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Modern Instrumentation PHYS 533CHEM 620

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Title: Modern Instrumentation PHYS 533CHEM 620


1
Modern InstrumentationPHYS 533/CHEM 620
  • Lecture 4
  • Amplifiers
  • Amin Jazaeri
  • Fall 2007

2
Amplifiers
  • Properties of a perfect amplifier
  • Infinite gain
  • Infinite input impedance
  • will not load down source
  • Zero output impedance
  • will drive anything
  • Infinite CMRR
  • Zero Common mode voltage gain
  • Infinite Bandwidth

3
Operational Amplifiers
  • An operational amplifier is modeled as a voltage
    controlled voltage source.
  • Properties of Op-amps
  • Gain 106
  • Input impedance 100 M W
  • Output impedance 100 W
  • Bandwidth 1-20MHz
  • Common mode voltage gain 10-5

4
Amplifiers
  • Problems
  • Gain too high
  • slightest input noise causes max output
  • Other problems to be discussed later
  • Solutions
  • Use feedback
  • Gain depends only on resistance Rf / Rin
  • can control precisely

5
Applications of Op Amps
  • Amplifiers provide gains in voltage or current.
  • Op amps can convert current to voltage.
  • Op amps can provide a buffer between two
    circuits.
  • Op amps can be used to implement integrators and
    differentiators.
  • Lowpass and bandpass filters.

6
The Op Amp Symbol
High Supply
Non-inverting input
Output
Inverting input
Ground
Low Supply
7
The Op Amp Model
v
Non-inverting input

vo
Rin


Inverting input
A(v -v- )
v-
8
Operational Amplifier (OP-AMP)
  • Basic and most common circuit building device.
    Ideally,
  • No current can enter terminals V or V-. Called
    infinite input impedance.
  • VoutA(V - V-) with A ?8
  • In a circuit V is forced equal to V-. This is
    called the virtual ground property.
  • An opamp needs two voltages to power it Vcc and
    -Vee. These are called the rails.

A
Vo (A V -A V ) A (V - V )

-

-
9
Characters of Operational Amplifiers
  • high open loop gain
  • high input impedance
  • low output impedance
  • low input offset voltage
  • low temperature coefficient of input offset
    voltage
  • low input bias current
  • wide bandwidth
  • large common mode rejection ratio (CMRR)

10
INPUT IMPEDANCE
Input impedance the impedance seen by the sensor
when connected to the op-amp. Typically this
impedance is high (ideally infinite) It varies
with frequency. Typical impedances for
conventional amplifiers is at least 1 M? but it
can be of the order of hundreds of M? for FET
input amplifiers. This impedance defines the
current needed to drive the amplifier and hence
the load it represents to the sensor.
Input Circuit Output
Impedance between input terminals input
impedance
11
OUTPUT IMPEDANCE
Output impedance the impedance seen by the load.
Ideally this should be zero since then the
output voltage of the amplifier does not vary
with the load In practice it is finite and
depends on gain. Usually, output impedance is
given for open loop whereas at lower gains the
impedance is lower. A good amplifier will have
an output resistance lower than 1?.
12
Voltage output
  • The linear range of an amplifier is finite, and
    limited by the supply voltage and the
    characteristics of the amplifier.
  • If an amplifier is driven beyond the linear range
    (overdriven), serious errors can result if the
    gain is treated as a constant.

13
Bandwidth
  • Bandwidth the range of frequencies that can be
    amplified.
  • Usually the amplifier operates down to dc and has
    a flat response up to a maximum frequency at
    which output power is down by 3dB.
  • An ideal amplifier will have an infinite
    bandwidth.
  • The open gain bandwidth of a practical amplifier
    is fairly low
  • A more important quantity is the bandwidth at the
    actual gain

14
Bandwidth
15
Temperature Noise
  • Temperature and noise refer to variations of
    output with temperature and noise characteristics
    of the device respectively.
  • These are provided by the data sheet for the
    op-amp and are usually very small.
  • For low signals, noise can be important while
    temperature drift, if unacceptable must be
    compensated for through external circuits.

16
Signal Conditioning
External Power

Filter
Motor, Speaker, Alarm etc.
Amp
Transducer
-
17
Op-Amp (Analysis)
  • The key to op amp analysis is simple
  • No current can enter op amp input terminals.
  • gt Because of infinite input impedance
  • The ve and ve (non-inverting and inverting)
    inputs are forced to be at the same potential.
  • gt Because of infinite open loop gain
  • Use the ideal op amp property in all your
    analysis.

18
What is inside an op-amp
19
Inverting Amplifier
20
Analysis of Inverting Amplifier
Ideal transfer characteristics
21
Inverting op-amp
  • The output is inverted with respect to the input
    (180? out of phase).
  • The feedback resistor, Rf, feeds back some of
    this output to the input, effectively reducing
    the gain.
  • The gain of the amplifier is now given as

In the case shown here this is exactly 10
22
Inverting op-amp
  • The input impedance of the amplifier is given as

Here it is equal to 1 k?. If a higher resistance
is needed, larger resistances might be needed
Or, perhaps, a different amplifier will be
needed (noninverting amplifier)
23
Inverting op-amp
  • The output impedance of the amplifier is given as

AOL is the open loop gain as listed on the data
sheet Open loop gain is the open loop gain at
the frequency at which the device is operated
24
Inverting op-amp
  • Example, for the LM741 amplifier, the open loop
    output impedance is 75W and the open loop gain at
    1 kHz is 1000. This gives an output impedance of

The bandwidth is also influenced by the feedback
25
Non-Inverting Amplifier
26
Non-inverting amplifier
  • The non-inverting amplifier gain is

For the circuit shown, this is 11 The gain is
slightly larger than for the noninverting
amplifier for the same values of R. The main
difference however is in input impedance.
27
Non-inverting amplifier
  • Input impedance is

Rop is the input impedance of the op-amp as given
in the spec sheet Aol is the open loop gain of
the amplifier. Assuming an open loop impedance
of 1 M? (modest value) and an open loop gain of
106, we get an input impedance of 1011 ?.
(almost ideal)
28
Non-inverting amplifier
  • The output impedance and bandwidth are the same
    as for the inverting amplifier.
  • The main reason to use a noninverting amplifier
    is that its input impedance is very large making
    it almost ideal for many sensors.
  • There are other properties that need to be
    considered for proper design such as output
    current and load resistance but these will be
    omitted here for the sake of brevity.

29
The voltage follower
30
Voltage follower
  • The input impedance now is very large and equal
    to

The output impedance is very small and equal to
31
Voltage follower
  • The value of the voltage follower is to serve in
    impedance matching.
  • One can use this circuit to connect, say, a
    capacitive sensor or, an electronic microphone.
  • If amplification is necessary, the voltage
    follower may be followed by an inverting or
    noninverting amplifier

32
Differential Amplifier
  • Op amp output actually depends on voltage
    difference at two inputs
  • Insensitivity to common voltage at both inputs
    CMRR
  • Real op amps have problems with unbalanced input
    impedance

33
Differential Amplifier
Redefine the inputs in terms of two other
voltages 1. differential mode input vdm ? vb
va 2. common mode input vcm ? (va vb)/2 so
that va vcm (vdm/2) and vb vcm
(vdm/2) Then it can be shown that
common mode gain
differential mode gain
34
Differential Amplifier
  • An ideal differential amplifier amplifies only
    the differential mode portion of the input
    voltage, and eliminates the common mode portion.
  • provides immunity to noise (common to both
    inputs)
  • If the resistors are not perfectly matched, the
    common mode rejection ratio (CMRR) is finite

35
SUMMING AMPLIFIER
Recall inverting amplifier and If I1
I2 In
If
VOUT -Rf (V1/R1 V2/R2 Vn/Rn) If
R1R2Rf, then Vout V1 V2 Vn
Summing amplifier is a good example of analog
circuits serving as analog computing amplifiers
(analog computers)! Note analog circuits can
add, subtract, multiply/divide (using logarithmic
components, differentiat and integrate in real
time and continuously.
36
Frequency Response
37
Circuit building Tips
Vcc15V
Signal
1) Pin numbers on the circuit diagram
R2
R1
Eg.
R2
2
7
-
R1
3
8
7
6
5
6

4
To Oscilloscope
741
Gnd
2) Use color coding
1
2
3
4
3) Use power strips

4) Separate components from chip - use
insulated wire back to chip 5) Scope probes - to
scope (ground) BNC cable - from signal
generator 6) Build and check in sections
-Vcc-15V
GND
38
Trouble Shooting Tips
Bread board wiring
Check circuit diagram
Check breadboard wiring
Check supply voltages
Check voltages at nodes of Interest in your
circuit
To oscilloscope
8
7
6
5
2
7
-
741
3
6

4
1
2
3
4
To signal generator
Circuit diagram
Write down pin numbers on the circuit diagram
Use different color wires for supply and signals
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