dBµV
Reading Voltage on a Decibel Scale
Working with signals that span microvolts at a receiver front end up to volts at a transmitter output makes a linear voltage axis impractical. The dBµV unit compresses that range by expressing every level as a logarithmic ratio against a fixed 1 microvolt reference. Because the scaling factor is 20 rather than 10, the unit follows the field-quantity convention used for voltage and current, not the power convention used by the bel. A 10:1 change in voltage is therefore 20 dB, and a 2:1 change is roughly 6.02 dB. This keeps instrument readouts positive and easy to compare: an EMI receiver noise floor near 5 dBµV and a strong ambient broadcast carrier near 110 dBµV sit comfortably on the same display.
The unit is unavoidable in electromagnetic compatibility testing. CISPR 16 receivers, FCC Part 15 conducted-emission limits, and automotive CISPR 25 component limits all specify thresholds in dBµV measured across a 50Ω line impedance stabilization network. Radiated limits are specified in dBµV/m, a field-strength version of the same scale. Because the underlying physical measurement is the voltage developed across the instrument input, dBµV maps directly onto the receiver hardware without assuming any power is actually transferred into a matched load, which is what makes it the natural unit for compliance instrumentation.
Converting to power-referenced units requires a known impedance. In a 50Ω system the 1 microvolt reference develops 0.02 pW, which is about −107 dBm, so the conversion collapses to a single constant offset. The offset shifts for other impedances, which is why a 75Ω cable-television measurement and a 50Ω EMI measurement of the identical voltage report different dBm values. Engineers should always confirm the system impedance before applying any dBµV-to-dBm relationship.
Core Conversion Equations
V(dBµV) = 20 × log10(VRMS / 1µV)
dBµV to dBm (50Ω):
P(dBm) ≈ V(dBµV) − 107
dBµV to dBm (75Ω):
P(dBm) ≈ V(dBµV) − 108.75
Field strength via antenna factor:
E(dBµV/m) = V(dBµV) + AF(dB/m) + Lcable(dB)
Where VRMS = measured RMS voltage, AF = antenna factor, Lcable = cable loss. Example: 60 dBµV in 50Ω → −47 dBm; with AF = 8 dB/m and 2 dB cable loss → 70 dBµV/m.
Reference Levels and Conversions
| Level (dBµV) | Linear voltage | dBm @ 50Ω | dBm @ 75Ω | Typical context |
|---|---|---|---|---|
| 0 | 1 µV | −107 | −108.75 | Sensitive receiver floor |
| 20 | 10 µV | −87 | −88.75 | Weak signal / margin test |
| 40 | 100 µV | −67 | −68.75 | CISPR conducted limit zone |
| 60 | 1 mV | −47 | −48.75 | Strong in-band signal |
| 107 | ≈224 mV | 0 | −1.75 | 1 mW reference in 50Ω |
| 120 | 1 V | +13 | +11.25 | Transmitter / generator level |
Frequently Asked Questions
How do I convert dBuV to dBm in a 50-ohm system?
In 50Ω the conversion is a fixed offset: P(dBm) = V(dBµV) − 107, because a 1 microvolt RMS reference develops 0.02 pW (about −107 dBm) across 50Ω. So 60 dBµV = −47 dBm and 0 dBµV = −107 dBm. In a 75Ω system the offset becomes −108.75. Confirm the system impedance first, since EMI receivers default to 50Ω while broadcast and cable gear often use 75Ω.
Why do EMI receivers and field-strength meters display results in dBuV rather than dBm?
Standards such as CISPR 22, FCC Part 15, and CISPR 25 set conducted limits in dBµV at a 50Ω LISN and radiated limits in dBµV/m. Voltage is the quantity physically present at the antenna or LISN terminal, so a voltage-referenced decibel maps directly to the instrument input without assuming a matched power transfer. It also keeps displayed numbers positive, with noise floors near 0 to 10 dBµV and strong signals at 100 to 140 dBµV.
What is the difference between dBuV and dBuV per meter?
dBµV is a voltage referenced to 1 microvolt at a connector or receiver input; dBµV/m is an electric field strength referenced to 1 microvolt per meter in space. They are linked by the measuring antenna's antenna factor: E(dBµV/m) = V(dBµV) + AF(dB/m) + cable loss. A 42 dBµV reading with AF = 8 dB/m and 2 dB cable loss corresponds to 52 dBµV/m. Omitting the antenna factor is a common radiated-emissions error.