Calculate the thermal (Johnson-Nyquist) noise voltage generated by a resistor at a given temperature and bandwidth.
📊 Thermal RMS noise only, bandwidth-specific. This calculates Johnson-Nyquist thermal noise RMS voltage over the stated bandwidth. Does NOT account for 1/f noise (flicker noise), shot noise, or other real-world resistor noise sources. Real resistor noise depends on type, frequency range, age, and circuit topology.
Thermal noise, also known as Johnson-Nyquist noise, is the electronic noise generated by the thermal agitation of charge carriers (usually electrons) inside an electrical conductor at equilibrium, which happens regardless of any applied voltage.
This noise is "white," meaning its power spectral density is nearly constant throughout the frequency spectrum. It is a fundamental limit to the sensitivity of electronic instruments and amplifiers.
Where:
• v_n is the RMS noise voltage
• k is Boltzmann's constant (1.38 × 10⁻²³ J/K)
• T is the absolute temperature in Kelvin
• R is the resistance in Ohms
• Δf is the bandwidth in Hertz
No, thermal noise is present even when no current is flowing. This fundamental property makes thermal noise a limiting factor in all passive components. However, some resistors (like carbon composition) generate additional 'excess noise' when current flows, which is separate from thermal noise.
Several strategies work: (1) Use lower resistance values—noise is proportional to R, (2) Reduce operating temperature—noise is proportional to T, (3) Limit measurement bandwidth—only measure the frequencies you need, (4) Use low-noise amplifiers after the resistor, (5) Select low-noise resistor types (metal film are better than carbon film).
Thermal noise is "white," meaning its power is evenly distributed across all frequencies. The total noise power you measure is proportional to the bandwidth you're measuring. If your circuit has a 1 kHz bandwidth, you capture all noise in that range. Doubling bandwidth doubles noise power. This is why precision measurements use narrowband filters.
Noise is the random signal component from thermal motion, shot noise, etc. Noise floor is the cumulative effect of all noise sources in a system (resistors, amplifiers, instruments). For example, a 10 μV noise floor means your system cannot reliably measure signals below 10 μV because they're masked by noise.
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