dBm is one of the most common units in radio-frequency engineering, but it can be confusing when RF equipment is also specified in milliwatts or watts. A transmitter may be rated at 30 dBm, an SDR input may have a safe limit expressed in dBm, an RF power meter may display -20 dBm, while an amplifier may be advertised as 5 W.
Fortunately, dBm to watts conversion follows a simple logarithmic relationship. The most important reference point is:
0 dBm = 1 milliwatt = 0.001 watt
From there, every increase of 10 dB multiplies power by 10. That means 10 dBm is 10 mW, 20 dBm is 100 mW, 30 dBm is 1 W, 40 dBm is 10 W, and 50 dBm is 100 W.
This guide includes a dBm to watts calculator, watts to dBm calculator, conversion formulas, common RF power tables, practical SDR and transmitter examples, dBm vs dB vs dBW explanations, 50-ohm voltage examples, and safe RF measurement advice.
Browse RF power meters, RF dummy loads, RF test and measurement equipment, software-defined radio hardware, and request a formal RF equipment quote from SDRstore.eu.
Enter a value below to convert dBm to watts, milliwatts, microwatts, nanowatts, and picowatts. You can also convert watts back to dBm.
| dBm | Watts | Common unit |
|---|---|---|
| -120 dBm | 0.000000000000001 W | 1 fW |
| -110 dBm | 0.00000000000001 W | 10 fW |
| -100 dBm | 0.0000000000001 W | 0.1 pW |
| -90 dBm | 0.000000000001 W | 1 pW |
| -80 dBm | 0.00000000001 W | 10 pW |
| -70 dBm | 0.0000000001 W | 100 pW / 0.1 nW |
| -60 dBm | 0.000000001 W | 1 nW |
| -50 dBm | 0.00000001 W | 10 nW |
| -40 dBm | 0.0000001 W | 100 nW / 0.1 µW |
| -30 dBm | 0.000001 W | 1 µW |
| -20 dBm | 0.00001 W | 10 µW |
| -10 dBm | 0.0001 W | 100 µW / 0.1 mW |
| 0 dBm | 0.001 W | 1 mW |
| 10 dBm | 0.01 W | 10 mW |
| 20 dBm | 0.1 W | 100 mW |
| 30 dBm | 1 W | 1 W |
| 40 dBm | 10 W | 10 W |
| 50 dBm | 100 W | 100 W |
| 60 dBm | 1000 W | 1 kW |
To convert dBm to watts:
P(W) = 10^((dBm - 30) / 10)
To convert dBm directly to milliwatts:
P(mW) = 10^(dBm / 10)
P(W) = 10^((20 - 30) / 10)
P(W) = 10^-1 = 0.1 W
Therefore:
20 dBm = 0.1 W = 100 mW
P(W) = 10^((30 - 30) / 10)
P(W) = 10^0 = 1 W
Therefore:
30 dBm = 1 W
P(W) = 10^((-60 - 30) / 10)
P(W) = 10^-9 W
Therefore:
-60 dBm = 1 nW
To convert watts to dBm:
dBm = 10 × log10(P(W)) + 30
If the power is already expressed in milliwatts:
dBm = 10 × log10(P(mW))
dBm = 10 × log10(5) + 30
dBm ≈ 36.99 dBm
Therefore:
5 W ≈ 37 dBm
dBm = 10 × log10(100) + 30
dBm = 50 dBm
Therefore:
100 W = 50 dBm
| dBm | mW | Watts |
|---|---|---|
| 0 dBm | 1 mW | 0.001 W |
| 1 dBm | 1.259 mW | 0.001259 W |
| 2 dBm | 1.585 mW | 0.001585 W |
| 3 dBm | 1.995 mW | 0.001995 W |
| 4 dBm | 2.512 mW | 0.002512 W |
| 5 dBm | 3.162 mW | 0.003162 W |
| 6 dBm | 3.981 mW | 0.003981 W |
| 7 dBm | 5.012 mW | 0.005012 W |
| 8 dBm | 6.310 mW | 0.006310 W |
| 9 dBm | 7.943 mW | 0.007943 W |
| 10 dBm | 10 mW | 0.01 W |
| 13 dBm | 19.95 mW | 0.01995 W |
| 14 dBm | 25.12 mW | 0.02512 W |
| 17 dBm | 50.12 mW | 0.05012 W |
| 20 dBm | 100 mW | 0.1 W |
| 23 dBm | 199.5 mW | 0.1995 W |
| 24 dBm | 251.2 mW | 0.2512 W |
| 27 dBm | 501.2 mW | 0.5012 W |
| 30 dBm | 1000 mW | 1 W |
| 33 dBm | 1995 mW | 1.995 W |
| 36 dBm | 3981 mW | 3.981 W |
| 37 dBm | 5012 mW | 5.012 W |
| 40 dBm | 10000 mW | 10 W |
| 43 dBm | 19950 mW | 19.95 W |
| 46 dBm | 39810 mW | 39.81 W |
| 47 dBm | 50120 mW | 50.12 W |
| 50 dBm | 100000 mW | 100 W |
| 53 dBm | 199500 mW | 199.5 W |
| 57 dBm | 501200 mW | 501.2 W |
| 60 dBm | 1000000 mW | 1000 W |
You do not need a calculator for every RF power estimate.
| Power | dBm |
|---|---|
| 1 mW | 0 dBm |
| 10 mW | 10 dBm |
| 100 mW | 20 dBm |
| 1 W | 30 dBm |
| 10 W | 40 dBm |
| 100 W | 50 dBm |
| 1 kW | 60 dBm |
The exact increase for double power is approximately 3.0103 dB, but the 3 dB rule is very useful for quick RF calculations.
If a 1 W or 30 dBm signal passes through a 3 dB attenuator:
30 dBm - 3 dB = 27 dBm
27 dBm is approximately 0.5 W.
dBm means decibels relative to one milliwatt.
The “m” is important because it defines the reference power:
0 dBm = 1 mW
Unlike plain dB, dBm represents an absolute power level.
| Unit | Meaning | Example |
|---|---|---|
| dBm | Absolute power referenced to 1 mW | 20 dBm = 100 mW. |
| dB | Relative gain or loss | A 20 dB attenuator reduces power by a factor of 100. |
This distinction makes RF link calculations convenient because a gain or loss in dB can be added directly to an absolute power level in dBm.
Suppose an SDR produces:
10 dBm
and an amplifier provides:
+20 dB gain
Ignoring losses:
10 dBm + 20 dB = 30 dBm
30 dBm equals 1 W.
Suppose a transmitter produces:
30 dBm
and you install a:
40 dB attenuator
The output becomes:
30 dBm - 40 dB = -10 dBm
-10 dBm equals 0.1 mW or 100 µW.
This type of calculation is essential before connecting a transmitter to a sensitive SDR receiver or spectrum analyzer.
A common beginner mistake is adding two independent power levels expressed in dBm.
20 dBm + 20 dBm does not equal 40 dBm.
Each 20 dBm source is 100 mW.
If two ideal independent 100 mW powers are combined:
100 mW + 100 mW = 200 mW
200 mW is approximately:
23 dBm
When adding actual powers:
This is different from adding a gain or loss in dB to a power level in dBm.
dBW is another logarithmic power unit, but its reference is one watt rather than one milliwatt.
The conversion is:
dBW = dBm - 30
dBm = dBW + 30
| Watts | dBm | dBW |
|---|---|---|
| 1 mW | 0 dBm | -30 dBW |
| 100 mW | 20 dBm | -10 dBW |
| 1 W | 30 dBm | 0 dBW |
| 10 W | 40 dBm | 10 dBW |
| 100 W | 50 dBm | 20 dBW |
| 1000 W | 60 dBm | 30 dBW |
No. Converting dBm to watts does not require knowing impedance.
30 dBm is 1 W whether the system is 50 ohms, 75 ohms, or another impedance.
Impedance matters when converting power into voltage or current.
For a resistive load:
V(RMS) = √(P × R)
| dBm | Power | Approx. voltage RMS into 50 Ω |
|---|---|---|
| 0 dBm | 1 mW | 0.224 V RMS |
| 10 dBm | 10 mW | 0.707 V RMS |
| 20 dBm | 100 mW | 2.236 V RMS |
| 30 dBm | 1 W | 7.071 V RMS |
| 40 dBm | 10 W | 22.36 V RMS |
These voltage values assume the stated RF power is delivered into a matched 50-ohm resistive load.
RF systems can involve enormous power ranges. A sensitive receiver may work with signals around -100 dBm while a transmitter can output +40 dBm or more.
In watts, those numbers become awkward:
dBm compresses this huge range into numbers that are easier to calculate and compare.
It also makes link budgets simple because gains and losses expressed in dB can be added or subtracted.
Suppose a transmitter starts at:
20 dBm
The RF chain contains:
The final power is:
20 + 10 - 2 - 20 = 8 dBm
8 dBm equals approximately 6.31 mW.
This is much easier than converting every stage into watts and multiplying individual power ratios.
The exact power level varies by device, band, hardware revision, gain configuration, and regulation, but these ranges help put dBm into context.
| Power range | Typical interpretation |
|---|---|
| -120 to -90 dBm | Very weak receiver-level signals. |
| -90 to -60 dBm | Common weak-to-moderate received radio signals. |
| -60 to -30 dBm | Strong receiver input levels in many SDR applications. |
| -30 to 0 dBm | Very strong for sensitive receiver inputs; common controlled lab signal levels. |
| 0 to +20 dBm | Signal-generator, SDR TX, module, or low-power transmitter territory depending on hardware. |
| +20 to +30 dBm | 100 mW to 1 W. |
| +30 to +40 dBm | 1 W to 10 W transmitter power. |
| +40 to +50 dBm | 10 W to 100 W high-power RF equipment. |
These ranges are examples rather than safe-input recommendations. Always check the actual maximum input specification of the connected device.
This is one of the most important practical uses of dBm conversion.
An SDR receiver is designed for weak radio signals. Connecting a transmitter directly to the receiver can overload or permanently damage the front end.
Consider this example:
Transmitter output:
30 dBm = 1 W
Desired receiver input:
-20 dBm = 10 µW
Required reduction:
30 dBm - (-20 dBm) = 50 dB
You therefore need approximately 50 dB of total path loss to reduce the ideal conducted level from 1 W to 10 µW.
That attenuation might include:
Always include margin and verify the result with a suitable RF power meter before connecting expensive equipment.
A 10 W transmitter produces:
40 dBm
Suppose the analyzer input should remain at or below:
-10 dBm
The required attenuation is:
40 - (-10) = 50 dB
A theoretical 50 dB attenuator chain would reduce:
40 dBm → -10 dBm
However, the attenuator connected closest to the transmitter must also be able to dissipate the input power. A small SMA attenuator is not automatically safe simply because its attenuation value is correct.
Check:
Both can display signal power in dBm, but their jobs are different.
| Tool | Best use |
|---|---|
| RF power meter | Direct conducted RF power measurement within its specified frequency and power range. |
| Spectrum analyzer | Viewing power distributed across frequency, harmonics, spurs, interference, and signal bandwidth. |
| SDR | IQ capture, decoding, demodulation, and relative signal analysis. |
Browse RF power meters at SDRstore.eu.
Read: What Is a Spectrum Analyzer? Beginner Guide for RF Testing.
A dummy load provides a controlled RF termination, normally 50 ohms in common radio systems, and absorbs transmitter power instead of radiating it from an antenna.
This makes dummy loads useful for:
A dummy load also needs the correct frequency range and power rating.
A 1 W transmitter should not be connected to a load designed for only a few milliwatts, and a 100 W transmitter requires a load capable of dissipating substantial heat.
Browse RF dummy loads.
0 dBm = 1 mW = 0.001 W.
10 dBm = 10 mW = 0.01 W.
20 dBm = 100 mW = 0.1 W.
23 dBm ≈ 199.5 mW ≈ 0.2 W.
27 dBm ≈ 501 mW ≈ 0.5 W.
30 dBm = 1000 mW = 1 W.
33 dBm ≈ 1.995 W, commonly approximated as 2 W.
37 dBm ≈ 5.012 W, commonly approximated as 5 W.
40 dBm = 10 W.
43 dBm ≈ 19.95 W, commonly approximated as 20 W.
47 dBm ≈ 50.12 W, commonly approximated as 50 W.
50 dBm = 100 W.
60 dBm = 1000 W = 1 kW.
Negative dBm does not mean negative power.
It means the power is below the 1 mW reference level.
| dBm | Power |
|---|---|
| -10 dBm | 0.1 mW |
| -20 dBm | 0.01 mW / 10 µW |
| -30 dBm | 1 µW |
| -40 dBm | 0.1 µW / 100 nW |
| -50 dBm | 10 nW |
| -60 dBm | 1 nW |
| -70 dBm | 0.1 nW |
| -80 dBm | 10 pW |
| -90 dBm | 1 pW |
| -100 dBm | 0.1 pW |
Receiver work routinely involves extremely small powers, which is one reason dBm is much more convenient than watts.
Receiver sensitivity is often expressed in dBm because the signals involved are tiny.
Consider two hypothetical receivers:
The difference is 10 dB.
-110 dBm is one-tenth the power of -100 dBm, so Receiver B can theoretically detect a signal ten times weaker under the stated test conditions.
However, sensitivity comparisons are only meaningful when bandwidth, modulation, data rate, required BER/PER or SNR, noise figure, and measurement method are comparable.
Spectrum analyzers usually display signal level in dBm because they may need to show both very weak and comparatively strong RF signals on the same logarithmic scale.
For example:
The differences can then be read directly in dB.
Read: What Is a Spectrum Analyzer?.
RF signal generators commonly specify output level in dBm because engineers often need precise, repeatable signal levels for receiver testing.
For example, a receiver test may gradually reduce generator power:
-50 dBm
-60 dBm
-70 dBm
-80 dBm
-90 dBm
-100 dBm The engineer can then determine the signal level where the receiver stops meeting its required performance.
Read: What Is a Signal Generator? RF Signal Generators Explained for Beginners.
Suppose an amplifier has 20 dB gain.
If the input is:
-10 dBm
the ideal output is:
-10 dBm + 20 dB = 10 dBm
10 dBm equals 10 mW.
If the amplifier input rises to:
10 dBm
the ideal linear calculation gives:
10 dBm + 20 dB = 30 dBm = 1 W
But real amplifiers cannot increase output indefinitely. Output eventually reaches compression, saturation, thermal, voltage, current, or device limits.
Always check:
Attenuators are particularly easy to calculate when power is expressed in dBm.
| Input | Attenuation | Output |
|---|---|---|
| 20 dBm | 3 dB | 17 dBm |
| 20 dBm | 10 dB | 10 dBm |
| 20 dBm | 20 dB | 0 dBm |
| 20 dBm | 30 dB | -10 dBm |
| 30 dBm | 30 dB | 0 dBm |
| 40 dBm | 50 dB | -10 dBm |
Attenuators can also be combined:
10 dB + 20 dB + 20 dB = 50 dB total attenuation
However, check the power rating of every attenuator in the chain. The first attenuator receives the highest power and therefore normally has the most demanding dissipation requirement.
dBm is absolute power. dB is a relative ratio.
It does not. -30 dBm is a positive physical power of 1 µW.
20 dBm + 20 dBm is not 40 dBm. Convert the powers to linear units first.
3 dB is an excellent approximation. Exact doubling is approximately 3.0103 dB.
dBm to watts conversion does not depend on impedance. Voltage and current conversion do.
A 30 dBm transmitter does not necessarily deliver 30 dBm at the antenna after cable, connector, filter, and switch losses.
Convert and calculate the full path first. Use rated attenuation and verify safe input limits.
A practical conducted RF bench can include:
A typical transmitter measurement path might be:
Transmitter
→ rated directional coupler or attenuator
→ RF power meter / spectrum analyzer measurement path
→ rated 50-ohm dummy load The exact topology depends on transmitter power, frequency, measurement equipment, and required measurement accuracy.
dBm calculations become particularly useful during RF product development.
Engineers may need to compare:
Read: SDR Hardware for RF Product Testing: Pre-Compliance, Interference, and Signal Validation.
Best for: learning dBm, measuring signal-generator output, low-power transmitter testing, and basic RF bench work.
Best for: controlled SDR transmit experiments, GNU Radio projects, RF validation, and safe receiver testing.
Best for: amateur radio, service labs, transmitter alignment, RF amplifier testing, and higher-power product development.
An RF power meter is required to measure conducted transmitter and signal-generator power in dBm and watts, validate attenuator chains, verify amplifier output, and protect sensitive RF test equipment from excessive input levels.
Fixed and variable RF attenuators are required to reduce known transmitter power by controlled dB values, protect SDR and analyzer inputs, simulate path loss, and create repeatable receiver-sensitivity measurements.
A rated 50-ohm dummy load is required to absorb RF transmitter power without unnecessary radiation and provide a controlled termination for conducted power, SWR, amplifier, and transmitter testing.
Universities, RF laboratories, amateur-radio organizations, telecom teams, IoT developers, product-testing groups, cybersecurity labs, and public-sector buyers can request a formal quotation directly from SDRstore.eu.
Use the Add to Quote button on product pages or the document icon on product cards. Add RF power meters, dummy loads, SDRs, spectrum analyzers, NanoVNA/VNA equipment, cables, filters, attenuators, adapters, and project requirements to one quote request.
A quote request is useful for:
Read the SDRstore.eu quote-request guide.
The fastest way to understand dBm is to remember three reference points:
Then remember that every +10 dB multiplies power by ten and approximately +3 dB doubles power.
Use dBm when working with SDR receivers, spectrum analyzers, signal generators, amplifiers, attenuators, RF power meters, and link budgets because gains and losses become easy to calculate. Convert back to watts when you need to understand actual transmitter power, thermal dissipation, dummy-load ratings, or equipment safety.
Most importantly, never connect RF equipment based only on a rough dBm-to-watts conversion. Check the actual input limit, frequency range, attenuation, power rating, impedance, and complete RF path before connecting a transmitter to a receiver or test instrument.
dBm is an absolute logarithmic power unit referenced to one milliwatt. 0 dBm equals 1 mW.
Use P(W) = 10^((dBm - 30) / 10). For example, 30 dBm converts to 1 watt.
Use dBm = 10 × log10(P(W)) + 30. For example, 10 watts converts to 40 dBm.
20 dBm equals 0.1 watt, or 100 milliwatts.
30 dBm equals exactly 1 watt.
40 dBm equals 10 watts.
50 dBm equals 100 watts.
60 dBm equals 1000 watts, or 1 kilowatt.
-30 dBm is still positive power. It equals 1 microwatt, or 0.000001 watt.
dBm represents an absolute power level referenced to 1 mW. dB represents a relative gain or loss. A 20 dB amplifier can therefore increase a -10 dBm signal to an ideal +10 dBm output.
dBm is referenced to 1 milliwatt, while dBW is referenced to 1 watt. dBW equals dBm minus 30.
No. Power conversion between dBm and watts does not depend on impedance. Impedance becomes necessary when converting the power into voltage or current.
Approximately. An exact doubling of power is about +3.0103 dB. The +3 dB rule is normally accurate enough for quick RF calculations.
Not when they represent two independent powers. Convert each dBm value to watts or milliwatts, add the linear powers, then convert the result back to dBm. Gains and losses expressed in dB can be added directly to a dBm power level.
Yes. Use the Add to Quote button on product pages or the document icon on product cards. Add RF power meters, dummy loads, SDRs, spectrum analyzers, attenuators, cables, adapters, and project notes so the complete RF measurement setup can be quoted together.
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