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"What Are Input and Output Impedance in Op-Amps?" - "1.1 Impedance Overview" -> "Understanding Impedance Basics" - "1.2 Input Impedance of Op-Amp" -> "Why Does an Op-Amp Need High Input Impedance?" - "1.3 Output Impedance of Op-Amp" -> "Why Does an Op-Amp Need Low Output Impedance?" - "1.4 Ideal Op Amp Impedance" -> "Ideal vs. Practical Op-Amp Impedance" - "Ⅱ High Input Impedance and Low Output Impedance Effect" -> "The Effects of High Input and Low Output Impedance" - "Ⅲ How to Calculate Input Impedance and Output Impedance" -> "How to Calculate Op-Amp Impedance"- Missing or improvable schema types detected: Missing Article schema, FAQPage schema.- Sections with vague/unsupported claims: "A small amount of current is decreased by any electrical input..." (Rewritten for technical accuracy: "Every electrical input sources or sinks a small amount of leakage current."); Formula for impedance was inverted (ΔI/ΔV instead of ΔV/ΔI) and has been corrected.- Estimated content freshness score: 5/10-->Summary: Operational amplifiers (op-amps) rely on extremely high input impedance to prevent signal degradation and very low output impedance to drive loads effectively. Understanding how to calculate and optimize these impedance values is critical for preventing loading effects and ensuring accurate signal amplification in modern circuit design.IntroductionThe input and output impedance of an amplifier is the ratio of voltage to current flowing in or out of these terminals. The input impedance may depend upon the source supply feeding the amplifier, while the output impedance may also vary according to the load impedance (RL) across the output terminals. Ideally, op-amps are supposed to have zero output impedance and infinite input impedance. However, practical op amp input impedance and output impedance are finite, making them critical factors in the design of any robust electronic circuit. What Are Input and Output Impedance in Op-Amps?Understanding Impedance BasicsIn electronic circuits, impedance defines the complex relationship between voltage and current. It is a combination of resistance (which is frequency-independent) and reactance (which is frequency-dependent, driven by inductors and capacitors). The input impedance of an op-amp acts as the load impedance to the preceding signal source. Conversely, the output impedance of the op-amp acts as the source impedance to the subsequent load receiving the amplified signal. Understanding these parameters is essential for proper impedance matching and signal integrity.Why Does an Op-Amp Need High Input Impedance?While the input impedance of an ideal op-amp is assumed to be infinite, practical devices always draw a microscopic amount of bias current. Every electrical input sources or sinks a small amount of leakage current, which can be modeled as a high-value resistor connected in parallel to the input terminals. Modern CMOS op-amps can achieve input impedances in the tera-ohm ($10^{12} Omega$) range, drastically reducing this current draw.Although input impedance is typically represented as a simple resistor, the input terminals also possess a tiny parasitic capacitance. At lower frequencies, this capacitance is negligible. However, at high frequencies, this parasitic capacitance provides a substantial load for AC signals, hindering rise and fall times and potentially causing severe signal distortion.Why Does an Op-Amp Need Low Output Impedance?An ideal amplifier should be capable of driving infinite current into any load without voltage loss, but practical op-amps have strict physical limitations. For instance, the widely used LM358 op-amp can typically source only 40mA and sink 20mA of current. This restriction in the output drive capability is modeled as a small internal resistor placed in series with an ideal voltage source.Because the actual output voltage is measured after this internal resistor, overloading the op-amp causes a significant voltage drop across it. Consequently, the delivered voltage falls short of the amplifier's intended output. To counter this limitation when driving heavy loads, engineers often add an external discrete output stage (like a push-pull transistor buffer) to boost current capacity.Ideal vs. Practical Op-Amp ImpedanceAn ideal op-amp features infinite input impedance and zero output impedance. Infinite input impedance ensures that absolutely no current flows into or out of the inverting and non-inverting terminals. Zero output impedance guarantees that the output voltage remains perfectly stable, regardless of the current demanded by the load.ParameterIdeal Op-AmpPractical Op-Amp (e.g., CMOS)Input ImpedanceInfinite (∞)Very High (Mega-ohms to Tera-ohms)Output ImpedanceZero (0 Ω)Very Low (10 to 100 ohms)Op Amp Impedance MatchingThe Effects of High Input and Low Output ImpedanceHigh input impedance ensures that the amplifier draws virtually no current from the preceding signal source. Because op-amps are primarily voltage-gain devices, their core task is to convert a low-energy, voltage-driven signal into a higher-voltage output without distorting the original source.Preventing the Loading Effect: If the input impedance were low, the op-amp would draw excessive current, causing a voltage drop across the source's internal resistance and degrading the signal.Maximizing Voltage Transfer: According to Ohm's Law (V=IR), a higher input impedance ensures that the maximum possible voltage drops across the amplifier's input terminals rather than being lost in the source wiring.Safe Current Management: Low impedance circuits can inadvertently trigger high current draws, which may damage sensitive sensor outputs. High input impedance safely isolates these delicate components. How to Calculate Op-Amp ImpedanceImpedance is mathematically represented by the ratio of voltage variation (ΔV) to current variation (ΔI). For an op-amp, the variation in the input common-mode voltage range is measured against the variation in the input bias current to determine dynamic input impedance.Input Impedance and Output Impedance of AmplifierUsing the voltage divider principle, you can determine the actual input and output voltages of an amplifier based on its gain, source impedance, and output impedance. The formula for the effective input voltage is:Vin = Vsource • (Zin / (Rs + Zin)) ......(1)Where Vin is the actual voltage the amplifier receives, Vsource is the original source voltage, Zin is the amplifier's input impedance, and Rs is the source's internal impedance.Similarly, you can calculate the voltage delivered to the load:Vload = Vout • (Rload / (Rload + Zout)) ......(2)Where Vload is the voltage dropped across the load, Vout is the amplifier's internal generated output voltage, Rload is the load resistance, and Zout is the amplifier's output impedance.To measure the output impedance practically, you can model it as a Thevenin equivalent circuit:Zout = Vo / Isc ......(3)Where Vo is the open-circuit output voltage, and Isc is the short-circuit output current. This formula assumes a strictly linear relationship between the output voltage and current.ConclusionOp-amps are essential in circuit designs where the input impedance must be vastly larger than the source impedance, and the effective output impedance must be infinitesimal compared to the load. The specific demands of your application will dictate the required precision of the op-amp. Ultimately, the input and output impedance of amplifiers stem from internal parasitic resistance and capacitance. By understanding these physical limits and applying the correct voltage divider formulas, engineers can design highly efficient, distortion-free amplification stages. Frequently Asked QuestionsWhat happens if an op-amp has low input impedance?If an op-amp has low input impedance, it draws excessive current from the signal source. This creates a loading effect, causing a significant voltage drop across the source's internal resistance. Consequently, the amplifier receives a degraded signal, leading to inaccurate amplification and potential signal distortion.Which type of op-amp provides the highest input impedance?Modern CMOS (Complementary Metal-Oxide-Semiconductor) and JFET operational amplifiers provide the highest input impedance. Unlike older bipolar junction transistor models like the LM741, CMOS op-amps can achieve input impedances in the tera-ohm range, drawing nearly zero bias current from the source.How does a unity-gain buffer utilize impedance matching?A unity-gain buffer leverages the op-amp's extremely high input impedance and near-zero output impedance to bridge circuits. It prevents a low-impedance load from drawing too much current from a high-impedance source, ensuring the signal voltage transfers perfectly without degradation or power loss.Can you measure op-amp output impedance directly with a multimeter?No, you cannot measure an active op-amp's output impedance directly using a standard multimeter's resistance setting. Instead, you must calculate it dynamically by measuring the open-circuit output voltage, applying a known load resistor, measuring the loaded voltage drop, and using the voltage divider formula.{ "@context": "https://schema.org", "@graph":[ { "@type": "Article", "headline": "Op Amp Input and Output Impedance Guide", "datePublished": "2021-01-23T15:45:51Z", "dateModified": "2026-03-19T15:12:00+08:00", "author": { "@type": "Organization", "name": "ApogeeWeb" }, "publisher": { "@type": "Organization", "name": "ApogeeWeb" } }, { "@type": "FAQPage", "mainEntity":[ { "@type": "Question", "name": "What happens if an op-amp has low input impedance?", "acceptedAnswer": { "@type": "Answer", "text": "If an op-amp has low input impedance, it draws excessive current from the signal source. This creates a loading effect, causing a significant voltage drop across the source's internal resistance. Consequently, the amplifier receives a degraded signal, leading to inaccurate amplification and potential signal distortion." } }, { "@type": "Question", "name": "Which type of op-amp provides the highest input impedance?", "acceptedAnswer": { "@type": "Answer", "text": "Modern CMOS (Complementary Metal-Oxide-Semiconductor) and JFET operational amplifiers provide the highest input impedance. Unlike older bipolar junction transistor models like the LM741, CMOS op-amps can achieve input impedances in the tera-ohm range, drawing nearly zero bias current from the source." } }, { "@type": "Question", "name": "How does a unity-gain buffer utilize impedance matching?", "acceptedAnswer": { "@type": "Answer", "text": "A unity-gain buffer leverages the op-amp's extremely high input impedance and near-zero output impedance to bridge circuits. 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IntroductionAn operational amplifier, or op amp is used in a wide variety of applications in electronics. It generally comprises a differential-input stage with high input impedance, an intermediate-gain stage, and a push-pull output stage with a low output impedance. Common operational amplifier has two input pins and one output pin. Its basic role is to amplify and output the voltage difference between the two input pins. So what are these op-amp parameters meaning? This note tells you the typical parameters of op-amp and their definitions, also there have several examples with specific values to explain deeply for you. CatalogIntroductionⅠ How Does An Op Amp Work?Ⅱ Understanding Basic Op-amp Parameters2.1 What are the Parameters of Op Amp?2.2 Questions about Op Amp Important ParametersⅢ Common Op-amp ICs Datasheet OverviewⅣ ConclusionⅠ How Does An Op Amp Work?An op-amp is a multi-stage , direct coupled, high gain negative feedback amplifier. It is basically a three-terminal device which consists of two high impedance inputs. Ideally, it only amplifies the difference in voltage between the two, also called differential input voltage. Op-amps are still a primary building block for analog systems, performing tasks like amplification, active filtering, and signal transformation. In digital systems, op-amps are used in buffers, analog-to-digital converters, digital-to-analog converters, and regulated power supplies, to name a few applications.Ⅱ Understanding Basic Op-amp ParametersOp-amps are linear devices that are ideal for DC amplification and are used often in signal conditioning, filtering or other mathematical operations. So understanding its basic parameters is important to employ it well in circuits.Parameters Of Op-Amp2.1 What are the Parameters of Op Amp?Gain Bandwidth1) Gain bandwidth product: Due to parasitic junction capacitance and minority-carrier change storage in devices, the voltage gain of op amp decreases at high frequencies, it refers to the bandwidth and gain product.2) Unity gain bandwidth: As the input signal of the frequency increases, the open-loop gain drops off until it finally reacts to the value 1. The frequency at which the gain reduces to 1 is defined as unity gain frequency or unity-gain bandwidth.Input Offset VoltageIt is a very small voltage applied at the outputs, to make the output terminal zero of the operational amplifier. It reflects the symmetry of the the op amp circuit. The better the symmetry, the smaller the input offset voltage.Input Offset Voltage DriftThe input offset voltage drift is also called the temperature coefficient. In a given temperature range, it is the ratio of the change in the input offset voltage to the temperature change. This parameter is actually a supplement to the input offset voltage. Within a given operating range, the magnitude of the drift of the amplifying circuit depends on the temperature changes.Input Bias CurrentWhen the output current voltage of the op amp is zero, input bias current refers to the average value of the bias current of the two input terminals that flows into the inverting and non-inverting input terminals of the Op-Amp. It has a greater impact on the places where the input impedance is required, and it is generally related to the manufacturing process. The smaller the input bias current the smaller the drift.Input Offset CurrentWhen the output current voltage of the op amp is zero, input offset current means the difference between the bias currents of the two input terminals. It also reflects the symmetry of the circuit inside the op amp. The better the symmetry, the smaller the input offset current.Input Resistance1) Differential mode input impedance: when the operational amplifier is working in the linear region, it is the ratio of the voltage change at the two input terminals to the corresponding current change. It includes input resistance and input capacitance, and only refers to input resistance at low frequencies.2) Common mode input impedance: It is the ratio of the input current change when the op amp is inputting a signal, that is, the same signal is input at the two input terminals of the op amp. At low frequencies, it appears as a common-mode resistance.Output ResistanceWhen the operational amplifier works in the linear region, a voltage signal is added to the output terminal of the operational amplifier, output resistance means the ratio of the voltage change to the corresponding current change. At low frequencies, it only refers to the output resistance of the op amp. This parameter needs to be tested in an open loop state.Voltage Gain1) Open-loop gain: the amplification factor of the op amp without negative feedback (in open loop state). The ideal value is infinite, generally about thousands to tens of thousands of times, and it represents by dB and V/mV.2) Closed-loop gain: in the case of negative feedback, it refers to the amplifier magnification.Voltage SwingWhen the op amp is working in the linear region, voltage swing is the maximum voltage amplitude that the op amp can output under the specified load and the current power supply voltage.Input Voltage Range1) Differential mode input voltage range: The maximum differential mode input voltage is defined as the maximum allowable input voltage difference between the two input terminals of the operational amplifier. When the input voltage difference of the op amp exceeds it, the input stage of the op amp may be damaged.2) Common mode belongs to the rabbit voltage range: when the operational amplifier is working in the linear region, when the common mode rejection ratio of the operational amplifier deteriorates significantly is the maximum common mode input voltage. It limits the maximum common-mode input range in the input signal, therefore, special attention is required in the case of interference.Slew RateThe slew rate of the op amp is defined as the input of a large signal (including a step signal) to the input under the closed loop condition. It indicates how fast the output of OP-AMP can change in response to change in input frequency. The output rise rate of the op amp is measured from the output of the op amp. Since the op amp is in a closed loop state during conversion, the feedback loop of the op amp does not work, that is to say, the slew rate has nothing to do with the closed loop gain.CMRRThe Common Mode Rejection Ratio (CMRR) is defined as the ratio of the differential voltage gain to the common-mode voltage gain.Unity GainA unity gain amplifier is an amplifier that has a gain of 1 that also means there is no gain. The output voltage will be the same as the input voltage it is commonly known as a voltage follower amplifier.Common Mode Rejection RatioWhen the op amp works in the linear region, it means the ratio of the differential mode gain of the op amp to the common mode gain. It is an extremely important indicator, it suppresses differential mode interference signals. Since the common-mode rejection ratio is very large, the common-mode rejection ratio of most op amps is recorded and compared in decibels.Supply Voltage Common Mode Rejection RatioWhen the op amp works in the linear region, it means the input offset current of the op amp varies with the supply voltage. Supply voltage common mode rejection ratio reflects the impact of power supply changes on the output of the op amp. Pay special attention when used for DC signals or small signals.Equivalent Input VoltageA well-shielded op amp without signal input, any AC interference voltage generated at its output end, when this noise is converted to the input of the op amp, it is called the input noise voltage (sometimes also expressed by noise current).2.2 Questions about Op Amp Important ParametersWhy do op amps need negative voltage?Op-amps themselves don't have a 0V connection but their design assumes the typical signals will be more towards the center of their positive and negative supplies. Thus, if your input voltage is right at one extreme or forces the output toward one supply, chances are it won't work properly. Why op amp has high gain?The gain of an op amp represents how much greater in magnitude its output will be than its input, hence its amplification factor. This is usually defined as an open-loop gain or large signal voltage gain. Why Positive feedback is not used in op amp?In an op-amp circuit with no feedback, there is no corrective mechanism, and the output voltage will saturate with the tiniest amount of differential voltage applied between the inputs. What is CMRR?The Common Mode Rejection Ratio (CMRR) is defined as the ratio of the differential voltage gain to the common-mode voltage gain. CMRR is infinity. Why CMRR should be high?A high CMRR is required when a differential signal must be amplified in the presence of a possibly large common-mode input, such as strong electromagnetic interference (EMI). An example is audio transmission over balanced line in sound reinforcement or recording. What is the maximum gain of op amp?The maximum gain is the open loop gain. It depends on the opamp model, and can go anywhere from 60 dB to 120 dB voltage gain. The open-loop bandwidth is however very small. Another issue is that this gain is very variable between different parts of the same product number due to variations. What is slew rate of op amp?Slew rate (SR) is the maximum rate of voltage change that can be generated by the op-amp's output circuitry. It is measured as voltage relative to time, and the typical unit used in datasheets is volts per microsecond (V/µs). SR is infinity, which means the ideal op-amp will produce a change in the output instantly in response to an input step voltage. What is bandwidth of an operational amplifier?The operational amplifiers bandwidth is the frequency range over which the voltage gain of the amplifier is above 70.7% or -3dB (where 0dB is the maximum) of its maximum output value as shown below. Is higher slew rate better?Higher slew rates are not always better: Higher slew rate makes for higher operating current. This means higher power consumption. Faster slew rate will make higher bandwith. Ⅲ Common Op-amp ICs Datasheet OverviewLM741The LM741 series are general-purpose operational amplifiers which feature improved performance over industry standards like the LM709. It is intended for a wide range of analog applications. It has only one op-amp inside. An operational amplifier IC is used as a comparator which compares the two signal, the inverting and non-inverting signal.Figure 1. LM741 Op Amp PinoutTable 1: LM741 SpecificationsMax supply voltage: ±22 VVoltage gain: 200V/mVMax input voltage: ±15 VBuilt-in output short circuit protectionMax output short circuit current is 40 mA.Input resistance: 6MMax low offset voltage of 6mv and can drift 15 µV/°CApplications include comparator, dc amplifier, summing amplifier, integrator or differentiators and active Filters.Max input offset current of 70nA and can drift up-to 0.5 nA/°C.Max Bandwidth is 1.5Mhz;Max Slew rate is 0.7 V/us.Max CMRR is 90 dB.Similar Products: UA741, µA741Max peak output voltage swing is 16VOperating temperature range –50 to 125 °C LM709 SeriesThe LM709 series is a monolithic operational amplifier in tended for general-purpose applications. The precursor to the popular LM741 is the LM709. The 709 had no internal frequency compensation, unlike the 741. Frequency compensation is used to purposely limit an operator's bandwidth. As the input frequency increases, the operator's phase shift also increases. This can contribute to unnecessary oscillation, as an unintended phase-shift oscillator forms the feedback network.Figure 2. LM709 Op Amp PinoutTable 2: LM709 SpecificationsMax supply voltage: ±18VInput resistance: 750KMax input voltage: ±10VOutput resistance: 150ΩMax low offset voltage of 6mv and can drift 6 µV/°CApplication includes voltage follower, basic comparator, multivibrator and frequency generator.Max input offset current of 500nA and can drift up-to 22.8 nA/°CPackage: TO-5, Pin Nb=8Max CMRR is 70dB.Similar parts: OP77, UA70Peak output voltage swing is 24VOperating temperature range –55 to 125 °C LM1458LM1458 is a dual general purpose Operational Amplifier (Op-amp). Its has two built-in amplifiers having common power supply, and short circuits protected and require no external components for frequency.Figure 3. LM1458 Op Amp PinoutTable 3: LM1458 SpecificationsMax supply voltage: ±18 VInput resistance: 1MΩMax input voltage: ±15VMax CMRR is 90dBvoltage gain: 15V/mVbuilt-in output short circuit protectionMax low offset voltage of 6mv and can drift 15 µV/°CInput offset current of 300nA max and can drift up-to 0.5 nA/°CMax peak output voltage swing is 14V.Max bandwidth is 1MHz.Operating temperature range 0 to 70 °CApplications include summing amplifiers, portable devices, comparators, integrators, etc.Similar Products: MC1458Packages have TO-CAN, DSBGA, SOIC and PDIP. LM324The LM324 series are low−cost, quad operational amplifiers with true differential inputs. They have several distinct advantages over standard op amps. It is a single supply, high gain, internally frequency compensated quad op amp. And it can be operated from a single or split power supplies.Figure 4. LM324 Op Amp PinoutTable 4: LM1324 SpecificationsMax supply voltage: 32 VOutput resistance: 350ΩVoltage gain: 100 V/mVMax output short circuit current is 60 mAInput bias current: 100nABuilt-in output short circuit protectionMax low offset voltage of 3mv and can drift 30µV/°CMax input offset current of 30nA and can drift up-to 300 pA/°CMax CMRR is 85dB.Max peak output voltage swing is 16V.Bandwidth is 1MHzOperating temperature range 0 to 70 °CPackages: 14-pin PDIP, 14-pin CDIP, 14-pin SOIC, and 14-pin TSSOP NE5532Compared to the standard dual op amps, the NE5532 is a Dual Low Noise Op-Amp in 8-pin package commonly used as amplifiers in audio circuits for its noise immunity and high output drive capability. The Op-Amp is internally compensated for high unity gain with maximum output swing bandwidth, low distortion and high slew rate.Figure 5. NE5532 Op Amp PinoutTable 5: NE5532 SpecificationsMax supply voltage: ± 15VInput bias current: 1000nAMax supply current: 10mALow offset voltage: 5 mVInput offset current: 200nABuilt-in output short circuit protectionMax output short circuit current is 60 mAInput resistance: 300KΩMax CMRR is 100dB.Output resistance: 0.3ΩMax peak output voltage swing is 26V.Max bandwidth is 10Mhz.Max slew rate is 9 V/us.Operating temperature range -65 to 150 °CApplications include Av Receivers, Audio mixer, High-performance audio preamplifier and many more.Ⅳ ConclusionOp amps are used in a wide variety of applications in electronics. Some of the more common applications are: as a voltage follower, selective inversion circuit, a current-to-voltage converter, active rectifier, integrator, a whole wide variety of filters, and a voltage comparator. Based on your circuit requirements, you should check out datasheets of different op-amps and select one.

IntroductionIn electronics, current sense amplifiers are special-purpose amplifiers that output a voltage proportional to the current flowing in a power rail. They are often referred to as current shunt amplifiers because they use a shunt resistor in the power rail that provides a small voltage drop when current flows through the resistor. These devices are designed to handle common-mode voltages that can exceed their own supply voltage. The working principle of a current sensing amplifier is based on Ohm's law (V = I × R), where the voltage drop across the sense resistor is converted and amplified to a measurable output voltage by the current sense amplifier.Ⅰ Current Sense Amplifier Overview1.1 What is a Current Sense Amplifier?Current sense amplifiers are designed for the specific purpose of amplifying very small sensed voltages across a shunt resistor, typically within a range of 10 to 100 mV. These amplifiers are optimized for DC precision (e.g., low input offset voltage, typically less than 50 µV) and high common-mode rejection ratio (CMRR). Current sensing amplifiers can measure current flowing in a single direction (unidirectional) or in both directions through the sensing resistor. When an amplifier is capable of detecting current flow in both directions, it is called a bidirectional current sensing amplifier. Modern current sense amplifiers also feature enhanced bandwidth (up to several MHz), low quiescent current (as low as 50 µA), and integrated protection features such as overcurrent detection and alert outputs.1.2 Common-Mode Voltage and CMRRCommon-mode voltage is critical for both standard amplifiers and current sense amplifiers. The common-mode voltage refers to the average voltage applied to the inputs of the amplifier. This parameter is crucial because the amplifier has a limited ability to distinguish and differentiate signals depending on the common-mode voltage level. A standard op-amp's input range is typically insufficient for precision current sensing operations. In current sense amplifiers, the common-mode voltage range often extends well beyond the actual supply voltage of the amplifier. For example, modern current sense amplifiers can achieve supply operating voltage ranges from -4 V to +80 V, with some specialized devices supporting ranges up to +120 V or even higher for automotive and industrial applications.Op-Amp CMRR (Common Mode Rejection Ratio) ExplainedThe CMRR (common-mode rejection ratio) is the ratio of differential gain to common-mode gain, typically expressed in decibels (dB). For an ideal op-amp, the CMRR is infinite, but in real circuits, it typically ranges from 80 to 120 dB for high-performance current sense amplifiers. A high CMRR means that the amplifier can effectively reject common-mode signals while accurately amplifying the differential signal. For a current sense amplifier, high CMRR is essential because it determines how well the amplifier can measure small differential voltages in the presence of large common-mode voltages. Modern current sense amplifiers achieve CMRR values exceeding 100 dB, enabling them to sense tiny voltage drops across shunt resistors even when the common-mode voltage is several orders of magnitude larger. The high CMRR also helps eliminate noise on the current sense lines, improving measurement accuracy and system reliability.1.3 Main Types of Current Sense AmplifiersHigh-side AmplifiersThe current is measured between the supply rail and the load. The DC voltage applied to the input pins can be much higher than the amplifier's power supply voltage. High-side sensing is preferred in applications requiring ground fault detection and load diagnostics.Low-side AmplifiersThe current is measured between the load and ground. The voltage applied to the input pins is close to ground potential. Low-side sensing is simpler to implement but can interfere with ground reference integrity.Bidirectional AmplifiersThese amplifiers can measure current flow in both directions, making them ideal for battery monitoring, motor control, and applications with regenerative braking.Integrated Current Sense Amplifiers with ADCModern devices integrate analog-to-digital converters (ADC) and digital interfaces (I²C, SPI) for direct microcontroller communication, simplifying system design.Figure 1. High-side Current Sensing AmplifierⅡ Current Sense Amplifiers vs Common AmplifiersCurrent sense amplifiers and common operational amplifiers have different specifications and are designed for specific purposes. Standard operational amplifiers typically cannot amplify very small differential voltages in the presence of large common-mode voltages and have relatively low CMRR (typically 80-90 dB). In contrast, precision current sense amplifiers can detect and amplify very small voltage drops (as low as a few millivolts) while maintaining high CMRR (100-120 dB or higher).For normal operational amplifiers, the input voltage must remain between the power supply rails (VCC and VEE), and the amplifiers can only operate on input signals within this range. In a standard amplifier, applying an external voltage beyond the power rails to the input pins will activate internal ESD protection diodes, potentially causing large currents to flow and damaging the device.However, current sense amplifiers are designed to handle input voltages that far exceed their supply voltage. For example, an amplifier powered by 3.3V or 5V can safely measure voltages on power rails operating at 12V, 24V, 48V, or even higher. These amplifiers use specialized input architectures and protection circuits that allow them to operate with high common-mode voltages. When the common-mode input voltage exceeds VCC, the amplifier employs advanced circuit techniques to maintain accurate measurements without damage. Some modern current sense amplifiers also feature integrated overcurrent detection, alert outputs, and enhanced EMI/RFI rejection for robust performance in noisy industrial and automotive environments. Ⅲ How to Design a Circuit Using Current Sense AmplifiersConsider a design example with a 12V, 1A power rail where high-precision current sensing is required. Current sense amplifiers provide an ideal solution for this application. However, proper component selection is critical for optimal performance.For this application, select a current sense amplifier rated for at least 12V common-mode voltage with sufficient bandwidth for the application (typically 100 kHz to 1 MHz for DC and low-frequency AC measurements). Choose between high-side and low-side sensing based on system requirements. High-side current sensing is preferred for detecting fault or short-circuit conditions while maintaining ground integrity. Low-side current sensing offers simpler implementation but disrupts the ground reference path.The LT6108 (now part of Analog Devices) is an excellent choice for this application. This amplifier features a wide input common-mode voltage range (-0.3V to +60V), high gain accuracy, and low offset voltage. The device can operate with supply voltages from 2.9V to 60V, making it suitable for both 12V and lower voltage control circuits. Key specifications include: input offset voltage of 50 µV (typical), CMRR of 125 dB (minimum), and bandwidth of 500 kHz.Figure 2. LT6108 Circuit for Fault Protection with Fast Latching Load DisconnectThe circuit above demonstrates a practical implementation using the LT6108. A 1-ohm sense resistor creates a voltage drop proportional to the load current (1V drop at 1A). The IRF9640 P-channel MOSFET serves as the switching element, while the 2N2222 NPN transistor (note: 2N2700 in the original text appears to be a typo) provides the control function. The amplifier output can trigger the switching MOSFET to disconnect the load when current exceeds a preset threshold. In this configuration, the trip point is set at 250 mA. The circuit will open when current exceeds this limit, providing overcurrent protection. For different current thresholds (e.g., 1A), adjust the voltage divider network at the comparator input. The VOUT pin provides a voltage proportional to the sensed current, enabling real-time current monitoring. This circuit topology can be adapted using other current sense amplifiers with appropriate input voltage ranges. For higher voltage applications (24V, 48V), select amplifiers with extended common-mode voltage ranges, such as the INA240 (up to 80V) or MAX40080 (up to 60V).Design Considerations:Sense Resistor Selection: Choose a value that provides adequate voltage drop (typically 50-100 mV at full scale) while minimizing power dissipation. For 1A measurement, resistor values between 0.05Ω and 0.1Ω are common.PCB Layout: Use Kelvin connections to the sense resistor to eliminate errors from trace resistance. Keep traces short and symmetric to minimize offset errors.Filtering: Add input filtering capacitors (typically 0.1 µF ceramic) close to the amplifier inputs to reduce noise and improve stability.Gain Setting: Many current sense amplifiers offer programmable gain through external resistors, allowing optimization for specific current ranges. Ⅳ Common Applications of Current Sensing ICs4.1 Low-side Current Sense ICLow-side current sensing places the shunt resistor between the load and ground. This configuration measures current by monitoring the voltage drop across the sense resistor in the ground return path. The diagrams below demonstrate low-side measurement circuits.Practical implementations include using the INA181 current sense amplifier with its output connected to an ADC (Analog-to-Digital Converter) for digital processing. Another approach employs the AD8202 current sense amplifier from Analog Devices for sensing current through inductive loads. Modern alternatives include the INA190 series and MAX9938, which offer enhanced precision and lower power consumption.1) AdvantagesLow-side current measurement offers several benefits. The configuration is straightforward to implement because the common-mode voltage remains close to ground potential. Standard operational amplifiers or simple differential amplifiers can be used since high common-mode rejection is not critical. The low common-mode voltage simplifies circuit design and reduces component costs. Additionally, low-side sensing typically provides better noise immunity in the measurement path.2) DisadvantagesThe primary limitation of low-side current measurement is the disruption of the ground reference. Placing the shunt resistor in series with the ground path means the load no longer has a direct connection to system ground. This can cause ground bounce issues, interfere with proper operation of the load, and make it impossible to detect ground faults or short circuits to ground. Additionally, low-side sensing cannot detect leakage currents or faults that bypass the sense resistor. For these reasons, high-side sensing is often preferred in safety-critical applications.4.2 High-side Current Sense ICUnlike low-side current sensing, high-side current sensing places the shunt resistor between the positive power supply and the load. This configuration preserves ground integrity while enabling current measurement. The circuits shown below illustrate high-side current sensing implementations.Practical examples include the TI INA240, which provides analog output or integrated comparators for overcurrent detection. Some variants offer digital output via I²C interface for direct microcontroller communication. The Linear Technology LT6100 (now Analog Devices) demonstrates high-side current sensing with a fused load for enhanced protection. Modern alternatives include the INA226 (with integrated 16-bit ADC and I²C interface), MAX40080 (with integrated 12-bit ADC), and INA3221 (triple-channel monitor for multi-rail systems).Figure 3. TI INA240 in Circuit1) AdvantagesHigh-side current measurement offers significant advantages over low-side sensing. First, it maintains ground integrity, ensuring the load has a solid ground reference. This prevents ground bounce and interference issues. Second, it enables detection of all fault conditions, including short circuits to ground, since all current must flow through the sense resistor. Third, high-side sensing allows accurate measurement of the actual load current without ground path interference. Fourth, it provides better system diagnostics and fault isolation capabilities. Finally, high-side sensing is essential for battery monitoring applications where the negative terminal is grounded.2) DisadvantagesThe primary challenge of high-side current sensing is the requirement for high common-mode rejection. The small differential voltage (typically 50-100 mV) across the shunt resistor sits on top of a large common-mode voltage equal to the supply rail voltage. This requires specialized amplifiers with high CMRR (>100 dB) and wide common-mode input ranges. Additionally, high-side sensing circuits are typically more complex and expensive than low-side alternatives. However, advances in integrated circuit technology have made high-side current sense amplifiers increasingly affordable and easy to implement.4.3 Bidirectional Current Sense ICBidirectional current sense circuits use a single shunt resistor but require amplifiers capable of detecting current flow in both directions. These circuits are essential for applications such as battery charge/discharge monitoring, motor control with regenerative braking, and power management systems with bidirectional power flow.Several architectures enable bidirectional current sensing. One approach uses two current sense amplifiers (such as the INA300) connected in a configuration where each amplifier detects current flow in one direction. The circuit requires reverse polarity protection and switching logic to select the appropriate amplifier output based on current direction.A more elegant solution uses integrated bidirectional current sense amplifiers such as the INA240, INA180, or MAX40080. These devices use a reference voltage (typically mid-supply or an external reference) as the zero-current point. When current flows in one direction, the output voltage rises above the reference; when current reverses, the output falls below the reference. The differential output voltage is proportional to current magnitude, while the polarity indicates current direction.Modern bidirectional amplifiers like the INA226 and INA3221 integrate ADCs and digital interfaces, providing signed current measurements directly to microcontrollers. These devices simplify system design by eliminating external ADCs and reference voltage circuits. For high-precision applications, devices like the MAX40080 offer 12-bit resolution with ±0.1% accuracy across the full bidirectional range.4.4 Isolated Current Sense ICIsolated current sensing techniques provide galvanic isolation between the current measurement circuit and the control electronics. This is essential for high-voltage applications, safety-critical systems, and situations requiring ground loop elimination. Several isolation methods are available:Current Transformer (CT) Isolation: Uses magnetic coupling through a transformer core. The primary winding carries the measured current, inducing a proportional voltage in the secondary winding. This method is limited to AC current measurement and provides excellent isolation (typically >4 kV).Hall Effect Sensors: Measure the magnetic field generated by current flow through a conductor. Hall effect sensors can measure both DC and AC currents and provide good isolation. Examples include the ACS712, ACS724, and TMCS1100 series.Isolated Amplifiers: Use capacitive or magnetic isolation to transmit the measurement signal across an isolation barrier. Examples include the AMC1200 (capacitive isolation), Si8920 (magnetic isolation), and ACPL-C87A (optical isolation). These devices typically provide 3-5 kV isolation and can measure both DC and AC currents.Rogowski Coils: Air-core coils that measure the rate of change of current (di/dt). These are ideal for high-frequency AC current measurement and provide inherent isolation.Isolated current sensing is mandatory in applications such as motor drives, solar inverters, electric vehicle charging systems, and industrial power monitoring where high voltages and safety requirements necessitate galvanic isolation between measurement and control circuits.Figure 4. Low-side Current Sensing CircuitⅤ Key Specifications and Selection CriteriaWhen selecting a current sense amplifier, consider the following critical specifications:Common-Mode Voltage Range: Must exceed the maximum voltage on the power rail being monitored. Include margin for transients and voltage spikes.Input Offset Voltage: Determines minimum detectable current. Lower offset voltage (typically <50 µV) enables accurate measurement of small currents.CMRR: Higher values (>100 dB) provide better rejection of common-mode noise and more accurate differential measurements.Bandwidth: Must be sufficient for the application. DC to 100 kHz for most power monitoring; 1 MHz or higher for motor control and fast transient detection.Gain Options: Fixed or programmable gain allows optimization for specific current ranges.Supply Voltage: Must be compatible with system power rails. Many devices operate from 2.7V to 5.5V for easy integration with digital systems.Quiescent Current: Important for battery-powered applications. Modern devices offer quiescent currents as low as 50 µA.Package and Size: SOT-23, SOIC, and DFN packages are common. Smaller packages reduce PCB footprint but may have thermal limitations.Integrated Features: Some devices include comparators, ADCs, digital interfaces (I²C, SPI), alert outputs, and overcurrent protection.Temperature Range and Accuracy: Industrial (-40°C to +125°C) and automotive (-40°C to +150°C) grades are available. Temperature drift should be <2 µV/°C for precision applications.Ⅵ Emerging Trends and Future DevelopmentsThe current sense amplifier market continues to evolve with several notable trends:Higher Integration: Modern devices integrate ADCs, digital interfaces, voltage monitors, and power calculation engines on a single chip, reducing component count and system cost.Wider Voltage Ranges: New amplifiers support common-mode voltages up to 120V or higher, enabling direct monitoring of high-voltage rails without external attenuation.Lower Power Consumption: Shutdown modes and ultra-low quiescent current (<50 µA) enable use in battery-powered IoT devices and energy harvesting applications.Enhanced Accuracy: Improved manufacturing processes deliver offset voltages below 25 µV and gain errors below 0.1%, enabling precision measurements with smaller sense resistors and lower power loss.Automotive Qualification: AEC-Q100 qualified devices for electric vehicles, battery management systems, and 48V automotive systems.Digital Configurability: Software-programmable gain, filtering, and alert thresholds enable flexible, adaptive current monitoring systems.Multi-Channel Integration: Devices like the INA3221 integrate multiple current sense channels for simultaneous monitoring of multiple power rails.Ⅶ ConclusionAs an essential component of modern electronics, current sense amplifiers provide high-precision, flexible solutions for a wide array of applications including automotive systems, power management, battery monitoring, motor control, and industrial automation. Devices like the INA280, INA226, MAX40080, and LT6108 offer high-precision current measurement capabilities by accurately sensing voltage drops across shunt resistors. With diverse circuit requirements, a broad range of current sense amplifiers are available, including high-voltage, high-resolution, bidirectional, and isolated variants. The continued evolution of current sense amplifier technology—featuring higher integration, wider voltage ranges, lower power consumption, and enhanced digital connectivity—ensures these devices will remain critical components in next-generation power management and monitoring systems. When selecting a current sense amplifier, carefully consider application requirements including voltage range, accuracy, bandwidth, power consumption, and integration features to ensure optimal performance and system reliability. Frequently Asked Questions about Current Sense Amplifier Circuits1. What is a current sense amplifier?Current sense amplifiers (also called current shunt amplifiers) are special-purpose amplifiers that output a voltage proportional to the current flowing in a power rail. They utilize a "current-sense resistor" (shunt resistor) to convert the load current in the power rail to a small voltage, which is then amplified by the current sense amplifier. The currents in the power rail can range from milliamps to 20 A or more, requiring the current-sense resistor to be typically in the range of 1 mΩ to 100 mΩ. These amplifiers are specifically designed to handle high common-mode voltages while accurately measuring small differential voltages. 2. How does a current sense amplifier work?Current sense amplifiers work by measuring the small voltage drop across a shunt resistor placed in series with the load current. According to Ohm's law (V = I × R), the voltage drop is directly proportional to the current. The amplifier's differential inputs measure this voltage drop while rejecting the large common-mode voltage present on the power rail. The amplifier then amplifies the differential signal to produce an output voltage that can be easily measured by ADCs or comparators. Unlike normal differential amplifiers that are powered between two power supply rails (VCC and VEE) and can only handle signals between these rails, current sense amplifiers use specialized input stages that can tolerate input voltages far exceeding their supply voltage without activating ESD protection diodes or causing damage. 3. What are the main types of current sense amplifiers?The main types of current sense amplifiers include:High-Side Current Sense: Measures current between the power supply and load, maintaining ground integrity.Low-Side Current Sense: Measures current between the load and ground, offering simpler implementation.Bidirectional Current Sense: Measures current flow in both directions, essential for battery monitoring and regenerative systems.Isolated Current Sense: Provides galvanic isolation using magnetic, capacitive, or optical coupling for high-voltage and safety-critical applications. 4. What is the main purpose of a current sense amplifier?The main purpose of a current sense amplifier is to accurately measure current flow in power rails by amplifying the small voltage drop across a shunt resistor. These amplifiers can detect and amplify very small voltages, typically in the 10 to 100 mV range, while rejecting large common-mode voltages. Applications include power management, battery monitoring, motor control, overcurrent protection, system diagnostics, and energy measurement. Current sense amplifiers enable precise current monitoring for efficiency optimization, fault detection, and system protection. They can measure current flowing in a single direction (unidirectional) or in both directions (bidirectional) through the sense resistor, depending on the application requirements. 5. What is the difference between a voltage amplifier and a current sense amplifier?While both are amplifiers, they serve different purposes and have distinct specifications. Standard voltage amplifiers (operational amplifiers) are general-purpose devices designed to amplify signals within their power supply rails. They typically have moderate CMRR (80-90 dB), input voltage ranges limited to their supply voltages, and are not optimized for measuring very small differential voltages in the presence of large common-mode voltages.Current sense amplifiers, in contrast, are specialized devices optimized for measuring small voltage drops across shunt resistors. They feature very high CMRR (100-120 dB or higher), ultra-low input offset voltage (<50 µV), and the ability to handle common-mode voltages far exceeding their supply voltage. For example, a current sense amplifier powered by 3.3V can safely measure voltages on a 48V power rail. Current sense amplifiers use specialized input architectures that prevent ESD protection diodes from conducting when input voltages exceed supply rails, enabling them to operate in high-voltage environments. They are specifically designed for DC precision, high common-mode rejection, and wide common-mode voltage ranges—characteristics essential for accurate current measurement in power management applications. 6. How do I select the right shunt resistor value?Shunt resistor selection involves balancing several factors: voltage drop, power dissipation, and measurement accuracy. The voltage drop should be large enough for accurate measurement (typically 50-100 mV at full-scale current) but small enough to minimize power loss. Use the formula R = V / I, where V is the desired voltage drop and I is the maximum current. For example, for 1A measurement with 50 mV drop: R = 0.05V / 1A = 0.05Ω (50 mΩ). Power dissipation is calculated as P = I² × R. For 1A through 50 mΩ: P = 1² × 0.05 = 0.05W (50 mW). Select a resistor with adequate power rating (typically 2-4× calculated power) and low temperature coefficient (<50 ppm/°C) for stable measurements. Consider resistor tolerance (typically 1% or better) as it directly affects measurement accuracy. 7. What are the key advantages of high-side vs. low-side current sensing?High-side sensing places the shunt resistor between the power supply and load, maintaining ground integrity and enabling detection of all fault conditions including ground shorts. It provides better system diagnostics but requires amplifiers with high CMRR and wide common-mode voltage range. Low-side sensing places the shunt resistor between load and ground, offering simpler implementation and lower cost since common-mode voltage is near ground. However, it disrupts ground reference and cannot detect ground faults. High-side sensing is preferred for safety-critical applications, battery monitoring, and systems requiring fault detection, while low-side sensing is suitable for cost-sensitive applications where ground disruption is acceptable. 8. Can current sense amplifiers measure AC current?Yes, many current sense amplifiers can measure AC current, provided their bandwidth is sufficient for the frequency of interest. The amplifier's bandwidth must be at least 10× the highest frequency component of the AC signal for accurate measurement. For example, measuring 60 Hz AC requires minimum 600 Hz bandwidth. Most modern current sense amplifiers offer bandwidths from 100 kHz to several MHz. For AC-only measurements (where DC component is not needed), current transformers or Rogowski coils provide better performance. For combined DC and AC measurement (such as motor current with PWM ripple), use a current sense amplifier with adequate bandwidth and consider adding filtering to reduce high-frequency noise while preserving the signals of interest.

IntroductionOperational amplifier (op amp for short) is basically a voltage amplifying device designed to be used with components like capacitors and resistors, between its in/out terminals, or is simply a linear Integrated Circuit (IC) having multiple-terminals. In electronics, the open-loop voltage gain of the actual operational amplifier is very large, which can be seen a differential amplifier with infinite open loop gain, infinite input resistance and zero output resistance. In addition, it has positive and negative inputs which allow circuits that use feedback to achieve a wide range of functions. And meanwhile, it can be further simplified into an ideal op amp model, referred to as an ideal op amp (also called ideal OPAMP).CatalogIntroductionⅠ Ideal Op Amp Characteristics1.1 Infinite Input Resistance1.2 Zero Output Impedance1.3 Infinite Open-loop Gain1.4 Infinite Common-mode Rejection Ratio1.5 Infinite BandwidthⅡ Assumptions of Ideal Op AmpⅢ Working Characteristics of Ideal Operational Amplifiers3.1 Work in Linear Region3.2 Work in Nonlinear RegionⅣ Analysis of Ideal Operational Amplifier CharacteristicsⅤ Balanced Resistance Presets5.1 The Role of Balanced Resistance5.2 Input Balancing Resistor ExplanationⅥ Ideal Op Amp EquationsⅦ Several Common Op Amp CircuitsⅧ Difference Between Ideal Op-amp and Practical Op-ampⅠ Ideal Op Amp CharacteristicsWhen analyzing various application circuits of operational amplifiers, the integrated operational amplifier is often regarded as an ideal operational amplifier. The so-called ideal op amp is to idealize various technical indicators of op amps, and it must have the following characteristics.Characteristics of An Ideal Op-Amp1.1 Infinite Input ResistanceThe input terminal of an ideal operational amplifier does not have any current to flow in. In electronics, op amps are voltage gain devices. They amplify a voltage fed into the op amp and give out the same signal as output with a much larger gain. In order for an op amp to receive the voltage signal as its input, the voltage signal must be dropped across the op amp. If you know the concept of a voltage divider, voltage drops primarily across components with high impedances, proportionally according to ohm’s law by the formula V=IR. So the greater the resistance (or impedance) of a device, the greater the voltage drop across that device is. To make sure that the voltage signal drops fully on the op amp, it must have a very high input impedance, so that the voltage drops fully across it. If it had a low input impedance, the voltage may not drop across it and it would not receive the signal. This is why op amps must have high-input impedances.It’s also easy to make the input impedance lower (put a resistor in parallel) or the source impedance higher (put a resistor in series).Figure 1. Ideal Op Amp Symbol and Transfer Characteristic Curve 1.2 Zero Output ImpedanceThe output of an ideal op amp is a perfect voltage source, no matter how the current flowing to the amplifier load changes, the output voltage of the amplifier is always a certain value, that is, the output impedance is zero. In practice, zero output impedance is actually a distinct property from infinite input impedance, but for a very long time infinite input impedance was approached only with compromises in offset voltage and noise. 1.3 Infinite Open-loop GainIn an open-loop state, the differential signal at the input has an infinite voltage gain. This feature makes the operational amplifier very suitable for practical applications with upper negative feedback configuration. 1.4 Infinite Common-mode Rejection RatioAn ideal operational amplifier can only respond to the difference between the voltages at both ends of V+ and V-. In addition, the same part of the two input signals (ie common mode signal) will be completely ignored. What’s more, a high CMRR is required when a differential signal must be amplified in the presence of a possibly large common-mode input, such as strong electromagnetic interference (EMI). An example is audio transmission over balanced line in sound reinforcement or recording. 1.5 Infinite BandwidthThe ideal operational amplifier will amplify the input signal of any frequency with the same differential gain, which will not change with the change of signal frequency.Ⅱ Assumptions of Ideal Op AmpThe op amp can be considered a voltage controlled current source, or it is an integrated circuit that can amplify weak electric signals. Based on it, for an ideal OPAMP, what is the relationship between it and these electrical signals?First, assume that the current flowing into the input of the op amp is zero. This assumption is almost completely correct for FET op amps, because the input current for FET op amps is below 1pA. But for dual high-speed op amps, this assumption is not always correct, because the input current of it can sometimes reach tens of microamperes.Second, assume that the gain of the op amp is infinite, so the op amp can swing the output voltage to any value to meet the input requirements. It means that the output voltage of the op amp can reach any value. In fact, when the output voltage is close to the power supply voltage, the op amp will saturate. Maybe this hypothesis does exit, but needs a limit in practical. For example, at higher frequencies, the internal junction capacitors of transistor come into play, thus reducing the output and therefore the gain of amplifier. The capacitor reactance decreases with increase in frequency bypassing the majority of output. The opamp is in saturation state.Figure 2. Op Amp SaturationFor example, as per datasheet of LM741, large signal voltage gain is 200V/mv. It means an open loop gain of 200,000. If you operate an op-amp in open-loop condition(i.e. without negative feedback) ,even microvolts of input voltage (input offset voltage of LM741 is 3mv) will drive the output to saturation.In most of the amplifier circuits op-amp is configured to use negative feedback which greatly reduces the voltage gain (i.e. closed loop gain). In oscillators and schmit triggers, Op-amp is configured to use positive feedback. Comparator circuit is an example of the circuit which utilizes open-loop gain of op-amp. Its output will be always at saturation either positive or negative saturation. In an integrator circuit, the DC gain should be limited by adding a feed back resistor in parallel with capacitor ;else the output will get saturated .Even in amplifier circuits, the amplitude of the input signal and the voltage gain of the circuit should be balanced so that the output voltage does not exceed power supply voltage . For example for a non-inverting amplifier with a voltage gain of 100, the maximum permissible input voltage will be 150 mv if the VCC is 15 Volts. If you apply a signal of 200 mv ,the op-amp output will goto saturation as the required output will be 20 volts which exceeds the VCC of 15 Volts.Third, the assumption of infinite gain also means that the input signal must be zero. The gain of the op amp will drive the output voltage until the voltage (error voltage) between the two input terminals is zero. The voltage between the two input terminals is zero. The zero voltage between two input terminals means that if one input terminal is connected to a hard voltage source like ground, the other input terminal will also be at the same potential. In addition, since the current flowing into the input terminal is zero, the input impedance of the op amp is infinite.Fourth, of course, the output resistance of an ideal op amp is zero. An ideal op amp can drive any load without any voltage drop due to its output impedance. At low currents, the output impedance of most op amps is in the range of a few tenths an ohm, so this assumption is true in most cases. Ⅲ Working Characteristics of Ideal Operational Amplifiers3.1 Work in Linear RegionWhen the ideal op amp works in the linear region, the output and the input voltage show a linear relationship. Where u0 is the output voltage of the integrated op amp; u+ and u- are the voltages at the non-inverting input terminal and the inverting input terminal, respectively. Auo is the open loop differential voltage magnification. According to the characteristics of the ideal op amp, two important characteristics of the ideal op amp in the linear region.1) Zero differential input voltageSince the open-loop differential voltage magnification of an ideal op amp is equal to infinity, and the output voltage is a certain value, the voltage values at the non-inverting input terminal and the inverting input terminal are approximately equal. Just like short circuit between input and output, but it is fake. Because it is an equivalent short circuit, not a real short circuit, so this phenomenon is called "virtual short".2) Zero input currentSince the open-loop input resistance of an ideal op amp is infinite, no current flows into the op amp at either input. At this time, the current at the non-inverting input terminal and the inverting input terminal are both equal to zero. Like an disconnection, but an equivalent disconnection, so this phenomenon is called "virtual break". Virtual short and virtual break are two important concepts for analyzing the ideal op amp working in the linear region.In fact, the ideal operational amplifier has the characteristics of "virtual short" and "virtual break". These two characteristics are very useful for analyzing linear amplifier circuits. The necessary condition for virtual short is negative feedback. When negative feedback is introduced, at this time, if the forward terminal voltage is slightly higher than the reverse terminal voltage, the output terminal will output a high voltage equivalent to the power supply voltage after the amplification of the op amp. In fact, the op amp has a respond time changing from the original output state to the high-level state (the golden rule of analyzing analog circuits: the change of the signal is a continuous change process). Due to the feedback resistance of the reverse end change will inevitably affect its voltage, when the reverse end voltage infinitely close to the forward end voltage, the circuit reaches a balanced state. The output voltage does not change anymore, that is, the voltage at the forward end and the reverse end is always close. (Note: The analysis method is the same when the voltage decreases.) 3.2 Work in Nonlinear RegionWhen the op-amp operates in the nonlinear region, the output voltage no longer increases linearly with the input voltage, but saturates. The ideal op amp also has two important characteristics when operating in the nonlinear region.1) When u+ ≠ u-, the output voltage of the ideal op amp reaches the saturation value.When u+ > u-, the op-amp operates works in positive saturation region with a positive output voltage.When u+ < u-, the op-amp operates works in negative saturation region with a negative output voltage.Ideal op amp operates in the nonlinear region, u+ ≠ u-, there is no “virtual short”.2) The input current is equal to zero.Although the input voltage u+ ≠ u- above, the input current is considered to be zero. Ⅳ Analysis of Ideal Operational Amplifier CharacteristicsAs for Op-amp, there's probably a description like this: three-terminal element (circuit structure with double-ended input, single-ended output), ideal transistor, high-gain DC amplifier.(1) High input resistanceUnder this situation, the current flowing into the input terminal is close to 0, almost no signal source current is used, which is close to the voltage control characteristic. And virtual break is derived from this.(2) Lower output resistanceIt has the characteristics of adapting to any load. And the impedance of the subsequent load circuit will not affect the output voltage.(3) Infinite voltage amplification(4) Under a certain supply voltage condition, the amplifier can only work in closed-loop (negative feedback) mode, and the actual amplification is limited. Because op-amps themselves don't have a 0V connection but their design assumes the typical signals will be more towards the center of their positive and negative supplies. Thus, if your input voltage is right at one extreme or forces the output toward one supply, chances are it won't work properly. Working in open-loop mode is the like a comparator, and the output is high level orlow level.In the closed-loop (limited amplification) state, the amplifier is randomly compare the potentials of the two input terminals. The output stage makes immediate adjustments when they are not equal. So the final purpose of amplification is to make the potentials of the two input terminals equal. And virtual short is derived from this. Ⅴ Balanced Resistance Presets5.1 The Role of Balanced Resistance1) A suitable resistance is generally required to ensure that the input impedance is matched.2) In order to reduce the input current imbalance, the in-phase resistor should be equal to the parallel value of the two resistors at the reverse end in theory. In practice, as a result of the closed loop, especially in deep negative feedback conditions, the misalignment is not obvious at the output. And there is no need of in-phase grounding resistor when the misalignment is not the main problem. Because a balanced resistor is the starting point for an ideal op amp. In-phase grounding resistance is useful for bipolar op amps, and has no meanings for MOS-type op amps.3) Ground input termination resistance: it is necessary for impedance matching and high frequency setting.4) Bias current and offset current.For operational amplifiers with bias current greater than offset current, input resistance matching can be reduced, and precision circuits can compensate bias current to a minimum. If the bias current and offset current are similar, the matching resistance will increase the error.5) Set for the bias current at the input, the purpose of which is to equalize the impedance of the invertingand non-inverting inputs, so that two inputs with equal bias currents are assumed to have equal voltage drops, thereby counteraction can be made. 5.2 Input Balancing Resistor ExplanationA op-amp is connected to an inverting amplifier:Set the input resistance for R1, feedback resistance for Rfi,Assume that the non-inverting end is not connected to a balanced resistor, but grounded directly.Set the input bias current for the op-amp IB (same voltage in inverting and non-inverting end).The current flows through R1 and Rf are represented by I1 and If.Inverting voltage is V-, The op-amp gain is A.Use KCL in the inverting end (set the input signal to 0).Where (0-V-)/R1- (A+1)V- /Rf=IBFrom the above equation, it follows that V-=-(IB×R1×Rf/(Rf+(A+1)R1))At this time, the output voltage of the op-amp is Vo=A×(IB×R1×Rf/(Rf+(A+1)R1))The above formula can be approximated as Vo=IB×((A×R1)/Rf)If the in-phase terminal passes through a resistor R2 to ground and R2=R1/Rf, then the voltage at the in-phase terminal is V+=-IB×R2KCL is applied to the inverted terminal, where (0-V-)/R1+(A×(V+-V-)-V-)/Rf=IBAt this time the output voltage of the op-amp is Vo=0. Ⅵ Ideal Op Amp EquationsUnderstanding the basic conditions of an ideal op amp, and combining it with the Kirchhoff's current law (KCL) node voltage method and the superposition theorem of the node, is an effective method to analyze the ideal op amp circuit.As shown below, find the output voltage uoFigure 3. OPAMP Circuit1) Equation based on KCLFrom the concept of virtual break, i+=i-=0, then i1=i2, i3=i4, so (a)Based on virtual break, u+=u-, then (b)2) Node voltage methodList the node voltage equations for node 1 and node 2, and get (c)Note: Because the output current of the op amp is unknown at 1) and 2), it is not possible to list the KCL equation or node voltage equation at the output of the op amp. In addition, the op amp output uo in 2) should be treated as an independent voltage source. 3) Superposition theoremWhen there are multiple signal inputs, choosing the superposition theorem to solve can simplify the analysis and calculation process. The size of the output signal uo can be regarded as the superposition of the output signal obtained by the independent action of u1 and u2. When u1 acts alone, the u2 terminal is grounded, and the op amp output is: (d)Therefore, the final output of the operational amplifier is:   (e) Ⅶ Several Common Op Amp CircuitsNon-inverting Amplifier CircuitA non-inverting amplifier is an op-amp circuit configuration which produces an amplified output signal. It provides a high input impedance along with all the advantages gained from using an operational amplifier. Inverting Amplifier CircuitAn inverting amplifier (also known as an inverting operational amplifier or an inverting op-amp) is a type of operational amplifier circuit which produces an output which is out of phase with respect to its input by 180 degrees out of phase with respect to input signal. In the following figure, two external resistors to create feedback circuit and make a closed loop circuit across the amplifier. Op-amp as AdderAn adder circuit can be made by connecting more inputs to the inverting op amp. The circuit diagram of a summing amplifier is as shown in the following figure. Differential AmplifierDifferential amplifier is an analog circuit with two inputs and and one output in which the output is ideally proportional to the difference between the two voltages. It is a very useful op-amp circuit and by adding more resistors in parallel with the input resistors as shown in the following. Composite AmplifierThe composite amplifier is termed as a combination of multiple operational amplifiers that are cascaded together with a negative-feedback loop around the entire network. The resistance in the circuit is generally selected at the K ohm level, the ratio of the resistance affects the gain and bias, in addition, the supply current, frequency response and capacitive load driving capability of the op amp determine their specific values in circuits. If it is used in a high-frequency circuit, the resistance needs to be reduced to obtain a better high-frequency response, but it will increase the input bias current, thereby increasing the current of the power supply. Ⅷ Difference Between Ideal Op-amp and Practical Op-ampIdeal op amps use no power, have infinite input impedance, unlimited gain-bandwidth and slew rate, no input bias current, and no input offset. They have unlimited voltage compliance.Practical op amps consume some power, have very high input impedance have limited gain-bandwidth and limited slew rate, have some input bias current and input offset voltage. Voltage compliance is limited by the power supply rail, or frequently even less.Still practical op amps are very useful because most of the limitations listed above are way better than what your circuit needs.For an ideal amplifier, it does not draw any current at all from its input. Assuming a two input amplifier the signal current in both input probes is zero. In other words the input impedance must be infinite. The output, should operate as the output of an ideal voltage source. This means that the potential between the output and the ground must be A(v2−v1), no matter how much current would a load connected to the output would draw. In other words the output impedance must be zero.For a real amplifier, the input impedance must be as large as possible while the output impedance must be as low as possible.In fact, An op-amp in real life, however, cannot operate with zero current flow. Frequently Asked Questions about Ideal Op Amp1. What is characteristic of ideal opamp?Ideal op amps will have infinite voltage gain, infinitely high impedance, zero output impedance, its gain is independent of input frequency, it has zero voltage offset, its output can swing positive or negative to the same voltages as the supply rails, and its output swings instantly to the correct value. 2. How does an ideal op amp work?An operational amplifier, or op amp, generally comprises a differential-input stage with high input impedance, an intermediate-gain stage, and a push-pull output stage with a low output impedance (no greater than 100 Ω). ... Open-loop voltage gain runs very high, on the order of 1 million. 3. Why are op amps not ideal?Op-amps with FET inputs have an Ibias that is so small that this method becomes less practical. Instead of measuring the voltage drop across a resistor, one can monitor the change in voltage across a capacitor as it is charged by the bias current. 4. How are real op amps different from ideal op amps?In real op amps, the amplified signal will not fully reach the DC supply rails. They will fall short of it. In an ideal op amp, the output will swing instantly to the amplified voltage value. There will be no time delay between the time the voltage is input into the op amp till the time it is output. 5. What are the four main ideal characteristics of an open-loop op amp?An ideal op amp is usually considered to have the following characteristics:Infinite open-loop gain G = vout / vInfinite input impedance Rin, and so zero input currentZero input offset voltageInfinite output voltage rangeInfinite bandwidth with zero phase shift and infinite slew rateZero output impedance R

IntroductionIn electronics, operational amplifiers are generally dual/quadruple configurations. So users can consider using the extra amplifier as a comparator. Electrical symbols of the comparator and the operational amplifier are very similar. They are devices with one input inverting terminal and one non-inverting terminal, and one output terminal. In addition, the output voltage range of the output terminal is generally between the rail-to-rail power supply. Meanwhile, they have same features of low bias voltage, high gain and high common-mode rejection ratio. When an op amp is used as a comparator, its own gain bandwidth product, group delay, slew rate and other parameters are likely to be changed due to internal frequency compensation and saturation effects. For an optimized single device, this change can be seen as an economical solution. This article discusses the specifications and characteristics to consider when using op-amps as comparators and provides design advice. How operational amplifier be a comparator and what the difference between them.Op Amp vs ComparatorCatalogIntroductionⅠ Operational Amplifier and Comparator1.1 Electronic Op Amp1.2 Electrical ComparatorⅡ Circuit Structure Comparison2.1 Op Amp2.2 ComparatorⅢ Difference between Amplifier and Comparator3.1 Total Difference Summary3.2 Distinctions between Op-amp and ComparatorⅣ Basic Use of Comparators and Op AmpsⅤ Op-amp Comparator5.1 Technique5.2 Op Amp Comparators DisadvantagesⅥ Using Op Amps as Comparators NotesⅦ ConclusionⅠ Operational Amplifier and Comparator1.1 Electronic Op AmpThe operational amplifier is a kind of differential amplifiers with high input resistance, low output resistance, high open gain (open-loop gain), and has the function of amplifying the voltage difference between the active input pin and the negative input pin. Operational amplifiers and voltage comparators are indeed the same in principle and diagram symbol. That said, they have 5 pins: two of which are power supply (+) and supply power (-), another two pins are non-inverting input (+) and non-inverting input terminal (-), and the last pin is the output terminal.Figure 1. Op Amp Symbol1.2 Electrical ComparatorComparing two or more data items to determine whether they are equal, or determining the  relationship and arrangement order between them is called comparison. A circuit or device that can realize this is called a comparator. Specifically, it is a circuit that compares an analog voltage signal with a reference voltage. The two inputs of the comparator are analog signals, and the output is a binary signal 0 or 1. When the difference of the input voltage increases or decreases and the sign of the positive and negative remains unchanged, the output remains constant. Comparing the voltages of the two input terminals, if the voltage at the positive input terminal is a and the voltage at the negative input terminal is b, when a>b, the output is high level(logic 1); when a<b, the output is low level(logic 0). The schematic diagram is shown below (the voltage at the input terminals of the comparator is IN1 and IN2, the power supply is VCC/GND, the pull-up resistor is 1K, and the pull-up voltage is VCC.).Figure 2. Volatge ComparatorWhen output voltage IN1＞IN2, positive input is in high level with high voltage.When output voltage IN2＞IN1, negative input is in low level with high voltage.A reference voltage is usually applied to an input terminal. Then the output will indicate the  signal applied to the other input. Comparators are often used to determine whether a signal is above or below the reference level. And meawhile, the comparator can form a non-sinusoidal waveform conversion circuit and be used in fields such as analog and digital signal conversion.When the reference voltage is zero, the comparator is called a zero-crossing detector. It uses to convert a sine wave into a square wave. Two comparators can form a "window" circuit, which is used to determine whether a signal is between two limited values. In an output state of the comparator changes as quickly as possible, and sometimes the output of the comparator is required to have a certain logical relationship with the input, a dedicated strobe pulse is required. At this time, the op amp comparator only has an output during operation. In general, a dedicated comparator IC has better performance. And it replaces the operational amplifier in some applications. The most common advantage is that the comparator IC operates with a single power supply.The comparator has a wide range of uses, and can be used for discrete control of voltage signals such as thermistors and photosensitive sensors. For example, the voltage value of the photoresistor is collected by a comparator to determine whether it is day or night. What’s more, the comparator can also be used for voltage adjustment in an analog negative feedback circuit.Figure 3. TLC311 ComparatorIt can be seen from the diagram that the difference between the operational amplifier and the comparator lies in the output circuit. The operational amplifier uses a dual-transistor push-pull output. While the comparator uses only one transistor, the collector is connected to the output terminal, and the emitter is grounded. In addition, the comparator requires an external pull-up resistor from the positive power supply terminal to the output terminal, which is equivalent to the collector resistance of the transistor. Op amp can be used for linear amplifying circuit (negative feedback), as well as the non-linear signal voltage comparison (open-loop or positive feedback). The comparator can only be used for signal voltage comparison, not for linear amplifier circuits (because it has no frequency compensation). Both can be used for signal voltage comparison, but the comparator is designed as a high-speed switch, which has a faster conversion rate and a shorter delay than an operational amplifier. Ⅱ Circuit Structure Comparison2.1 Op AmpFigure 4. Op Amp CircuitOp amp circuit generally consists of input segment, gain segment, and output segment. The input  is composed of a differential amplifier section for amplifying the voltage difference between two pins. In addition, the in-phase signal component (the state where there is no potential difference between the pins and the input voltage is some) is not amplified to take a cancellation effect. If only relying on the differential amplifier circuit, the gain is insufficient, so the gain section is used to further increase the open gain of the operational amplifier.The anti-vibration phase compensation capacitor is connected between the gain section of the ordinary operational amplifier. In order to avoid changes in the characteristics of the operational amplifier due to loads such as resistors connected to the output pins, a compensation capacitor is connected with the output as a buffer.The change (distortion, voltage drop, etc.) in output characteristics caused by the load is mainly determined by the circuit structure and current capability of the output section.Generally, types of output circuit stages are A, B, C, and AB type, which are classified according to the amount of drive current flowing in the output (the difference in bias voltage). Depending on the amount of drive current, the level of distortion coefficient in the output section will change. The order of general circuit distortion from small to large is type A, type AB, type B, and type C. 2.2 ComparatorFigure 5. Comparator CircuitThe comparator circuit structure is basically the same as that of an operational amplifier. Because a negative feedback circuit is not used, there is no built-in phase compensation capacitor for vibration isolation. Owing to it can limit the operating speed between the input and output, the response time is significantly improved compared with the operational amplifier.The output circuit form of the comparator is mainly divided into open collector (open drain) type and push-pull output type. The figure shows the internal equivalent circuit of BA10393, it is also an open collector output circuit. Ⅲ Difference between Amplifier and Comparator3.1 Total Difference Summary(1) The main difference between amplifier and comparator is the closed-loop characteristic. Most of the amplifiers work in a closed loop state, so it is required that they cannot be self-excited after the closed loop. Most of the comparators work in an open loop state and pursue speed. For the case of relatively low frequencies, the amplifier can completely replace the comparator (the output level should be considered), but in most cases, the comparator cannot be used as an amplifier.In order to increase the speed, the comparator optimization will reduce the range of closed-loop stability. While the op amp is optimized for the closed-loop stable range, so the speed is reduced. If an amplifier used as a comparator, as for performance, you may pay more than an amplifier price for its closed-loop stability.In other words, whether an op amp is used as a comparator or not is to see the negative feedback depth of the circuit. Therefore, a shallow closed-loop comparator may work in the amplifier state and will not have self-excited state. However, a lot of experiments must be done to ensure that the op amp is stable under all working conditions.(2) In general speaking, the comparator is an open-loop application of the op amp, but the comparator is designed for voltage threshold comparison. The required comparison threshold must be accurate, and the rise or fall time of output edge after comparison should be short. It conforms to TTL/CMOS level/or OC, etc., does not require the accuracy of the intermediate links, in addition, the driving capability is also different. In short, using op amps as comparators cannot achieve full-scale output in most cases, or the edge time after comparison is too long. So it is better to use special comparators in the design.Figure 6. Op Amp and Comparator Symbol3.2 Distinctions between Op-amp and ComparatorAlthough the electrical symbols of the comparator and the op amp are the same on the circuit diagram, the two devices have big differences and are generally not interchangeable. The differences are as following:1. The flipping speed of the comparator is fast, on the level of ns, while the flipping speed of the op amp is generally us level(except for special high-speed op amps).2. The op amp can be connected to the negative feedback circuit, but the comparator cannot use negative feedback. Although the comparator also has two input terminals of the inverting and non-inverting phase, when connecting negative feedback, the circuit cannot work stably without phase compensation circuit inside. But it is the main reason why the comparator is much faster than the op amp.3. The output stage of the operational amplifier generally adopts a push-pull circuit and a bipolar output. The output stage of most comparators is an open collector structure, so pull-up resistors and unipolar output are needed, which are easy to connect to digital circuits.4. Based on input, many operational amplifiers have built-in protection circuits to prevent large voltages from damaging the chip. When a large differential voltage is input, the input work will become abnormal, because the differential input voltage range of the op amp is usually limited. In addition, the common-mode input voltage range of non-rail-to-rail op amps cannot reach the positive power rail, but the comparator supports the positive power rail. Op amps and comparators have many similar parameters. It is more convenient to choose op amps instead of comparators in applications that require low offset voltage, low offset current, and high common mode rejection. Ⅳ Basic Use of Comparators and Op AmpsFigure 7. Operational Amplifier and ComparatorThe comparator is an open-loop circuit. Its function is to compare the voltage of the output terminal. When the voltage at the positive input terminal is large (IN2>IN1), the output is in high level (note: The comparator is an OC output, and the output terminal needs a pull-up resistor. A few volts will be pulled up to output a few volts, otherwise, the output will be an open circuit). When the negative input terminal voltage is large (IN1>IN2), the output will be in low level (GND). The voltage comparator input signal is an analog voltage, and the output signal generally only has two steady-state voltages of high level and low level. The voltage comparator can convert various periodic signals into rectangular waves.Operational amplifier can be used in linear amplifying circuit, and can also be used in non-linear circuit (used as comparator). It is widely used in electrical circuits, such as non-inverting amplification, inverse proportional amplification, difference, addition circuit, subtraction circuit, integral and differential circuit.  Ⅴ Op-amp Comparator5.1 TechniqueThe functions of the operational amplifier are more complicated, but the comparator is relatively simple. When the frequency requirement is not high, the operational amplifier can also be used as a low-performance comparator in practical applications.In theory, an operational amplifier with an open-loop configuration (no negative feedback) can function as a low-end comparator. When the voltage of the non-inverting input terminal (V+) is higher than the inverting input terminal (V-), due to the higher open-loop gain, a positive saturation voltage +U is output. When the voltage of the inverting input terminal (V-) is higher than the positive input terminal (V+), a reverse saturation voltage -U is output. For an op amp that works in a linear negative feedback configuration and is powered by a separate voltage (±V), is different from a non-linear comparator without negative feedback. 5.2 Op Amp Comparators DisadvantagesIn practice, the use of op amp comparators has the following disadvantages compared with the use of dedicated comparators:1) The op amp is designed to work in a linear segment with negative feedback, so saturated op amps generally have a slower flip speed. Most op amps have a compensation capacitor used to limit the slew rate of high-frequency signals. This makes the op amp comparator generally have a propagation delay on the level of microseconds, but a dedicated comparator is on the level of nanoseconds.2) The op amp does not have a built-in hysteresis circuit and requires a special external network to delay the input signal. 3) The static operating current of the op amp is stable only under negative feedback conditions. When the input voltage is not equal, there will be a DC offset.   4) The function of the comparator is to generate the input signal for the digital circuit. When using the op amp comparator, it is necessary to consider the compatibility with the digital circuit interface.5) Interference may occur between different frequencies of multiple op amps.6) Many op amps have diodes connected in reverse series at the input. The input of the two poles of the op amp is generally the same, which will not cause operational problems. But the two poles of the comparator need to be connected to different voltages, which may cause unexpected breakdown of the diode.7) Integrated circuits of dedicated comparator, which better combine the characteristics of analog and digital. It provides an output representing the logic state related to two analog voltages, one of which is a fixed reference quantity. When another voltage exceeds the reference value, is less than the reference value, or is in a specified range, the comparator can send a signal. It has an optimized combination of high gain, wide bandwidth and large flip rate to quickly change the output state. And the conversion time of digital signals is usually very fast. Ⅵ Using Op Amps as Comparators NotesThere are many points should remember when using op amps as comparators in circuits. You must consider five main op-amp characteristics to ensure expected performance:1) Power SupplyIf the logic and operational amplifier share the same power supply, the rail-to-rail operational amplifier can drive CMOS and TTL logic. but if they do not share the same power supply, an additional interface circuit is required.2) Input impedance and Bias CurrentWhen the operational amplifier is used as a comparator, it must meet the high input impedance condition. The input impedance of the CMOS voltage feedback operational amplifier is in the megohm level, which meets the requirement. As for current feedback (transconductance) operational amplifiers, the inverting input terminal has extremely low impedance, which cannot be used as a comparator.3) Differential Input CharacteristicsThe original intention of operational amplifier design is to cooperate with negative feedback to reduce the differential input as much as possible. In specific applications, the actual differential input voltage and the maximum differential input voltage that the op amp can actually provide should be considered.4) Common-mode Input CharacteristicsFor the old FET-type input operational amplifier, when the input exceeds the common-mode voltage range allowed by the device, a phase reversal will occur. At present, the op amps produced by various manufacturers use various methods to prevent the op amps from phase inversion. If the actual common-mode voltage range exceeds the allowable input common-mode voltage range of the op amp, you need to actually verify whether it is working properly.5) StabilityBecause there is no negative feedback externally, the open loop gain of the op amp used as a comparator is very high. Therefore, parasitic capacitance of the PCB and ground impedance of the non-inverting input terminal may cause the output to oscillate.Figure 8. Window Comparator CircuitⅦ ConclusionAlthough op amps are not designed to be used as comparators, nevertheless, many applications where the use of an op amp as a comparator is an economical engineering decision. It is important to make an reasonable decision to ensure that the op amp chosen performs as expected.That said, it is necessary to read the data sheets carefully and to consider the effects of op amp parameters on the application. Because the op amp is being used in a nonstandard manner, it may not reflect actual behavior, and some circuit experiment is advisable. Furthermore, because not all devices are typical in their behavior, some pessimism is warranted when interpreting the experimental results. Frequently Asked Questions about Operational Amplifier as Comparator1. Can an op amp be used as a comparator?However, op amps can also be used as comparators, which causes them to operate non-linearly. The inputs are driven hard and the output voltage slams to the power supply rail. 2. How does a comparator op amp work?A comparator circuit compares two voltages and outputs either a 1 (the voltage at the plus side; VDD in the illustration) or a 0 (the voltage at the negative side) to indicate which is larger. Comparators are often used, for example, to check whether an input has reached some predetermined value. 3. How op amp can be used as comparator in open loop configuration?Thus, an op-amp operating in open loop configuration will have an output that goes to positive saturation or negative saturation level or switch between positive and negative saturation levels and thus clips the output above these levels. This principle is used in a comparator circuit with two inputs and an output. 4. What is the difference between a comparator and an amplifier?Unlike operational amplifiers that usually operate with the input voltages at the same level, comparators typically see large differential voltage swings at their inputs. But some comparators without rail-to-rail inputs are specified to have a limited common mode input voltage range. 5. What is the difference between op amp and comparator?The difference between an op-amp comparator and a voltage comparator is in the output stage as a standard op-amp has an output stage that is optimized for linear operation, while the output stage of a voltage comparator is optimized for continuous saturated operation as it is always intended to be close to one supply.

Ⅰ IntroductionAs for operational amplifier applications, in electronic circuit, it is usually combined with a feedback network to form a certain functional module, with a special coupling circuit and feedback. Its output signal can be input signal addition, subtraction or differentiation, integration, etc, which early used in analog computers to do mathematical operations. Now they widely used in the electronics industry, regarded as precision AC and DC amplifiers, active filters, oscillators and voltage comparators.This Video is Introducing Operational Amplifier Applications in the CircuitCatalogⅠ Introduction1.1 Integrated Op AmpⅡ Op-amp ParametersⅢ Application MattersⅣ Classic Amplifier CircuitsⅤ One Question Related Op Amp and Going Further5.1 Question5.2 Answer1.1 Integrated Op Amp1.1.1 Evaluation AnalysisIntegrated operational amplifiers are one of the most widely used devices in analog integrated circuits. In various systems, because of different application requirements, the performance requirements of operational amplifiers are also different.Where there are no special requirements, try to use a universal integrated operational amplifier as much as possible, which can reduce costs and easily replace. When using multiple op amps in a system, use as many op amp integrated circuits as possible. For example, LM324 and LF347 always integrate four op amps together in a circuit.The evaluation of integrated op amps depends on their overall performance. Generally, the merit coefficient K is used to measure the excellent degree of integrated operational amplifiers, which is defined as: where SR is the slew rate and the unit is V / ms. The larger the value, the better the AC characteristics of the operational amplifier; The input bias current of the amplifier is lib, the unit is nA; VOS is the input offset voltage in mV. The smaller the Iib and VOS values, the better the DC characteristics of the op amp. Therefore, for circuits that amplify AC signals such as audio and video, op amps with large SR are better; for circuits that handle weak DC signals, op amps with high accuracy are more suitable (both offset current, offset voltage and temperature drift are relatively small).When selecting an integrated op amp, some factors should be considered in addition to the figure of merit coefficient K. For example, the signal source is a voltage source or a current source; the nature of the load, and whether the output voltage and current of the integrated op amp meet the requirements; operating voltage range, power consumption, and volume of the integrated op amp.Figure 1. Using Operational Amplifier as a Comparator1.1.2 Integrated Op Amp Basics Power supplyThe integrated op amp has two power terminals + VCC and -VEE, with different power supply methods. For different power supply modes, the requirements for input signals are different.1) Dual power supplyOp amps are mostly powered in this way. The positive power (+ E) and negative power (-E) relative to the common terminal (ground) are connected to the + VCC and -VEE pins of the op amp, respectively. In this way, the signal source can be directly connected to the input pin of the op amp, and the amplitude of the output voltage can make the positive and the negative symmetrical.2) Single power supplySingle-supply operation connects the -VEE pin of the op amp to ground. At this time, in order to ensure that the internal unit circuit of the operational amplifier has a suitable static operating point, a DC potential must be added to the input end of the op amp. Zero settingDue to the influence of the input offset voltage and input offset current of the integrated op amp, when the input signal is zero, the output is often not equal to zero. In order to improve the operation accuracy of the circuit, it is required to compensate the error caused by the offset voltage and the offset current. This is the zero setting of the operational amplifier. Commonly used zeroing methods include internal zeroing and external zeroing. For integrated op amps without internal zeroing terminals, external zeroing methods should be used. Self oscillationThe operational amplifier is a high-amplitude multi-stage amplifier. Under the condition of deep negative feedback, it is easy to cause self-excited oscillation. To make the amplifier work stably, a certain frequency compensation network must be added to eliminate the self oscillation. In addition, to prevent low-frequency oscillation or high-frequency oscillation caused by the internal resistance of the power supply, an electrolytic capacitor (10mF) and a high-frequency filter capacitor (0.01 mF ~ 0.1mF) should be connected. Device protectionThere are three aspects to the protection of the integrated op amp safety: power protection, input protection and output protection.1) Power protectionCommon faults of power supply are reverse polarity and voltage jump. For a power supply with poor performance, voltage overshoot often occurs at the moment when the power is turned on and off. Protection measures such as the use of FET current source and voltage regulator clamping protection. The voltage regulator’s voltage value is greater than the normal operating voltage of the integrated op amp and less than the maximum allowable operating voltage of the integrated op amp, and the current of the FET tube should be greater than the normal operating current of integrated op amp.2) Input protectionIf the input differential/common mode voltage of the integrated op amp is too high beyond the limit parameter range of the integrated op amp, it will be damaged.3) Output protectionWhen the integrated op amp is overloaded or the output is shorted, the op amp will be damaged if there is no protection circuit. However, some integrated op amps have internal current limit protection or short circuit protection, and no additional output protection is required to use these devices.Figure 2. An Inverting Op Amp CircuitⅡ Op-amp ParametersTo use the op amp better in the circuit, you must have a certain understanding of its internal parameters. Here are the technical parameters closely related to the op amp: Unity-gain bandwidth Definition: Under the condition that the closed-loop gain of the op amp is 1 time, a constant amplitude sinusoidal small signal is input to the input end of the op amp, and the closed-loop voltage gain measured from the output end of the op amp is reduced by 3dB (or equivalent to 0.707 times of the input signal of the op amp), that is to say, the frequency at which the output signal is reduced by -3dB is unity-gain bandwidth. It is a very important indicator. For a sinusoidal small signal amplification, the unity-gain bandwidth is equal to the product of the input signal frequency and the maximum gain at that frequency. In other words, when you know the frequency and gain of the signal to be processed, the unity-gain bandwidth (gain bandwidth = amplification * signal frequency) can be calculated to select the appropriate op amp. The higher the bandwidth, the higher the frequency of the signal that can be processed, and the better the high frequency characteristics, otherwise the signal will be easily distorted.    For small signals, the unity-gain bandwidth is also called the gain-bandwidth product, which can roughly show the ability of the op amp to process the frequency of the signal. For example, the gain bandwidth of a certain operational amplifier is 1MHz, if the actual closed-loop gain is 100, then the maximum frequency for theoretical processing of small signals is 1MHz / 100 = 10KHz.For the bandwidth of a large signal, that is, the power bandwidth, the influence of the slew rate SR is the major factor, and the unit is V/uS. In this case, the power bandwidth calculated by FPBW = SR / 2πVp-p, that is, the gain bandwidth and power bandwidth must be satisfied at the same time when designing the circuit.For DC signals, bandwidth issues are generally not considered, and accuracy and interference are mainly considered.When the amplification factor of an amplifier is n times, it does not mean that all input signals are amplified n times. When the signal frequency increases, the amplification capability decreases. Open bandwidthThe open-loop bandwidth is defined as: inputting a constant-amplitude sinusoidal small signal to the input of the op amp, the frequency measured at which the open-loop voltage gain decrease 3dB from the output of the op amp to the dc gain of the op amp. This is used for very small signal processing. Slew rate SRWith the op amp connected in a closed loop, a large signal (including a step signal) is input to the input of the op amp, and the output rise rate of the op amp is measured from the output of the op amp called SR. Because the input stage of the op amp is switched during the conversion, the feedback loop of the op amp does not work, that is, the conversion rate is independent of the closed-loop gain. The slew rate is a very important index for large signal processing. For general op amps, the slew rate SR <= 10V / μs, and the slew rate of high speed op amps is SR> 10V / μs. The highest conversion rate SR of current high-speed op amps reaches 6000V / μs. The larger the SR, the better the response of the op amp to the input signal changing at high speed. The larger the signal amplitude, the higher the frequency, and the greater the SR. This is used for op amp selection in large signal processing. Full-power bandwidthAt the rated load, under the condition that the closed-loop gain of the op amp is 1 time, a constant-amplitude sinusoidal large signal is input to the input end of the op amp, so that the output frequency of the op amp reaches the maximum (allowing certain distortion) signal. This frequency is limited by the slew rate SR of the op amp. Approximately, full power bandwidth is calculated by formula SR / 2πVop (Vop is the peak output amplitude of the op amp). It is a very important indicator for op amp selection in large signal processing. Setting timeAt the rated load, under the condition that the closed-loop gain of the op amp is 1 time, the time required to input a step large signal to the input of the op amp to increase the output from 0 to a given value. Because it is a step large signal input, a certain jitter will occur after the output signal reaches a given value. This jitter time is called the stabilization time. At this moment, stabilization time + rise time = settling time. For different output accuracy, there is a big difference in the stabilization time. The higher the accuracy, the longer the stabilization time. Equivalent input noise voltageIt refers to any AC random interference voltage generated at the output of an op amp with good shielding and no signal input. When this noise voltage is converted to the input of the op amp, it is called the input noise voltage of the op amp (sometimes expressed by noise current). For broadband noise, the effective value of the input noise voltage of ordinary op amps is about 10 ~ 20μV. This value often corresponds to a certain frequency band. Output impedanceIt refers to the ratio of the change in voltage to the corresponding change in current when the signal voltage is applied to the output of the op amp working in the linear region. At low frequencies it only refers to the output resistance of the op amp. Common mode input resistenceRefers to the ratio of the change in the input voltage of the common mode to the corresponding change in the input current when the two inputs of the op amp input the same signal. At low frequencies, it behaves as a common mode resistance. Generally, the common mode input impedance of the op amp is much higher than the differential mode input impedance, with a typical value above 108Ω. Common mode rejection ratioSame as the definition in the differential amplifier circuit, it is the ratio of the differential mode voltage gain to the common mode voltage gain, which is usually expressed in decibels. It is a parameter that measures the degree of symmetry of the input stage differential amplifier and the ability of the integrated op amp to suppress common mode interference signals. The larger the value, the better. Power supply rejection ratioThe power supply voltage rejection ratio is defined as the change ratio of the input offset voltage of the op amp with the power supply voltage in the linear region. The power supply voltage rejection ratio reflects the effect of power supply changes on the output of the op amp. At present, the power supply voltage suppression ratio is only about 80dB. Therefore, when used for DC signal or small signal processing for analog amplification, the power supply of the op amp needs to be carefully set. Of course, an op amp with a high common mode rejection ratio can compensate a part of the power supply voltage rejection ratio. In addition, when using dual power supplies, the power supply voltage rejection ratio of the positive and negative power supplies may be different. Differential mode input resistanceRefers to the ratio of the change in voltage at the two input terminals to the corresponding change in current at the input terminals when the op amp is operating in the linear region. The differential mode input impedance includes the input resistance and input capacitance, and refers only to the input resistance at low frequencies. General products specification only give input resistance. The input resistance of the op amp using the bipolar transistor as the input stage is not greater than 10MΩ; the input resistance of the op amp as the input stage of the field effect transistor is generally greater than 109Ω. Input offset voltageWhen the input voltage is zero, the output voltage is divided by the voltage gain, plus the negative sign, which is the offset voltage converted to the input. It is the compensation voltage applied at the input when the output voltage is zero. The input offset voltage actually reflects the circuit symmetry inside the op amp. The better the symmetry, the smaller the input offset voltage. The input offset voltage is a very important indicator of the op amp, especially when it is a precision op amp or used for DC amplification.The input offset voltage has a certain relationship with the manufacturing process. It is between ± 1 and 10 mV when op amps use the bipolar process (that is, the standard silicon process). If the field effect tube is used as the input stage, it will be greater. For precision op amps, it is generally below 1mV. The smaller the input offset voltage, the smaller the intermediate zero offset during DC amplification, and the easier it is to handle. Therefore, it is an extremely important index for precision op amps. Input offset voltage driftWithin the specified operating temperature range, it is the ratio of the change in input offset voltage with temperature to the change in temperature. It is actually a supplement to the input offset voltage, which is convenient for calculating the drift of the amplifier circuit due to temperature changes within a given operating range. It is an important indicator for measuring the temperature effect to the op amp. Under normal circumstances, it is about (10 ~ 30) uV / C (degree Celsius), the high quality can be <0.5uV / C. Input offset currentIt is defined as the difference between the base current of the differential pair of the differential input stage when the output DC voltage of the op amp is zero. Used to characterize the degree of asymmetry of the differential input current. The better the symmetry, the smaller the input offset current. Input offset current is a very important indicator for op amps, especially for precision operational amplifier or DC amplifier. The input offset current is approximately one to one-tenth of the input bias current. It has an important impact on small signal precision amplification or DC amplification, especially when a large resistor is used outside the op amp. The effect of input offset current may exceed the effect of input offset voltage on accuracy. The smaller the input offset current, the smaller the intermediate zero offset during DC amplification, and the easier it is to handle. Therefore, it is an extremely important index for precision op amps. Input offset current temperature driftWithin the specified operating temperature range, the ratio of the amount of change in input offset current with temperature to the amount of temperature change. It refers to the temperature coefficient of within the specified operating range, and is also an important indicator to measure the temperature effect on the op amp. It is usually about (1-50) nA / C, and the high quality is about several pA / C. This value is only given in the precision op amp parameters, and it needs attention when it is used for DC signal processing or small signal processing. Input bias current   It is defined as the average value of the bias currents of the two input terminals when the output DC voltage of the op amp is zero, in other words, it is the average current flowing into the input terminal when the operational amplifier is operating in the linear region. The input bias current has a greater impact on the places where input impedance is required, such as high-impedance signal amplification and integrator circuits. The input bias current has a certain relationship with the manufacturing process. If a field effect tube is used as the input stage, the input bias current generally lower than 1nA. It always used to measure the input current of the differential amplifier pair. Maximum differential mode input voltageIt is a voltage that the two input ends of the op amp can withstand. When it is exceeded, the reverse breakdown of the differential tube will occur. The NPN tube made by the plane process has a value of about 5V, and the Vidmax of the horizontal PNP tube can reach more than 30V. Maximum common mode input voltageIt an allowable range of common mode input voltage under normal operating conditions of the op amp. When the input differential pair saturates, the amplifier loses common mode rejection ability. In the case of interference, it is necessary to pay attention to this problem in the use of the circuit. Output peak to peak voltageWorking in the linear region, under the specified load, when the op amp is powered by the large power supply, it is the maximum voltage amplitude that the op amp can output. Except for low voltage op amps, the output peak-to-peak voltage of general op amps is greater than ± 10V, but less than the power supply voltage. This is due to the design of the output stage. The output stage of modern low-voltage op amps has been specially treated. The output peak-to-peak voltage is close to within 50mV of the power supply voltage, so it is called a full-scale output op amp, also known as a rail-to-raid op amp. It should be noted that the output peak-to-peak voltage of the op amp is related to the load, and the value is different for different loads; the positive and negative output voltage swings of the op amp are not necessarily the same. For practical applications, the closer the output peak-to-peak voltage is to the supply voltage, the easier the power supply design.Figure 3. Input Offset Voltage of an Op-ampⅢ Application Matters1) A single-supply op amp must be DC biased, otherwise it will not work properly. For the virtual ground design, in addition to the DC potential, it is necessary to pay attention to the voltage stabilization (it is best to use the reference voltage chip), and also to ensure low impedance AC decoupling, that is, low-frequency decoupling parallel to at least 10uF and high frequency decoupling under 0.1uF.2) The input of the non-inverting amplifier must be biased to ground as a DC path.3) Ordinary op amps cannot directly drive capacitive loads. If there is need, you must use capacitors for phase compensation or output series resistors and then connect the load.4) For the op amp input of the external interface, a TVS tube must be connected in parallel to the positive and negative input pins to prevent the op amp from reversing the polarity due to the too large input voltage signal, forming a parasitic false signal output.5) For amplifier circuits with a gain of more than 10 times, pay attention to controlling the bandwidth gain of the op amp to prevent the device from self oscillation.6) The output of the power amplifier needs to be protected by switching diodes to the power supply and ground, especially when inductive loads are connected.7) When using multiple op amps to process multiple signals, care must be taken to prevent the instantaneous changes in one of the signals from causing crosstalk to the other signal. Therefore, it is recommended not to use one op amp to process multiple signals.8) Most op amp chips are ESD sensitive devices, so pay more attention when using them.9) The pins of unused op amps (excess channels in multiple op amps) should not be left floating, and  grounded or connected to positive and negative power supplies. It is recommended to connect it as a follower (the output is connected to the reverse input) and the non-inverting input is connected to a potential between the power rails (the ground of the dual power system or any suitable point in the circuit). They can also used as buffer amplifiers and add them to a small impact location in the system.Figure 4. Op Amp 741Ⅳ Classic Amplifier CircuitsFigure 5. Inverting AmplifierFigure 5: The grounded non-inverting terminal of op amp is 0V. The inverting and non-inverting terminals are short-circuit, so the inverting end is also 0V. The input resistance of the inverting input terminal is very high, and it is virtual open. In other words, there is almost no current pass through. Therefore, the current flowing through each component in a series circuit is the same, that is, the current flowing through R1 and R2 are the same.Current flowing through R1: I1 = (Vi-V-)/R1Current flowing through R2: I2 = (V--Vout)/R2V- = V+ = 0, I1 = I2Solve the above algebraic equation to get Vout = (-R2/R1)*Vi, it is the input-output relationship of the inverting amplifier. Figure 6. Non-inverting AmplifierIn Figure 6, Vi and V- are virtual short, where Vi = V-. Because of the virtual open, there is no current flow through at the reverse input terminal, then R1=R2. If the current is I, which is obtained by Ohm's law: I = Vout/(R1+R2);Vi is equal to the partial voltage on R2, that is: Vi = I*R2.Virtual short: Vi = V-, R1=R2Ohm's law: I = Vout/(R1+R2), Vi = I*R2Where Vout=Vi*(R1+R2)/R2, represents the non-inverting amplifier. Figure 7. AdderFigure 7: Knowing from the Kirchhoff's law and virtual open theory, the sum of the current through R2 and R1 is equal to the R3, V- = V+ = 0 (short circuit), so (V1 – V-)/R1 + (V2 – V-)/R2 = (Vout – V-) /R3 can be transferred as V1/R1 + V2/R2= Vout/R3. If R1=R2=R3, then the formula becomes Vout=V1+V2, which is an adder. Figure 8. AdderIn Figure 8, because of the virtual open, no current flows through the non-inverting terminal, where V+ = V-, R1=R2, R4=R3, therefore, (V1 – V+)/R1 = (V+-V2)/R2, (Vout – V-)/R3 = V-/R4 can be simplified as V+ = (V1 + V2)/2 V- = Vout/2. So Vout = V1 + V2 is also an adder. Figure 9. SubtractorFigure 9 shows that the current through R1 is equal to the R2, and R4=R3, therefore, (V2– V+)/R1 = V+/R2, (V1 – V-)/R4 = (V--Vout)/R3. If R1=R2, then V+ = V2/2; if R3=R4, then V- = (Vout + V1)/2, because of V+ = V-, so Vout =V2-V1 is a subtractor. Figure 10. Integrator CircuitIn Figure 10, the input voltage at the inverting terminal is equal to the non-inverting terminal because of short circuit; the current through R1 is equal to the C1 because of virtual open. The current flowing through R1 and C1 are Ri=V1/R1, Ci=C*dUc/dt=-C*dVout/dt, respectively. So Vout=((-1/(R1*C1))∫V1dt, which is a integrator circuit. If V1 is a constant voltage U, then the above formula is transformed to Vout = -U*t/(R1*C1)t, then the Vout is a straight line that changes with time. Figure 11. Differential CircuitIn Figure 11, the current through capacitor C1 and resistor R2 is equal because of virtual open; V+ = V- because of short circuit, where Vout = -i * R2 = -(R2*C1)dV1/dt, which is a differential circuit. If V1 is a DC voltage, the output Vout corresponds to a pulse in the opposite direction to V1. Figure 12. Differential Amplifier CircuitFigure 12:Vx = V1……a, Vy = V2……bthen R1, R2, R3 can be regarded as a series, R1=R2=R3, the current I=(Vx-Vy)/R2……cwhere Vo1-Vo2=I*(R1+R2+R3) = (Vx-Vy)(R1+R2+R3)/R2 ……dIf R6=R7, then Vw = Vo2/2 ......e, similarly, if R4=R5, then Vout – Vu = Vu – Vo1, so Vu = (Vout+Vo1)/2 ……fdue to short circuit, Vu = Vw ……g, based on efg formulas, Vout = Vo2 – Vo1 ……hGet from dh, Vout = (Vy – Vx) (R1+R2+R3)/R2, where (R1+R2+R3)/R2 is a fixed value. This value determines the amplifier multiple of the difference (Vy-Vx), thus it is a differential amplifier circuit. Figure 13. Amplifier CircuitIt is a relatively common amplifier circuit. Many controllers accept 0~20mA or 4~20mA current from various measuring instruments. The circuit converts the current into voltage signal to become a digital signal by ADC. Figure 13 is such a typical circuit. As shown in Figure, 4~20mA current flows through the sampling 100Ω resistor R1, there will be a voltage difference of 0.4~2V on R1. Due to virtual open circuit, R3= R5 and R2=R4.Therefore: (V2-Vy)/R3 = Vy/R5 ……a  (V1-Vx)/R2= (Vx-Vout)/R4 ……bShort circuit: Vx = Vy ……cCurrent changes from 0~20mA, then V1 = V2 + (0.4~2) ……dPut cd formulas into b formula: (V2 +(0.4~2)-Vy)/R2 = (Vy-Vout)/R4 ……eIf R3=R2 , R4=R5, then e-a gets Vout =-(0.4~2)R4/R2 ……fIn Figure 13, R4/R2=22k/10k=2.2, then f formula Vout = -(0.88~4.4)V, that is to say, the current of 4~20mA is converted into a voltage range of -0.88~-4.4V. Current can be converted into voltage, and voltage can also be converted into current. Figure 14 is such a circuit. The negative feedback in the above figure does not directly feedback through the resistor, but the emitter junction of the transistor Q1 is connected in series. But it isn't a comparator. As long as it is an amplifying circuit, the law of short circuit and virtual open still conforms.Figure 14. Amplifier CircuitDue to virtual open, no current flows through the input of the op amp,Then (Vi – V1)/R2 = (V1 – V4)/R6 ……aSimilarly (V3 – V2)/R5 = V2/R4 ……bsince short circuit, V1 = V2 ……cIf R2=R6, R4=R5, then V3-V4=Vi can be obtained from abc.The above formula shows that the voltage across R7 is equal to the input voltage Vi, then the current through R7 is I=Vi/R7. If the load RL<100KΩ, the current through R1 and R7 are basically the same. Ⅴ One Question Related to Op Amp and Going Further5.1 QuestionWhat the Application of an Op Amp as a Phase Shifter?5.2 AnswerIn electronic circuit, op amp is used for direct coupling procedure and so DC voltage level at the emitter terminal increases from phase to phase. This rapidly increasing DC level is likely to shift the operating point of the upcoming stages. Thus to move down the increasing voltage swing, this phase shifter is applied.The phase shifter performs by adding a DC voltage level to the output of fall stage to pass the output to a ground level. Frequently Asked Questions about Operational Amplifier Applications1. Why is it called operational amplifier?It's called an “operational” amplifier because it performs a mathematical operation. The most obvious one is multiplication - it amplifies an input signal by a constant. ... But many different 'operations' can be performed by different circuit topologies. 2. What is inside an operational amplifier?Operations amplifiers — op-amps for short, are integrated circuits, constructed mostly out of transistors and resistors. These integrated circuits multiply an input signal to a larger output. You can use these components with voltage and current in both DC and AC circuits. 3. What are operational amplifiers used for?Op amps are used in a wide variety of applications in electronics. Some of the more common applications are: as a voltage follower, selective inversion circuit, a current-to-voltage converter, active rectifier, integrator, a whole wide variety of filters, and a voltage comparator. 4. What are linear applications of op amp?A linear amplifier like an op amp has many different applications. It has a high open loop gain, high input impedance and low output impedance. It has high common mode rejection ratio. Due to these favourable characteristics, it is used for different application. 5. How does an operational amplifier work?An operational amplifier, or op amp, generally comprises a differential-input stage with high input impedance, an intermediate-gain stage, and a push-pull output stage with a low output impedance (no greater than 100 Ω). ... That is, the output gets fed back to the inverting input through some impedance. 6. What do you mean by differential amplifier?A differential amplifier is a type of electronic amplifier that amplifies the difference between two input voltages but suppresses any voltage common to the two inputs. It is an analog circuit with two inputs and and one output in which the output is ideally proportional to the difference between the two voltages. 7. What are the non linear applications of op amp?Non-Linear Applications of Op AmpVoltage comparator.Two applications of comparator as window detector and zero crossing detector.Schmitt trigger circuit with the extension of regenerative comparator.Multivibrator circuits.Precision rectifier or super diode with the combination of op amp as voltage follower and a diode. 8. Why do we use differential amplifier?Differential amplifiers are used mainly to suppress noise. ... Noise is generated in the wires and cables, due to electromagnetic induction, etc., and it causes a difference in potential (i.e., noise) between the signal source ground and the circuit ground. 9. What does an operational amplifier do?An operational amplifier is an integrated circuit that can amplify weak electric signals. An operational amplifier has two input pins and one output pin. Its basic role is to amplify and output the voltage difference between the two input pins. 10. What is an ideal operational amplifier?Operational amplifier: The ideal op amp is an amplifier with infinite input impedance, infinite open-loop gain, zero output impedance, infinite bandwidth, and zero noise. It has positive and negative inputs which allow circuits that use feedback to achieve a wide range of functions.