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๐Ÿ“ก

Resistor Noise

Johnson-Nyquist thermal noise: V_n = โˆš(4kTRB). All resistors at T > 0 K generate white noise. Excess noise from DC current.

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V_n = โˆš(4kTRB). 1 kฮฉ at 300 K, 1 kHz BW: V_n โ‰ˆ 4 nV. Spectral density โˆš(4kTR) โ‰ˆ 0.13 nV/โˆšHz per โˆš(kฮฉ) at 300 K. Excess noise: carbon comp high; metal film, foil low. SNR = 10 logโ‚โ‚€(P_signal/P_noise) dB.

Key quantities
V_n = โˆš(4kTRB)
Johnson Noise
Key relation
โˆš(4kTR) V/โˆšHz
Spectral Density
Key relation
โˆ IยทโˆšRยทB
Excess Noise
Key relation
Signal/Noise power
SNR
Key relation

Ready to run the numbers?

Why: Low-noise amplifiers, sensors, and RF systems require noise budgeting. Johnson noise sets fundamental limit.

How: Thermal noise: V_n = โˆš(4kTRB). k=1.38ร—10โปยฒยณ J/K. Excess noise index (dB) for carbon comp; metal film quieter.

V_n = โˆš(4kTRB). 1 kฮฉ at 300 K, 1 kHz BW: V_n โ‰ˆ 4 nV.Spectral density โˆš(4kTR) โ‰ˆ 0.13 nV/โˆšHz per โˆš(kฮฉ) at 300 K.

Run the calculator when you are ready.

Calculate Resistor NoiseEnter resistance, temperature, bandwidth for Johnson-Nyquist and excess noise

๐ŸŽš๏ธ Low Noise Preamplifier Design

Designing input stage for precision audio amplifier with 10kฮฉ resistor

๐Ÿ“ก Sensor Interface Circuit

Temperature sensor with 1kฮฉ pull-up resistor at 50kHz bandwidth

๐Ÿ”ฌ Precision Measurement System

High-precision voltage measurement with 100kฮฉ reference resistor

๐Ÿ”Š Audio Amplifier Input

Audio preamp with 47kฮฉ input resistor, 20Hz-20kHz bandwidth

๐Ÿ“ป RF Receiver Frontend

RF frontend with 50ฮฉ matching resistor at 1MHz bandwidth

๐ŸŒก๏ธ High Temperature Application

Resistor at elevated temperature (100ยฐC) for industrial application

Input Parameters

Frequency Spectrum Analysis (Optional)

โ“ Frequently Asked Questions

What is Johnson-Nyquist noise and why does it occur?

Johnson-Nyquist noise (also called thermal noise) is the random voltage fluctuations generated by all resistors due to the thermal motion of charge carriers. It occurs at any temperature above absolute zero and is white noise with constant spectral density. The noise voltage is proportional to the square root of resistance, temperature, and bandwidth.

How does excess noise differ from thermal noise?

Excess noise (also called current noise or 1/f noise) occurs when DC current flows through a resistor. Unlike thermal noise which is always present, excess noise depends on the resistor material, construction, and DC voltage. Wire-wound resistors have the lowest excess noise, while carbon resistors have the highest. Excess noise typically increases with frequency as 1/f noise.

What is noise spectral density and why is it important?

Noise spectral density (en) is the noise voltage per square root of bandwidth, measured in V/โˆšHz. It's frequency-independent for thermal noise (white noise), making it useful for noise analysis at any frequency. To find total noise voltage, multiply spectral density by the square root of bandwidth. Typical values range from 0.1 nV/โˆšHz to 100 nV/โˆšHz.

How do I reduce noise in my circuit design?

To reduce noise: (1) Use lower resistance values when possible (noise โˆ โˆšR), (2) Reduce operating temperature, (3) Minimize bandwidth to only what's needed, (4) Choose low-noise resistor types (wire-wound or thin-film), (5) Avoid excess noise by minimizing DC voltage across resistors, (6) Use low-noise op-amps and proper grounding techniques.

What is a good signal-to-noise ratio (SNR)?

SNR requirements vary by application: Audio systems need 60+ dB for high quality, 40-60 dB is acceptable. Precision measurements require 80+ dB. RF systems typically need 20-30 dB minimum. The calculator shows SNR in both linear and dB scales. Higher SNR indicates better signal quality relative to noise floor.

How does temperature affect resistor noise?

Temperature directly affects Johnson-Nyquist noise - noise voltage increases with the square root of absolute temperature. At room temperature (293 K), noise is relatively low. Cooling resistors reduces thermal noise, which is why precision instruments often operate at reduced temperatures. Excess noise is less temperature-dependent but may increase slightly with temperature.

Which resistor types have the lowest noise?

For thermal noise, all resistors have the same Johnson-Nyquist noise at the same temperature and resistance. For excess noise: Wire-wound resistors have the lowest (-40 dB/decade), followed by thin-film (-30 dB/decade), thick-film (-20 dB/decade), and carbon resistors (-10 dB/decade). For low-noise applications, choose wire-wound or precision thin-film resistors.

๐Ÿ“š Official Data Sources

IEEE Standards Association

IEEE standards and publications on electronic noise, Johnson-Nyquist noise, and resistor specifications

Last Updated: 2026-02-07

NIST Electronics and Electrical Engineering Laboratory

National Institute of Standards and Technology standards for electronic components, noise measurements, and thermal noise

Last Updated: 2026-02-07

Electronics Tutorials

Comprehensive tutorials on resistor noise, thermal noise, excess noise, and noise analysis in electronic circuits

Last Updated: 2026-02-07

Analog Devices

Technical articles and application notes on low-noise design, resistor selection, and noise analysis

Last Updated: 2026-02-07

โš ๏ธ Disclaimer: This calculator provides theoretical noise estimates based on standard Johnson-Nyquist and excess noise models. Actual noise values may vary due to resistor manufacturing tolerances, temperature gradients, parasitic capacitances, circuit layout, electromagnetic interference, and component aging. Excess noise indices are typical values and may vary significantly between manufacturers and production batches. For critical applications such as precision instrumentation, medical devices, or low-noise amplifiers, always verify noise measurements using calibrated test equipment and consult manufacturer datasheets. This calculator is for educational and design planning purposes only.

Please enter a valid resistance value greater than 0

For educational and informational purposes only. Verify with a qualified professional.

๐Ÿ”ฌ Physics Facts

๐Ÿ“ก

Johnson (1928) and Nyquist (1928) derived thermal noise from thermodynamics.

โ€” IEEE

๐Ÿ“

White noise: flat spectrum up to ~100 GHz at room temperature.

โ€” NIST

โšก

Excess noise: 1/f at low f; depends on current and material.

โ€” Analog Devices

๐Ÿ“Š

Metal film resistors: ~0.1 ฮผV/V excess noise; carbon comp >10 ฮผV/V.

โ€” Component specs

What is Resistor Noise?

Resistor noise is the random electrical noise generated by resistors due to fundamental physical processes. The primary source is thermal noise (Johnson-Nyquist noise), which arises from the random thermal motion of charge carriers. Additionally, resistors can exhibit excess noise (current noise) when DC current flows through them, which depends on the resistor material and construction.

Johnson-Nyquist Noise

Thermal noise is present in all resistors at any temperature above absolute zero. It's white noise with constant spectral density.

Key Characteristics:

  • Present in all resistors
  • White noise spectrum
  • Proportional to โˆšR
  • Proportional to โˆšT

Noise Spectral Density

Noise voltage per square root of bandwidth. This parameter is frequency-independent for thermal noise.

Units:

  • V/โˆšHz
  • nV/โˆšHz (typical)
  • Frequency independent
  • White noise

Excess Noise

Additional noise that occurs when DC current flows through a resistor. Depends on resistor material and construction.

Resistor Types:

  • Wire-wound: Lowest
  • Thin-film: Low
  • Thick-film: Moderate
  • Carbon: Highest

How Does Resistor Noise Work?

Resistor noise calculations involve understanding thermal noise (Johnson-Nyquist noise), noise spectral density, excess noise, and their impact on signal-to-noise ratio. The calculator uses fundamental physics equations to determine noise characteristics.

๐Ÿ”ฌ Calculation Methods

Johnson-Nyquist Noise

  1. 1Enter resistance value (R) in ohms
  2. 2Enter temperature (T) in Celsius or Kelvin
  3. 3Enter bandwidth (ฮ”f) in Hz
  4. 4Calculate: Vn = โˆš(4kTRฮ”f)

Noise Spectral Density

  • Calculate spectral density: en = โˆš(4kTR)
  • Independent of frequency (white noise)
  • Useful for noise analysis at any frequency
  • Multiply by โˆšbandwidth for total noise

When to Use Resistor Noise Calculator

Resistor noise calculation is essential for electronic engineers designing low-noise circuits, precision measurement systems, audio amplifiers, sensor interfaces, and RF receivers. Understanding noise characteristics helps optimize circuit performance and select appropriate components.

Low Noise Preamplifiers

Design input stages for audio amplifiers, instrumentation amplifiers, and low-noise signal conditioning circuits.

Applications:

  • Audio preamps
  • Instrumentation amps
  • Low-noise op-amps

Precision Measurement

Analyze noise in precision voltage references, ADC input circuits, and high-resolution measurement systems.

Benefits:

  • Noise floor analysis
  • ADC resolution limits
  • Measurement accuracy

RF Receiver Design

Optimize noise performance in RF frontends, matching networks, and receiver input stages.

Design Tasks:

  • Noise figure analysis
  • Matching network design
  • SNR optimization

Resistor Noise Calculation Formulas

Understanding resistor noise formulas is essential for electronic circuit design. These formulas relate noise to resistance, temperature, bandwidth, and signal levels.

๐Ÿ“Š Core Noise Formulas

Johnson-Nyquist Noise (Vn)

Vn=sqrt4kTRDeltafV_n = \\sqrt{4kTR\\Delta f}

Thermal noise voltage in a resistor, where k is Boltzmann's constant (1.38ร—10โปยฒยณ J/K), T is absolute temperature in Kelvin, R is resistance in ohms, and ฮ”f is bandwidth in Hz.

Noise Voltage Spectral Density (en)

en=sqrt4kTR=fracVnsqrtDeltafe_n = \\sqrt{4kTR} = \\frac{V_n}{\\sqrt{\\Delta f}}

Noise voltage per square root of bandwidth. This is frequency-independent for thermal noise (white noise). Typical values range from 0.1 nV/โˆšHz to 100 nV/โˆšHz.

Noise Power (Pn)

Pn=kTDeltafP_n = kT\\Delta f

Available noise power from a resistor. Interestingly, this is independent of resistance value and depends only on temperature and bandwidth. At room temperature (293 K), this is approximately -174 dBm/Hz.

Signal-to-Noise Ratio (SNR)

textSNR=fracVsVn=20log10left(fracVsVnright)textdB\\text{SNR} = \\frac{V_s}{V_n} = 20\\log_{10}\\left(\\frac{V_s}{V_n}\\right) \\text{ dB}

Ratio of signal voltage to noise voltage. Higher SNR indicates better signal quality. Typical requirements range from 20 dB (acceptable) to 60+ dB (high quality).

Excess Noise (Vexcess)

Vtextexcess=VdctimessqrtfracR1textkOmegatimessqrtfracDeltaf1textHztimes10textENI/20V_{\\text{excess}} = V_{dc} \\times \\sqrt{\\frac{R}{1\\text{k}\\Omega}} \\times \\sqrt{\\frac{\\Delta f}{1\\text{Hz}}} \\times 10^{\\text{ENI}/20}

Additional noise that occurs when DC current flows through a resistor. ENI (Excess Noise Index) is typically -40 dB/decade for wire-wound resistors, -30 dB/decade for thin-film, -20 dB/decade for thick-film, and -10 dB/decade for carbon resistors.

Total Noise (Vtotal)

Vtexttotal=sqrtVtextjohnson2+Vtextexcess2V_{\\text{total}} = \\sqrt{V_{\\text{johnson}}^2 + V_{\\text{excess}}^2}

Combined noise from thermal (Johnson-Nyquist) and excess noise sources. Since these are uncorrelated, they add in quadrature (square root of sum of squares).

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