How To Chose The Right Op Amp
There are two categories of requirements that relate to the performance of an op amp: General
and Application Specific.
General requirements are the degree of mismatch between pairs of circuit elements within an op
amp IC. The best matched op amp will have an offset of zero between all its inputs.
Application Specific requirements are tradeoffs. For example, an op amp with the best input
noise performance has high operating quiescent current. An op amp with the lowest operating
quiescent current has the worse input noise.
Like the laws of quantum reality, the more control you exercise over one aspect of your life the
less control you have over everything else. If you overspecify the General requirements, you
restrict the potential performance of the Application Specific requirements.
The best way to select an op amp is to start by defining the minimum acceptable General
requirements for a circuit application.
Op amps with the best General requirements have the lowest yields and/or require postmanufacture
trimming.
General Category:
Input Offset Voltage
The voltage that must be applied directly between the input measuring terminals, with bias current
supplied by a resistance path, to reduce the output indication to zero. Or the voltage that must be
applied between the two input terminals of an operational amplifier to obtain zero output voltage.
Input Offset Voltage Match Dual or Quad Amps
Offset voltage will tend to introduce slight errors in any opamp circuit. So how do we
compensate for it? Unlike commonmode gain, there are usually provisions made by the
manufacturer to trim the offset of a packaged opamp. Usually, two extra terminals on the op
amp package are reserved for connecting an external "trim" potentiometer. These connection
points are labeled offset null.
Input Offset Voltage Drift
Just because you trimmed out the offset voltage, doesn't mean all is tranquil on paradise island.
The input offset voltage will drift with temperature; you have no control over this. But, knowing
your overall error budget, you can select an op amp with a low enough offset drift for the
intended temperature range.
Voltage Stability
The most stable circuits have the longest response times, lowest bandwidth, highest accuracy,
and least overshoot. The least stable circuits have the fastest response times, highest bandwidth,
lowest accuracy, and some overshoot.
Input Offset Voltage Shift Rail to Rail Amplifiers
The effect of reducing the power supply voltage is a shift in the amplifier's input offset voltage.
The problem stems from the fact that most conventional op amps, with a typical operating range
down to +4.5 volts, are generally tested, and have their input offset trimmed, at a specific
supply voltage, e.g., +15 volts. Reducing the supply voltage can produce a shift in the input
offset voltage. The shift in the offset voltage can be determined by looking at the "powersupply
rejection ratio" (PSRR), or "powersupply sensitivity" of offset voltage specification;
it provides a
measure of the change in offset for a given change in supply voltage.
Input Offset Current
The difference between the two currents that must be supplied to the input measuring terminals of
a differential instrument to reduce the output indication to zero (with zero input voltage and zero
offset voltage). Or the difference in the currents into the two input terminals of an operational
amplifier when the output is at zero.
Common Mode Rejection Ratio
Common Mode Rejection Ratio Match Dual or Quad Amps
A measure of an instrument's ability to reject an undesired signal that is common to both input
terminals.
Also, CMRR describes the ability of a differential amplifier to reject interfering signals common
to both inputs, and to amplify only the difference between the inputs.
Power Supply Rejection Ratio
Power Supply Rejection Ratio Match Dual or Quad Amps
This specification is the measure of how well the op amp rejects an AC signal riding on a nominal
input DC voltage.
Powersupply rejection ratio is at a maximum at low frequencies, and begins to fall above 1kHz
to 10kHz, depending upon the op amp design.
The only way to modify the basic rejection response of the regulator is to add an external
network at the input of the op amp.
There are three methods to choose from:
1. One or more cascades of external RC filters. The additional attenuation adds to the inherent
characteristic of the regulator. Typical values for the single RC and cascade RC filters range from
R=1 to 10, and C=100µF to 10µF respectively. Choose the network 3dB frequency to
coincide with that of the regulator PSRR characteristic.
2. An LC filter. The problem with using this type of filter is the lack of inherent damping at the
output of the network (input of the op amp). The source impedance of the network is low.
However, the op amp's VIN terminal presents a high impedance shunted with a small capacitor.
(When the op amp is operated away from dropout with a constant load, its input current does
not vary, to first order, when VIN is varied.) It is impossible to critically damp the LC network
at the input of the regulator without significant DC loss in the shunt damping resistor. For
example, a series 10µH inductor in combination with a shunt 100µF capacitor exhibits a turnover
frequency of 5kHz; this combination requires a critical damping resistor of 0.32ohms between
network output (op amp input) and ground.
3. An additional linear regulator. This method occupies a small PCB area and requires the least
design time of the other methods. Using two linear regulators in series doubles the PSRR at any
given frequency (assuming identical regulators). The "penalty" for this approach is the doubling
of
the dropout voltage and the need for an additional capacitor. A good design choice is to share
the voltage drop across each op amp. The total assembly requires three capacitors, one each at
the input, output, and the intermediate position.
Application Specific:
Input Bias Current
Opamp inputs usually conduct very small currents, called bias currents, needed to properly bias
the first transistor amplifier stage internal to the opamps' circuitry. Bias currents are small (in
the
microamp range), but large enough to cause problems in some applications.
Bias currents in both inputs must have paths to flow to either one of the power supply "rails"
or
to ground. It is not enough to just have a conductive path from one input to the other.
To cancel any offset voltages caused by bias current flowing through resistances, just add an
equivalent resistance in series with the other opamp input (called a compensating resistor). This
corrective measure is based on the assumption that the two input bias currents will be equal.
Any inequality between bias currents in an opamp constitutes what is called an input offset
current.
It is essential for proper opamp operation that there be a ground reference on some terminal of
the power supply, to form complete paths for bias currents, feedback current(s), and load
current.
Input Bias Current Shift Also General, Rail to Rail Amplifiers
As the input signal moves from one supply rail to the other, the amplifier shifts from one input pair
to the other. At the crossover point, this shift can cause changes in the input bias current and
offset voltage that affect both the magnitude and the polarity of these parameters. These offsetvoltage
changes typically worsen the distortion performance and precision specifications of railtorail amplifiers
(in comparison with groundsensing types). To minimize offsetvoltage shifts and
smooth the transition from one input pair to another, Manufactures trims the offset of its railtorail
amplifiers at both the high and the low ends of the commonmode range.
To reduce offset voltages caused by input bias currents, the designer should match impedances
at the op amp's inverting and noninverting nodes. Because input bias currents are typically larger
than input offset currents, this impedance matching is good practice for all types of op amps, not
just railtorail input amplifiers.
Output High Voltage
Output Low Voltage
The output of an op amp is required to swing railtorail or as close as possible. The output
swing is dependent on the amount of output loading.
The inputtooutput linearity will degrade as the output swing approaches the voltage supply.
If the output is pushed to the rails, it will change the offset voltage of the op amp.
The output swing of the op amp can vary between +V and V supply, and is controlled by the
voltage difference between +In and In. If the voltage at +In is positive with respect to In, then
the output of the op amp swings positive, toward the +V rail voltage. If the voltage at +In is
negative compared to the voltage at In, the output swings negative. It only takes a small
difference in voltage between the two inputs to create a large change in the output voltage. This is
known as the gain of the op amp.
Open Loop Voltage Gain
This is ratio of the input to the output voltage with no feedback applied. It is the D.C. gain of the
amplifier or the gain at a frequency of 1 Hz. It is dependent on the output voltage swing and
output load.
Common Mode Input Range
The range of input voltage for which the differential pairs behaves as a linear op amp. The upper
limit is determined by one of the two inputs saturating. The lower limit is determined by the input
bias current.
Input Noise Voltage
Input Noise Voltage Density
Input Current Noise
Input Current Noise Density
Op amp input noise specifications are usually given in terms of nV/H.z for noise voltage and
pA/H.z or fA/H.z for noise current and are therefore directly comparable with resistor thermal
noise. Due to the fact that noise density varies at low frequencies, most op amps also specify a
typical peaktopeak noise within a “0.1Hz to 10Hz or 0.01Hz to 1Hz bandwidth.
There are five types of noise in op amps and associated circuitry:
1) Shot noise
2) Thermal noise
3) Flicker noise
4) Burst noise
5) Avalanche noise
Some or all of these noises may be present in a design, presenting a noise spectrum unique to the
system. It is not possible in most cases to separate the effects, but knowing general causes may
help the designer optimize the design, minimizing noise in a particular bandwidth of interest.
Proper design for low noise may involve a “balancing act” between these sources of noise and
external noise sources.
Shot Noise
The name shot noise is short for Schottky noise. Sometimes it is referred to as quantum noise.
It is caused by random fluctuations in the motion of charge carriers in a conductor.
Put another way, current flow is not a continuous effect. Current flow is electrons, charged
particles that move in accordance with an applied potential. When the electrons encounter a
barrier, potential energy builds until they have
enough energy to cross that barrier. When they have enough potential energy, it is abruptly
transformed into kinetic energy as they cross the barrier. A good analogy is stress in an
earthquake fault that is suddenly released as an earthquake.
As each electron randomly crosses a potential barrier, such as a pn junction in a semiconductor,
energy is stored and released as the electron encounters and then shoots across the barrier. Each
electron contributes a little pop as its stored energy is released when it crosses the barrier.
Thermal Noise
Thermal noise is sometimes referred to as Johnson noise after its discoverer. It is generated by
thermal agitation of electrons in a conductor. Simply put, as a conductor is heated, it will become
noisy. Electrons are never at rest; they are always in motion. Heat disrupts the electrons’
response to an applied potential. It adds a random component to their motion.
Flicker Noise
Flicker noise is also called 1/f noise. Its origin is one of the oldest unsolved problems in
physics.
It is pervasive in nature and in many human endeavors. It is present in all active and many passive
devices. It may be related to imperfections in crystalline structure of semiconductors, as better
processing can reduce it.
Flicker noise is found in carbon composition resistors, where it is often referred to as excess
noise because it appears in addition to the thermal noise that is there. Other types of resistors
also exhibit flicker noise to varying degrees, with wire wound showing the least. Since flicker
noise is proportional to the dc current in the device, if the current is kept low enough, thermal
noise will predominate and the type of resistor used will not change the noise in the circuit.
Reducing power consumption in an op amp circuit by scaling up resistors may reduce the 1/f
noise, at the expense of increased thermal noise.
Burst Noise
Burst noise, also called popcorn noise, is related to imperfections in semiconductor material and
heavy ion implants. It is characterized by discrete highfrequency pulses. The pulse rates may
vary, but the amplitudes remain constant at several times the thermal noise amplitude. Burst noise
makes a popping sound at rates below 100 Hz when played through a speaker — it sounds like
popcorn popping, hence the name. Low burst noise is achieved by using clean device
processing, and therefore is beyond the control of the designer.
Modern processing techniques at Texas Instruments has all but eliminated its occurrence.
Avalanche Noise
Avalanche noise is created when a pn junction is operated in the reverse breakdown mode.
Under the influence of a strong reverse electric field within the junction’s depletion region,
electrons have enough kinetic energy that, when they collide with the atoms of the crystal lattice,
additional electronhole pairs are formed (Figure 10–4). These collisions are purely random and
produce random current pulses similar to shot noise, but much more intense.
When electrons and holes in the depletion region of a reversedbiased junction acquire enough
energy to cause the avalanche effect, a random series of large noise spikes will be generated.
The magnitude of the noise is difficult to predict due to its dependence on the materials. Because
the zener breakdown in a pn junction causes avalanche noise, it is an issue with op amp designs
that include zener diodes. The best way of eliminating avalanche noise is to redesign a circuit to
use no zener diodes.
Color Noise
While the noise types are interesting, real op amp noise will appear as the summation of some or
all of them. The various noise types themselves will be difficult to separate. Fortunately, there is
an alternative way to describe noise, which is called color. The colors of noise come from rough
analogies to light, and refer to the frequency content. Many colors are used to describe noise,
some of them having a relationship to the real world, and some of them more attuned to the field
of psychoacoustics.
White noise is in the middle of a spectrum that runs from purple to blue to white to pink and
red/brown. These colors correspond to powers of the frequency to which their spectrum is
proportional, as shown in the table below.
Color Frequency Content
Purple = frequencies squared
Blue = frequencies
White = 1
Pink = 1 / frequencies
Red Brown = 1 / frequencies squared
Gain Bandwidth Product
To determine the maximum gain that can be extracted from the circuit for a given frequency (or
bandwidth) and viceversa.
For example, if the GBW of an opamp is 1 MHz, it means that the gain of the device falls to
unity at 1MHz. Hence when the device is wired for unity gain it will work up to 1MHz (GBW
product = gain x bandwidth, therefore if BW = 1 MHz, gain = 1) without excessively distorting
the signal. The same device when wired for a gain of 10 will work only up to 100 kHz, in
accordance with the GBW product formula. Further, if the maximum frequency of operation is 1
Hz, then the maximum gain that can be extracted from the device is 1 x 10 to the 6 power.
Slew Rate
This is the rate of change of the op amp's voltage output over time when its gain is set to unity
(Gain =1).
3dB Bandwidth
3dB bandwidth is defined as the frequency at which the signal intensity (or gain) has fallen to 0.5
of the zero frequency value.
The bandwidth is the difference between the upper 3dB frequency and lower 3dB frequency of a
bandpass filter (High F3dB – Low F3dB).
Phase Margin
The phase margin is the difference between the phase of the response and 180° when the loop
gain is 1.0. The frequency at which the magnitude is 1.0 is called the unitygain frequency or
crossover frequency. It is generally found that gain margins of three or more combined with
phase margins between 30 and 60 degrees result in reasonable tradeoffs between bandwidth
and stability. The phase margin is the additional phase required to bring the phase of the loop
gain to 180 degrees.
The system is unstable when the loop gain equals 1. That is, gain has a magnitude of one and a
phase of 180 degrees. An unstable system oscillates. A system close to being unstable has a
large ringing overshoot in response to a step input.
Full Power Bandwidth
Full Power Bandwidth (FPBW) is the frequency at which the reconstructed output fundamental
drops 3 dB below its low frequency value for a full scale input.
Total Harmonic Distortion + Noise
THD is simply a measurement of how much RMS harmonic current is present in comparison to
the amount of fundamental current. THD does NOT take into account frequency. It is the RMS
value of ONLY the harmonics divided by the RMS value of the fundamental and is expressed in
percent.
The RMS value of a sine wave regardless of frequency is simply the peak value of the sine wave
divided by the square root of 2. (V means voltage)
Linear loads on a power system draw a load current that is a pure sine wave at the power
frequency of 60Hz. Most everyone has seen the typical sine wave of 60Hz voltage that can be
displayed on an oscilloscope. A linear load draws a current waveform of the same shape.
When a non linear load draws current from the power system (i.e. from the transformer), the
current waveform is distorted from the mathematically perfect shape of a sine wave. A square
wave or saw tooth waveform is an example of a distorted waveform.
The distorted waveform is actually a summation of the fundamental frequency sine wave and a
variety of harmonics. Harmonics are actually pure sine waves themselves but each has a
frequency that oscillates at a multiple of 60Hz (i.e. 3rd harmonic = 3 x 60 = 180Hz, 5th
harmonic = 5 x 60 = 300Hz).
To find the total RMS value of any distorted wave, you have to take "the square root of the sum
of the squares" of the RMS value of the fundamental and the series of harmonics. (admittedly it's
easier to see this demonstrated than to explain it!!)
In this example the fundamental current is 10 amps. The harmonic RMS value is 5 amps.
5 / 10 x 100% = 0.5 x 100% = 50%
Therefore the THD is 50% regardless of the harmonic frequency.
In truth, THD is limited in its application. It is really only good for expressing harmonic limits on
a
feeder or that is produced by a load in a general way. It doesn't tell you which harmonics are
present and how much of each harmonic (i.e. their RMS values) is present.
For that you need to perform a Harmonic Spectrum Analysis which is easily done with clamp on
meters that are readily available. (Fluke has some hand held models that cost around $1500)
These meters will tell you which harmonics are present, their respective RMS values, and even
the phase angle between the harmonic and the fundamental. (The phase angle is seldom used in
any calculation or harmonic study.)
You must have a Spectrum Analysis performed at different points on your power system (such
as at a non linear load, at the transformer, at capacitor banks, at the panelboard, etc.) before any
solution to any harmonic problem can be undertaken.
Once the analysis is complete, and if the harmonics are causing you trouble (such as overheating
transformers, blowing cap bank fuses, tripping breakers, causing telephone interference, etc.),
the information can be used to apply harmonic filters, to size K rated transformers, or to install
harmonic cancellation equipment.
Settling Time
This is the length of time for the output voltage of an operational amplifier to approach, and
remain within, a certain tolerance of its final value. This is usually specified for a fast fullscale
input step.
Operating Quiescent Current
Quiescent current is the current that flows in an electrical circuit when no load is present.
Differential Gain
The differential gain is the ratio of the difference of the outputs over the difference of the inputs.
In video it is the amount of change in the color saturation (amplitude of the color modulation) for
a change in lowfrequency luma (brightness) amplitude.
In fiber optics it's a type of distortion in a video signal that causes the brightness information to
be
incorrectly interpreted.
Differential Phase
In video it is the change in hue (phase of the color modulation) for a change in lowfrequency
luma (brightness) amplitude.
