperature range where the amplifier is accurate. This is the temperature of the board that the amplifier is on, not the temperature of the thermocouple itself.
As you increase the gain, the noise gain line moves up and the usable bandwidth goes down.
I also want to remind you that every month Analog Devices presents a webcast on a current Hot Topic in designing with Semiconductors. Next month we’ll be presenting a webcast on Challenges in Embedded Design for Motor Control systems, in April we’ll look at MEMs solutions for Instrumentation applications, and in May we’ll tackle multi-parameter vital signs patient monitors. Registration will be available for each about a month before broadcast at www.analog.com slash webcast, where you can also access our library of archived webcasts that you can view anytime, on demand.