An operational amplifier (op amp) is an analog circuit block that takes a differential voltage input and produces a single-ended voltage output. Understanding these fundamental 10 op amp circuits allows you to easily study more complex circuits. Op-Amps: Ubiquitous ICs with Multiple Applications. An op-amp operates on analog input. · Op-Amp Basics (1): An Inverting Amplifier Circuit. The circuit shown in. INVESTING MONEY IN INDIA FROM US See also Capturing private bathroom also. Define their infrastructure, to a xmonad 1 silver badge. But keep in you need, and on the bottom install and use.
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As a rule, you should never allow either input voltage to rise above the positive power supply rail voltage, or sink below the negative power supply rail voltage, even if the op-amp in question is protected against latch-up as are the and op-amp models. At worst, the kind of latch-up triggered by input voltages exceeding power supply voltages may be destructive to the op-amp.
While this problem may seem easy to avoid, its possibility is more likely than you might think. Consider the case of an operational amplifier circuit during power-up. If the circuit receives full input signal voltage before its own power supply has had time enough to charge the filter capacitors, the common-mode input voltage may easily exceed the power supply rail voltages for a short time.
If the op-amp receives signal voltage from a circuit supplied by a different power source, and its own power source fails, the signal voltage s may exceed the power supply rail voltages for an indefinite amount of time! Another practical concern for op-amp performance is voltage offset. That is, effect of having the output voltage something other than zero volts when the two input terminals are shorted together.
When that input voltage difference is exactly zero volts, we would ideally expect to have exactly zero volts present on the output. However, in the real world this rarely happens. Even if the op-amp in question has zero common-mode gain infinite CMRR , the output voltage may not be at zero when both inputs are shorted together. This deviation from zero is called offset. A perfect op-amp would output exactly zero volts with both its inputs shorted together and grounded.
However, most op-amps off the shelf will drive their outputs to a saturated level, either negative or positive. In the example shown above, the output voltage is saturated at a value of positive For this reason, offset voltage is usually expressed in terms of the equivalent amount of input voltage differential producing this effect. In other words, we imagine that the op-amp is perfect no offset whatsoever , and a small voltage is being applied in series with one of the inputs to force the output voltage one way or the other away from zero.
Offset voltage will tend to introduce slight errors in any op-amp circuit. So how do we compensate for it? Unlike common-mode gain, there are usually provisions made by the manufacturer to trim the offset of a packaged op-amp. These connection points are labeled offset null and are used in this general way:. On single op-amps such as the and , the offset null connection points are pins 1 and 5 on the 8-pin DIP package. Inputs on an op-amp have extremely high input impedances.
We analyze the circuit as though there was absolutely zero current entering or exiting the input connections. This idyllic picture, however, is not entirely true. Op-amps, especially those op-amps with bipolar transistor inputs, have to have some amount of current through their input connections in order for their internal circuits to be properly biased.
These currents, logically, are called bias currents. Under certain conditions, op-amp bias currents may be problematic. The following circuit illustrates one of those problem conditions:. At first glance, we see no apparent problems with this circuit. In other words, this is a kind of comparator circuit , comparing the temperature between the end thermocouple junction and the reference junction near the op-amp. The problem is this: the wire loop formed by the thermocouple does not provide a path for both input bias currents, because both bias currents are trying to go the same way either into the op-amp or out of it.
In order for this circuit to work properly, we must ground one of the input wires, thus providing a path to or from ground for both currents:. Another way input bias currents may cause trouble is by dropping unwanted voltages across circuit resistances.
Take this circuit for example:. We expect a voltage follower circuit such as the one above to reproduce the input voltage precisely at the output. But what about the resistance in series with the input voltage source? But even then, what slight bias currents may remain can cause measurement errors to occur, so we have to find some way to mitigate them through good design. One way to do so is based on the assumption that the two input bias currents will be the same. In reality, they are often close to being the same, the difference between them referred to as the input offset current.
If they are the same, then we should be able to cancel out the effects of input resistance voltage drop by inserting an equal amount of resistance in series with the other input, like this:. With the additional resistance added to the circuit, the output voltage will be closer to V in than before, even if there is some offset between the two input currents.
In either case, the compensating resistor value is determined by calculating the parallel resistance value of R 1 and R 2. Why is the value equal to the parallel equivalent of R 1 and R 2? This gives two parallel paths for bias current through R 1 and through R 2 , both to ground. A related problem, occasionally experienced by students just learning to build operational amplifier circuits, is caused by a lack of a common ground connection to the power supply.
This provides a complete path for the bias currents, feedback current s , and for the load output current. Take this circuit illustration, for instance, showing a properly grounded power supply:. The effect of doing this is profound:. Thus, no electrons flow through the ground connection to the left of R 1 , neither through the feedback loop.
This effectively renders the op-amp useless: it can neither sustain current through the feedback loop, nor through a grounded load, since there is no connection from any point of the power supply to ground. The bias currents are also stopped, because they rely on a path to the power supply and back to the input source through ground. The following diagram shows the bias currents only , as they go through the input terminals of the op-amp, through the base terminals of the input transistors, and eventually through the power supply terminal s and back to ground.
Without a ground reference on the power supply, the bias currents will have no complete path for a circuit, and they will halt. Since bipolar junction transistors are current-controlled devices, this renders the input stage of the op-amp useless as well, as both input transistors will be forced into cutoff by the complete lack of base current.
Bias currents are small in the microamp range , but large enough to cause problems in some applications. 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 op-amp 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 op-amp constitutes what is called an input offset current. It is essential for proper op-amp 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.
Being semiconductor devices, op-amps are subject to slight changes in behavior with changes in operating temperature. Any changes in op-amp performance with temperature fall under the category of op-amp drift.
Drift parameters can be specified for bias currents, offset voltage, and the like. The latter action may involve providing some form of temperature control for the inside of the equipment housing the op-amp s. This is not as strange as it may first seem. If extremely high accuracy is desired over the usual factors of cost and flexibility, this may be an option worth looking at. Op-amps, being semiconductor devices, are susceptible to variations in temperature.
Any variations in amplifier performance resulting from changes in temperature is known as drift. Drift is best minimized with environmental temperature control. With their incredibly high differential voltage gains, op-amps are prime candidates for a phenomenon known as feedback oscillation. Because we have no nice virtual ground at the non-inverting input, we have to analyze the non-inverting summing amplifier a little differently to the inverting version.
We can then write replace the currents above with the voltage difference divided by the resistance:. As described in the Section 4. Op-amps can be used to perform level-shifting. The concept of level-shifting is very similar to what is achieved by summing amplifiers. Ideal diode circuits are useful when:. You have to rectify a signal with precision the forward voltage drop across the diode is unacceptable. Figure 21 shows the most basic form of an ideal diode a.
Figure 22 shows the response of the basic ideal diode circuit. The ideal diode is only ideal up to a point. It is not limited by the bandwidth and max. There is also an issue with slew rates with the above circuit. This will cause some delay on the output limited by the slew rate when the input once again goes positive.
Figure 23 shows an improved half-wave rectifier with additional circuitry to prevent the op-amp from saturating when in the blocked part of the cycle . The basic op-amp based sample and hold circuit is an extension of the ideal diode circuit, but with an added capacitor on the output to maintain with the voltage when the input signal is removed. The common-mode input voltage range is the range of voltages that can appear at the input to the op-amp and it still work correctly. It is a DC measurement parameter.
In an ideal op-amp, the op-amp only amplifies a difference between the inputs, and so the output is 0V when the difference is 0V, hence the input offset voltage is 0V. However, real-world op-amps always have some unavoidable differences in the internal components that make up the op-amps specifically, in the input differential stage of the internal circuitry , and thus the inputs are not perfectly identical.
Figure 25 shows how the input offset voltage is modelled as a voltage source in series with one of the inputs of an ideal op-amp. A non-zero input offset voltage results in gain errors between the input and output of a op-amp. The input offset voltage is typically in the following ranges:.
For example, the OPAx family of op-amps has a max. Input offset voltages vary by op-amp transistor technology. The input offset voltage varies with both temperature and time drift. The change of input offset voltage with time is called aging. But since aging is a physical process that follows the "random walk pattern" Brownian motion , it is more accurate to describe it proportional to the square root of elapsed time. Some op-amps are trimmed by the manufacturer after the op-amp is packaged.
Performing trimming after packaging prevents any production-line effects from effecting the input offset voltage. The offset is trimmed with a special digital code using no extra pins i. Once programmed, poly-silicon fuses are blown to permanently set the trim values . If your op-amp lacks a dedicated trim pin, you can make your own trimming circuit as shown in Figure This is for an op-amp in the inverting configuration.
In reality, always some small amount of current will flow. Typical input bias currents range from nA. The amount and behaviour of input bias current depends on the op-amp transistor technology. Input bias currents are a problem because these currents will flow through external circuitry connected to the op-amps inputs.
This current when flowing through resistors and other impedances will create unwanted voltages which will increase the systematic errors. The input impedance is the internal resistance to ground from the two input pins. In an ideal op-amp, this value is infinite. The multiplication of the gain with the frequency gives the gain-bandwidth product, which is relatively constant for a particular op-amp.
Hence if the gain bandwidth of a particular op-amp is 1Mhz, and the gain is 10, the maximum frequency that the op-amp can operate linearly at still provide a gain of 10 is at kHz. Or if the gain was set to , then the maximum frequency is 10kHz. This also means that an op-amp acts as a low-pass filter, as the gain drops for very high frequencies.
A low gain-bandwidth is around 1kHz reminiscent of less advanced, older op-amps. Not realising this can be confusing! The GBW product is closely related to the slew rate. The LM is rumoured to only be able to drive the output near ground if it is sourcing current, but only to 0. The slew rate of an op-amp defines the maximum rate the output voltage can change with respect to time.
In an ideal op-amp, this would be infinite. It can be thought of as the slope of the output waveform if one of the inputs of the input was subjected to a step voltage change. Op-amps have a limited output slew rate due to internal compensation capacitor combined with a finite output drive current. Figure 27 shows how the non-infinite slew rate of an op-amp distorts the shape of an input square-wave "pulse".
The max. This parameter usually increases as the GBW of the op-amp increases. Higher slew rate op-amps also tend to have higher quiescent currents. Figure 28 shows different levels of distortion for a 10V peak 20kHz sine wave when it is generated by an op-amps with different slew rates. The quiescent current current with no load, device in steady-state is generally constant over the total rated supply voltage range. Obviously, if there is a load on the op-amp, the current drawn through the power pins the supply current will be the sum of the quiescent current and the current going through the load.
Quiescent currents for standard op-amps are typically between 1. A 'low-power' op-amp has a typical quiescent current between 0. Then there are ultra-low power op-amps that only draw pA such as the LMC You normally sacrifice slew-rate and gain-bandwidth for ultra-low power. Likewise, higher gain-bandwidth and higher slew rate op-amps typically have larger quiescent currents. Cascading op-amps is concept when the output of one op-amp is connected to the input of another. There can be an arbitrary number of op-amps in the cascade, but usual limits are For a fixed-gain, cascading op-amps can also be used to increase the bandwidth , as each individual op-amp now can operate at a lower gain and therefore has a larger bandwidth as defined by the gain-bandwidth product.
Note though that each additional op-amp added to increase the bandwidth gives diminishing returns. Also important to note that op-amp bandwidth is defined as the -3dB gain points. Hence the bandwidth does not stay the same total bandwidth gets smaller when two identical op-amps are cascaded, as these will now the -6dB points. A practical limit for fixed-total-gain increased-bandwidth cascading is about op-amps.
When cascading op-amps, the total gain is the product of all of the individual op-amps gains, i. As a rule-of-thumb, you should use the lowest acceptable resistances in op-amp feedback paths to reduce instabilities. A rail-to-rail op-amp is an op-amp which supports input voltages near the power rails, and can drive the output close to the one or more of the power rails. Rail-to-rail op-amps just support wider ranged input voltages and can drive closer to the rails than general purpose op-amps can.
For "rail-to-rail" op-amps, this will usually be about mV about ground at normal load currents. This also means that a rail-to-ral single-supply op-amp cannot output 0V. To achieve a true ground output, you need a negative voltage supply. There are dedicated ICs designed to provide a small negative power supply to op-amps so that they can output true ground.
Micropower is a termed used for extremely low quiescent current op-amps that are designed for battery or energy recovery-based power supplies. The supply current of micropower op-amps is typically within the range of uA at a supply voltage of V. Because they are designed for battery-based systems, they are also commonly single-supply op-amps. Instrumentation amplifiers are analog voltage amplifier circuits that, although are drawn the the same symbol as an op-amp, are typically made up internally from three op-amps and passives.
You can either make an instrumentation amplifier out of discrete op-amps or purchase a instrumentation amplifier IC which contains all the op-amps within the same chip. OPAx : Zero-drift 36V rail-to-rail op-amps. Internally compensated for unity-gain stability. TLE : Texas Instruments family of "high-speed low-power" precision operational amplifiers.
Belong to the Excalibur family of TI op-amps which uses "isolated vertical PNP transistors" to give unity-gain bandwidth and slew rate improvements. We can generalize the circuit of an op-amp with negative feedback to the block diagram shown below.
With that, we can simply the closed loop gain to be:. Below are some examples of op-amps that stand out from the crowd for some reason, be it popularity, years in service, or functionality wise. Good for high precision stuff! Awesome for photo-diode amplification both current-to-voltage and voltage-to-voltage configurations.
A common family of op-amps that has been around for along time, they can operate of a single supply and can swing right to ground, but cannot swing to the rail voltage. This is a ultra-wideband, current-feedback op-amp. If you need an op-amp with a ridiculously high gain-bandwidth product, this is along the lines of what you want to use. Dedicated charge-pump topology power supply ICs are available that supply a small negative voltage to the op-amps V- pin.
Isolation amplifiers provide galvanic isolation between the input sensor and output measurement circuitry. They are used to protect the sensor measurement and recording circuitry e. A common application would be to isolate and amplify the voltage across a current-sense resistor on a high-power motor, or to protect humans with medical sensors connected to them from the measurement system.
Basic isolation amplifiers require two power supplies one for each side of isolation , while others incorporate built-in transformers so that you only have to provide one power source. One of the first things you learn about an op-amp is that the input impedance on the input pins are very large ideally infinite. So naturally you would start to question why resistors would be connected to the input pins of an op-amp like shown in Figure The resistor limits this current to a safe value.
Some op-amps which are designed to have very low input offset voltages also come with offset nulling pins to further trim the input offset voltage once the op-amp is installed in circuit. The OP07 is one op-amp which has these pins. A negative impedance converter NIC is a clever op-amp circuit which creates negative impedance you might be wondering what negative impedance actually is, more on this later. A NIC can be constructed from an op-amp and a few passive components as shown in the following schematic:.
What does negative impedance actually mean? This means the circuit behaves just like a simple resistor connected to ground, except that the current comes out of the resistor, not into it. Since no current flows into the inverting terminal of the op-amp, this also must be current flowing "out" of the input terminal.
Op-amps are usually packaged in industry standard through-hole and surface mount packages. For many of these packages, there are industry standard pinouts which means you can easily find pin-compatible alternatives for any given op-amp. This section aims to illustrate some of these industry standard pinouts.
Texas Instruments. Op Amp Input Bias Current. Analog Devices. Schematic Symbol An op-amp is commonly drawn on schematics as:. Sometimes they can be drawn swapped around relative to the symbol shown above. Uses Buffers a. Op-Amp Topologies 4. Voltage Followers a.
Buffers A voltage follower also known as a buffer is one of the most basic circuits you can make with an op-amp. Figure 3. A simulation schematic for an op-amp configured as a voltage-follower buffer.