Non Inverting Amplifier: Circuit, Gain Formula, Engineering Design & Applications

December 21 2023
Ersa

Clear diagram, step-by-step gain derivation, design limits (GBW, CMR, output swing), buffer/ADC use, and a practical inverting vs non-inverting comparison with FAQs.

What Is a Non-Inverting Amplifier?

A non-inverting amplifier is a type of operational amplifier (op-amp) configuration where the input signal is applied to the non-inverting input (+) terminal of the op-amp. The output voltage is in phase with the input, meaning there is no phase inversion, unlike an inverting amplifier.

Working Principle

The basic operation of a non-inverting amplifier is as follows: the input signal is applied to the non-inverting input terminal (+), while the inverting input terminal (–) is connected to the feedback network. The op-amp amplifies the signal and produces an output that is in phase with the input. The gain of the amplifier is determined by the feedback resistor (Rf) and the input resistor (Rin), with the formula:

Gain (Av) is always ≥ 1, making the non-inverting amplifier ideal for voltage buffering and low-power applications.

Typical Applications

  • Buffer (Voltage Follower): Used for isolating different stages of a circuit without affecting signal integrity. The output follows the input voltage.
  • ADC Pre-Amplification: Used in applications where a weak signal from a sensor needs to be amplified before being fed into an analog-to-digital converter (ADC).

Non-Inverting Amplifier Circuit Diagram

Non-inverting amplifier basic diagram
Non-inverting amplifier basic circuit diagram showing the operational amplifier, feedback resistor (Rf), and input resistor (Rin).

The circuit diagram above shows the basic configuration of a non-inverting amplifier, where the input signal is applied to the non-inverting input and the output is fed back through the feedback resistor.

Non Inverting Amplifier Circuit & Working Principle

The non inverting amplifier circuit (an op amp non inverting amplifier) applies the input signal to the op-amp’s non-inverting (+) input while the inverting (−) input is tied to a feedback divider. The non inverting amplifier circuit diagram below labels all working nodes and components used in practice.

non-inverting-amplifier-circuit-diagram-with-bias-compensation
Non-inverting amplifier with labeled nodes: Vin, Vout, Rin, Rf, and bias-compensation Rb from the (+) input to reference (GND or Vref).

Working Principle — Virtual Short & Virtual Open

With negative feedback, the op-amp forces the inverting node to follow the non-inverting node: virtual shortV− ≈ V+. Because the input bias currents are extremely small, the op-amp inputs draw ~0 current: virtual open. In this configuration, V+ is driven by Vin, so the feedback makes the divider at the inverting node satisfy:

V− = Vout · (Rin / (Rin + Rf)) ≈ V+ = Vin

When Vin rises, V+ rises. The op-amp output increases through Rf until the divider raises V− to match V+. This feedback action keeps output in phase with the input (0° phase shift). The full gain derivation appears in the next section.

How Feedback Builds Same-Phase Gain (Step-by-Step)

  1. Input change: Vin nudges V+.
  2. Error appears: ε = V+ − V−.
  3. Op-amp amplifies the error ⇒ Vout moves to reduce ε.
  4. Through Rf, the inverting node rises/falls until V− ≈ V+.
  5. Result: Vout follows the polarity of Vin (same phase).

Bias-Current Compensation (Engineering Tip)

Input bias currents flowing through unequal source resistances create an offset at the inputs. To cancel this, add a resistor from the non-inverting (+) input to the reference node (GND or Vref):

Choose: Rb = Rin ∥ Rf

  • Placement: between the (+) input and the same reference used for the divider (ground or Vref).
  • Typical range: 1–20 kΩ (balance noise, bandwidth, and bias-induced offset).
  • If the signal source has resistance Rs, use Rb ≈ (Rs ∥ Rin ∥ Rf).

Practical Notes

  • Single-supply designs must keep Vin within the op-amp’s common-mode range; avoid hugging ground or VCC unless the device is rail-to-rail.
  • Output swing may not reach the rails; check the datasheet to prevent early saturation.
  • Power pins and supply decoupling (e.g., 0.1 µF close to VCC) are omitted from the simplified diagram but required on the PCB.

Non Inverting Amplifier Gain Formula & Derivation

This section derives the non inverting amplifier gain formula from first principles, then applies it to a step-by-step calculation. Keep these results handy—this is the core formula for non inverting amplifier design and the definitive non inverting amplifier equation used in practice.

Gain Formula — Step-by-Step Derivation

  1. From the divider at the inverting node (with negative feedback active): V- = Vout · Rin / (Rin + Rf).
  2. Virtual short in closed loop (ideal op amp): V+ ≈ V- and the non-inverting node is driven by the input: V+ = Vin.
  3. Equate the two: Vin = Vout · Rin / (Rin + Rf).
  4. Rearrange to obtain the gain of a non inverting amplifier:
    Vout / Vin = (Rin + Rf) / Rin = 1 + Rf / Rin

Therefore, the closed-loop voltage gain is Av = 1 + Rf/Rin, which is always ≥ 1 (unity gain if Rf=0).

Worked Example — Plug Numbers In

Given: Vin = 0.2 V, Rin = 10 kΩ, Rf = 40 kΩ.

  1. Compute gain: Av = 1 + Rf/Rin = 1 + 40k/10k = 1 + 4 = 5.
  2. Output: Vout = Av · Vin = 5 × 0.2 V = 1.0 V.

Tip: keep units consistent (Ω, kΩ). Mixing units is a common mistake.

Reverse Design — Target Gain to Resistor Ratio

Target: Av = 11

  1. From Av = 1 + Rf/Rin, solve for the ratio: Rf/Rin = 10.
  2. Pick an easily sourced value, e.g., Rin = 10 kΩRf = 100 kΩ (E24/E96 series).

Note: resistor tolerance (e.g., 1%) directly maps to gain tolerance; choose precision parts if needed.

non-inverting-amplifier-gain-formula-example-calculation
Step-by-step calculation card for the non-inverting amplifier gain formula and a worked example.

Practical Design Limits (What Datasheets Don’t Shout)

Beyond the ideal model, a non-inverting op-amp has real-world limits that cap gain, speed, and accuracy. This section turns those into engineer-ready rules covering non inverting amplifier impedance, bandwidth, stability, output swing, and practical phase difference near the closed-loop bandwidth.

non-inverting-amplifier-design-limits-gbw-slew-stability
At-a-glance limits: CMVR, output swing, GBW, slew rate, capacitive-load stability, and noise vs. resistor values.

Input Common-Mode Range (CMVR)

  • The non-inverting (+) input must stay within the device’s CMVR. On single-supply, avoid hugging GND or VCC unless the op-amp is rail-to-rail input.
  • If you must sense near ground/VCC, use rail-to-rail input devices or bias the input around a mid-supply reference Vref.
  • Beware: CMVR often shrinks over temperature and with heavy output loading; check “min” not just “typ”.

Output Swing to the Rails

  • Non-rail-to-rail outputs clip early, especially at higher load currents. Leave 100–300 mV headroom to each rail (device-dependent).
  • Check datasheet curves “VOH, VOL vs Iout” and ensure your expected Vout stays out of the saturation region.
  • Single-supply with mid-bias: output swings around Vref; top/bottom swing limits may be asymmetric.

Closed-Loop Bandwidth (GBW Rule)

Small-signal approximation: fCL,max ≈ GBW / Av. Example: GBW = 10 MHz, Av = 5≈ 2 MHz (use a 0.5 safety factor for flatness).

As you approach fCL, the loop adds phase lag; practical phase difference from input to output grows even though polarity remains non-inverting.

Slew Rate (Large-Signal Limit)

For an undistorted sine, SR ≥ 2π f · Vpkfmax,SR ≈ SR / (2π Vpk).

Example: SR = 0.5 V/µs, Vpk=1.0 Vfmax,SR ≈ 0.5×106 / (2π·1) ≈ 79.6 kHz. Large-signal limit often bites before GBW at higher amplitudes.

Stability with Capacitive Loads

  • Symptoms: ringing/overshoot or outright oscillation (phase margin too low) — a stability problem.
  • Quick fixes:
    • Series isolator at output: 10–100 Ω to decouple cable/ADC sampling caps.
    • Feedback cap across Rf: add Cf so fp ≈ 1/(2π Rf Cf) (place well above signal band).
    • Keep feedback network impedance moderate (1–20 kΩ) to help noise and phase margin.

Impedance, Noise & Resistor Selection

  • non inverting amplifier impedance: ideally very high at the input, but adding the bias-comp resistor Rb=Rin∥Rf makes the seen impedance roughly that value.
  • Thermal noise: resistor noise scales with value, en ≈ √(4kTRB) (Vrms). Excessively large R raises noise and bias-current-induced offsets.
  • Recommended range: choose 1–20 kΩ class for Rin, Rf to balance noise, bandwidth, and stability.

Phase Difference in Real Life

Ideal non-inverting gain has 0° phase shift. In practice, operate well below the closed-loop bandwidth (e.g., ≤ 0.1–0.2 × fCL) to keep phase error small and frequency response flat.

Design Check Matrix

Limit Symptom Quick Rule / Equation Check In Datasheet Action
CMVR Input pins near rails misbehave Keep V+ within CMVR Common-mode input range (min) Use RRI device or bias at Vref
Output swing Clipping near rails Reserve 100–300 mV headroom VOH/VOL vs Iout curves Reduce load / pick RRO device
Bandwidth Amplitude droop at high f fCL ≈ GBW / Av GBW, open-loop gain plot Lower gain or use higher-GBW op-amp
Slew rate Triangular tops, distortion fmax ≈ SR / (2π Vpk) SR (typ/min) Reduce Vpk/f or pick higher-SR device
Stability (C-load) Ringing/oscillation Series 10–100 Ω; add Cf Phase margin guidance Isolate load; tune Rf, Cf
Noise/Offsets High noise, DC offset drift en ≈ √(4kTRB); match seen resistances Input bias & noise specs Keep R in 1–20 kΩ; add Rb=Rin∥Rf

Takeaways

  • Check CMVR and output swing before celebrating the gain number.
  • For speed: small-signal limit f ≈ GBW/Av; large-signal limit f ≈ SR/(2πVpk).
  • Stability first with capacitive loads: series 10–100 Ω and/or feedback Cf.
  • Keep feedback resistors in the 1–20 kΩ range; add and match Rb to tame offsets.
  • Operate well below fCL for minimal phase difference and flat response.

Applications (Engineer-Ready)

This section turns theory into practice with three non inverting amplifier applications you can deploy immediately. Each module includes a quick recipe and a checklist, plus a concrete non inverting amplifier example when relevant.

non-inverting-amplifier-buffer-adc-driver-use-cases
Three engineer-ready use cases: voltage follower (buffer), sensor → ADC driver, and audio/instrumentation preamp.

Voltage Follower (Unity Gain Non Inverting Amplifier Buffer)

Use a unity-gain, non inverting amplifier buffer to isolate high source impedance from heavy/variable loads, or ahead of long cables and multiplexers.

Quick Recipe
  • Topology: tie output directly to (−) input (Rf=0, Rin=∞), input to (+).
  • Bias path for AC-coupled sources: add a high-value resistor from (+) to reference (Vref or GND), e.g. 100 kΩ–1 MΩ.
  • Capacitive loads: series output isolator Riso=10–50 Ω.
  • Op-amp must be unity-gain stable; aim for GBW ≥ 10× signal bandwidth.
Checklist
  • CMVR covers the entire input range (single-supply: avoid hugging rails unless RRI).
  • Output swing meets headroom at expected load current.
  • AC-coupled input has a defined DC bias path (no float).

Sensor → ADC Front-End (Non Inverting Gain)

Amplify low-level sensor signals to span the ADC full-scale while ensuring anti-alias filtering and stable drive of the sample/hold network.

  1. Set gain: Av = VFS,ADC(span) / Vsensor(span). Example: ADC 0–3.3 V, sensor 0.05–0.30 V ⇒ span 0.25 V ⇒ Av≈13.2 (choose 12–14 for margin).
  2. Choose resistors: keep Rin, Rf in 1–20 kΩ to balance noise and bandwidth.
  3. Anti-alias RC: one-pole LPF with fc ≈ fs/5 … fs/10 using fc=1/(2πRC).
  4. Drive SAR S/H: add output series Riso=10–100 Ω and a shunt cap at the ADC pin (e.g., 100–330 pF), ensuring tacq ≥ 5·Rsource,eff·CSH,eq.
  5. Single-supply bias if needed: Vout = Vref + Av(Vin − Vref).
Quick Recipe
  • Rin=10 kΩ, Rf=(Av−1)·Rin (use E24/E96).
  • Anti-alias: R=1–5 kΩ, choose C for target fc vs. fs.
  • ADC drive: Riso=22–68 Ω, Chold=100–330 pF (verify with ADC datasheet).
Checklist
  • GBW ≥ 10×Av×signal bandwidth; SR ≥ 2π f Vpk.
  • CMVR/output swing OK at temperature and load extremes.
  • Rsource,eff meets ADC acquisition timing; transition waveform shows no droop/overshoot.

Audio / Instrumentation Preamplifier

A low-noise, high-input-impedance non inverting amplifier is ideal as an audio or instrumentation front end.

  • Device choice: low noise density (audio target < 5 nV/√Hz), adequate GBW and SR.
  • Input & high-pass: AC-couple the source if needed; bias (+) at Vref with a divider and bypass. Set fHP=1/(2π R C) (audio: 2–10 Hz typical).
  • EMI/stability: series 100–470 Ω at input for RF damping; 10–47 Ω at output for capacitive-load isolation.
Quick Recipe
  • Set gain: Av = 1 + Rf/Rin; keep R values in 1–20 kΩ.
  • Input coupling: Cin=1–10 µF with effective R to target fHP.
  • Decoupling: 0.1 µF near each supply pin + 1–10 µF bulk close to the device.
Checklist
  • Noise/THD targets met; LF roll-off as designed.
  • Flat magnitude/phase within the audio/instrumentation band (operate ≤ 0.1–0.2× fCL).
  • Output swing and load drive meet the next stage requirements.

Comparison: Inverting vs Non-Inverting Amplifier

This table distills the essential difference between inverting and non inverting amplifier configurations. If you’re weighing inverting vs non inverting amplifier for your design, scan the rows below. They summarize how inverting and non inverting amplifier topologies differ in connection, phase, gain, impedance, bandwidth, and use cases.

Field Inverting Non-Inverting
Input node Signal into (−) via Rin; (+) at reference (GND/Vref). Signal into (+); (−) to divider Rin–Rf.
Phase relation 180° inverted vs input. 0° (same phase) as input.
Gain equation Av= −Rf/Rin Av= 1 + Rf/Rin (≥1)
Input impedance Rin (designer-set, often lower). Very high (limited by op-amp; with Rb roughly that value).
Summing capability Native summing (multiple inputs via virtual ground). Not convenient for accurate summing.
Typical uses Signed gain, summing/mixing, active filters, TIA. Buffer/voltage follower, high-Z sensors, ADC driver, audio/instrumentation preamp.
Closed-loop bandwidth GBW / (|Av| + 1) (noise gain). GBW / Av (noise gain = Av).
Voltage follower? No (−1 possible but input Z = Rin). Yes (requires unity-gain stable op-amp).
One-line guide: choose non-inverting when your source impedance is high, you need a true voltage follower/buffer, or you must drive an ADC input. Pick inverting for accurate summing/mixing or when you need a precise polarity inversion.
inverting-vs-non-inverting-amplifier-comparison-table
Side-by-side comparison of inverting and non-inverting amplifier configurations.

Real IC Examples for a Non-Inverting Op-Amp Front End

Here are some op amp non inverting amplifier ICs that are commonly used in different applications. For each example, we’ve included key specifications, typical use cases, and direct links to our catalog for easy selection.

non-inverting-op-amp-ic-examples-catalog-links
Examples of real ICs for non-inverting amplifiers across different use cases: general-purpose, rail-to-rail, and audio.

General-Purpose (Teaching / Lab / Legacy Systems)

LM741 and TL081 are ideal for basic educational and lab use, offering low cost and good general performance for small to moderate signals. These op-amps are not rail-to-rail and are typically powered by dual supplies, ±12V or ±15V.

Op-Amp Supply Voltage Rail-to-Rail GBW Typical Use Catalog Link
LM741 ±12V to ±15V No 1 MHz General-purpose, teaching, legacy systems View in Catalog
TL081 ±12V to ±15V No 3 MHz General-purpose, educational, low bias current View in Catalog

Rail-to-Rail, 1.8–5.5 V (Single-Supply / ADC Driver)

MCP6001 and TLV9062 are great choices for single-supply operation, ideal for low-voltage systems such as ADC drivers. These op-amps are rail-to-rail input and output, supporting voltages from 1.8V to 5.5V.

Op-Amp Supply Voltage Rail-to-Rail GBW Typical Use Catalog Link
MCP6001 1.8V to 5.5V Yes 1 MHz Low power, ADC driver, single-supply operation View in Catalog
TLV9062 1.8V to 5.5V Yes 10 MHz High-speed, single-supply operation, ADC front-end View in Catalog

Low-Noise Audio / Instrumentation

The OPA2134 is a great choice for low-noise, high-precision applications such as audio preamps and instrumentation. It provides low distortion and is ideal for use in sensitive, high-fidelity audio equipment.

Op-Amp Supply Voltage Rail-to-Rail GBW Typical Use Catalog Link
OPA2134 ±2.25V to ±18V No 8 MHz Low-noise audio preamp, instrumentation View in Catalog

Worked Design: From Spec to Values

This section shows how to take a non inverting amplifier example from specification to component values, and how to check important parameters like gain, GBW, slew rate, and CMVR.

Design Specification & Problem Setup

The goal is to amplify a sensor signal ranging from 50 mV to 300 mV up to 0.5–3.0 V, to fit the input range of a 3.3 V ADC. The chosen gain is Av = 10, ensuring the signal fits within the ADC's range.

Non-inverting amplifier example circuit showing components like resistors, capacitors, and op-amp for signal amplification.

Step-by-Step Design Approach

Step 1: Gain Calculation

We start by calculating the required gain: Av = Vout / Vin. For this design: Vin = 50–300 mV, Vout = 0.5–3.0 V, so the required gain is Av = 10.

The next step is choosing Rin and Rf to set the gain. Using the formula for the non-inverting amplifier: Av = 1 + Rf / Rin, we can calculate the appropriate values. For example, using Rin = 10 kΩ, we can solve for Rf ≈ 90 kΩ.

Step 2: GBW, SR, and CMVR Check

The next step is to ensure that the Gain-Bandwidth Product (GBW) and Slew Rate (SR) are sufficient for the design. We need to ensure that GBW ≥ Av × fsignal to ensure bandwidth sufficiency. For large-signal behavior, the SR must be high enough to avoid distortion. For this design, an op-amp with a GBW of at least 100 MHz would be a good choice.

For the Common-Mode Voltage Range (CMVR), ensure that the non-inverting input signal falls within the op-amp's CMVR. This is especially important in single-supply designs, where the input must stay above the ground voltage and below the supply voltage.

Step 3: Front-End RC and Output Series Resistor

We add a low-pass filter to the front-end to prevent aliasing by setting an appropriate cutoff frequency: fc ≈ fs / 10 where fs is the sampling frequency of the ADC. Using fc = 10 kHz and solving for RRC = 1 kΩ and CRC = 220 nF, we design the filter.

Finally, we include a series resistor at the output to drive the ADC's sample-and-hold capacitor. We select Riso = 22 Ω to isolate the load.

Final Values & Design Check

The final component values are:

  • Rin = 10 kΩ
  • Rf ≈ 90 kΩ
  • Front-end filter: RRC = 1 kΩ, CRC = 220 nF
  • Output isolation: Riso = 22 Ω
These values ensure that the sensor signal is amplified correctly to fit the 3.3 V ADC input range without distortion.

 

Design Limitations & Considerations

Some potential limitations to consider:

  • Bias current: High-source impedance may cause offset errors. Compensate with biasing resistors if necessary.
  • Bandwidth and gain balance: As gain increases, the available bandwidth decreases. This trade-off must be balanced for optimal performance.

 

Conclusion

By following this design flow and using the calculated component values, the sensor signal is amplified to the desired range for the ADC input. The design ensures stability, minimal distortion, and optimal performance for real-world applications.

Frequently Asked Questions

Below are answers to the most frequently asked questions about the non inverting amplifier. Click to expand and view more details.

What is a non inverting amplifier?

A non inverting amplifier is a type of operational amplifier (op-amp) circuit where the input signal is applied to the non-inverting (+) input. The output signal is in the same phase as the input, and the amplifier provides a gain greater than or equal to 1. See more in the introduction.

What is the formula for a non inverting op-amp?

The formula for the gain of a non-inverting amplifier is: A_v = 1 + \frac{R_f}{R_{in}} For example, if R_{in} = 10 kΩ and R_f = 90 kΩ, then the gain is: A_v = 1 + 90k/10k = 10. See more in the gain derivation section.

What is the phase difference in a non inverting amplifier?

The phase difference in a non-inverting amplifier is , meaning the output signal is in phase with the input signal. The gain-bandwidth product (GBW) and slew rate (SR) do not affect the phase inversion, as the signal remains non-inverted.

Difference between inverting and non inverting amplifier?

The key differences between an inverting and a non-inverting amplifier are:

Field Inverting Amplifier Non-Inverting Amplifier
Input Inverting (−) input Non-inverting (+) input
Phase 180° out of phase In-phase (0°)
Gain Formula Av = −Rf/Rin Av = 1 + Rf/Rin
Input Impedance Low (≈Rin) High (≈Rin)
Typical Use Inverting gain, active filters Buffer, ADC driver, sensor signal conditioning
Why use a non inverting amplifier instead of inverting?

A non inverting amplifier is often chosen because it offers high input impedance, making it suitable for buffering high-impedance sources. Additionally, it serves as a voltage follower and is commonly used to drive ADC inputs without introducing phase inversion.

Can a non-inverting amplifier have gain <1?

No, the gain of a non-inverting amplifier must be ≥ 1. If you need a gain of exactly 1, use a voltage follower configuration, which effectively provides no amplification while maintaining unity gain.

References + Downloadables

Below are some high-quality reference materials that provide deeper insights into the non inverting amplifier design and usage. These resources come from industry leaders and are valuable for further reading and design support.

Industry Application Notes & Models

Downloadable Resources

Click to download helpful resources in PDF format for quick reference and practical design guides.

Non-inverting Amplifier Cheat Sheet

A quick reference for the non-inverting amplifier formula and essential design checks. Great for fast calculations and decisions during design.

Download PDF

Inverting vs Non-Inverting Quick Table

A side-by-side comparison table for inverting and non-inverting amplifiers, highlighting key differences and helping you make fast design decisions.

Download PDF

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Ersa

Anastasia is a dedicated writer who finds immense joy in crafting technical articles that aim to disseminate knowledge about integrated circuits (ICs). Her passion lies in unraveling intricate concepts and presenting them in a simplified manner, making them easily understandable for a diverse range of readers.