Analyze resistor thermal noise with flexible engineering inputs. Inspect voltage, current, power, and density outputs. Plot bandwidth trends, export reports, and verify sample cases.
Johnson noise is thermal noise generated by a resistor. This calculator uses the standard rms voltage, rms current, and available noise power relationships for a resistive source.
Where k is the Boltzmann constant, T is absolute temperature in kelvin, R is resistance in ohms, and B is bandwidth in hertz.
| Resistance | Temperature | Bandwidth | RMS Noise Voltage | RMS Noise Current | Noise Power |
|---|---|---|---|---|---|
| 50 Ω | 290 K | 1 MHz | 0.895 µV | 17.897 nA | -113.98 dBm |
| 1 kΩ | 300 K | 1 kHz | 0.129 µV | 0.129 nA | -143.83 dBm |
| 10 kΩ | 300 K | 100 kHz | 4.070 µV | 0.407 nA | -123.83 dBm |
| 1 MΩ | 300 K | 1 Hz | 0.129 µV | 0.129 pA | -173.83 dBm |
Johnson noise is the random electrical noise produced by thermal agitation of charge carriers inside a resistor. It exists even without applied voltage and increases with temperature, resistance, and bandwidth.
Noise power accumulates across the observation bandwidth. A wider measurement bandwidth includes more random noise energy, so rms noise voltage and current increase as bandwidth increases.
The formula uses thermodynamic temperature. That means the calculation must internally use kelvin, even if you enter Celsius or Fahrenheit values at the form level.
For the same temperature and bandwidth, yes. Open-circuit rms voltage noise grows with the square root of resistance, while short-circuit rms current noise falls with the square root of resistance.
It expresses available thermal noise power relative to 1 milliwatt. This is useful in RF and instrumentation work where designers compare weak signals and noise floors on a logarithmic scale.
Spectral density shows noise per square root of hertz. It helps compare components independent of total bandwidth and is commonly listed as nV/√Hz or pA/√Hz.
No. It handles the resistor thermal-noise part only. Real circuits may also include amplifier noise, source impedance effects, filtering, matching losses, and frequency-dependent behavior.
It is useful during sensor, amplifier, RF, data-acquisition, and low-level measurement design. It quickly estimates whether thermal noise will limit the minimum detectable signal.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.