dB Converter
Convert between decibels and voltage / power ratios in both directions.
Enter dB value
Common values
Results
Formulas
dB (voltage ref)
dB = 20 · log₁₀(Vout / Vin)dB (power ref)
dB = 10 · log₁₀(Pout / Pin)Ratio from dB
ratio = 10^(dB/20) [voltage]Common dB Reference Values
| dB | Voltage Ratio | Power Ratio | Meaning |
|---|---|---|---|
| -20 dB | 0.1× | 0.01× | 1/10 voltage, 1/100 power |
| -10 dB | 0.316× | 0.1× | 1/10 power |
| -6 dB | 0.5× | 0.25× | Half voltage |
| -3 dB | 0.707× | 0.5× | Half power (-3 dB point) |
| 0 dB | 1× | 1× | No change (unity) |
| +3 dB | 1.414× | 2× | Double power |
| +6 dB | 2× | 4× | Double voltage |
| +10 dB | 3.162× | 10× | 10× power |
| +20 dB | 10× | 100× | 10× voltage, 100× power |
| +40 dB | 100× | 10000× | 100× voltage |
| +60 dB | 1000× | 10⁶× | 1000× voltage |
Understanding decibels
When to use this: Use this to convert between decibels and voltage or power ratios — for filter design, amplifier gain calculations, audio signal levels, and RF system link budgets. The reference table below is useful for instant mental math without entering values.
Decibels exist because our ears and many measurement instruments respond logarithmically, not linearly. A 10× increase in power sounds roughly 'twice as loud', not ten times louder. Using dB compresses wide ratios into manageable numbers: a 1,000,000:1 power ratio becomes just 60dB. An amplifier with 1,000,000× voltage gain is a '120dB amplifier'. Both are easier to work with.
There are two dB formulas and mixing them up is a common mistake. For power ratios: dB = 10 × log₁₀(P₂/P₁). For voltage or amplitude ratios: dB = 20 × log₁₀(V₂/V₁). The factor of 2 difference comes from the fact that power is proportional to voltage squared (P = V²/R). Both formulas give the same dB value for the same underlying power change.
This is why −3dB means two different things depending on what you're measuring. In power: −3dB is half the power (×0.5). In voltage: −3dB is 70.7% of the amplitude (×1/√2 ≈ 0.707). Filter cutoff frequencies are defined at −3dB because that's where output power drops to half — a natural engineering threshold.
The dBm scale pins a specific power level: 0dBm = 1mW. From there, +10dBm = 10mW, +20dBm = 100mW, +30dBm = 1W, −30dBm = 1µW. RF engineers use dBm to describe everything from transmitter output (+20 to +40dBm) to received signal levels (−70 to −100dBm). A signal 40dB below the noise floor is essentially undetectable.
A few values worth memorizing: +3dB doubles the power, +6dB doubles the voltage, +10dB multiplies power by 10, +20dB multiplies voltage by 10. Going negative reverses all of these. Filter spec sheets often state attenuation in dB: a −60dB stopband means the blocked signal is 1000× smaller in voltage. These numbers quickly become second nature.
Key Reference Points
- −3 dB ≈ half power, 70.7% of voltage
- −6 dB ≈ half voltage, 25% of power
- −20 dB = ÷10 voltage, ÷100 power
- +6 dB ≈ ×2 voltage, ×4 power
- +20 dB = ×10 voltage, ×100 power
- 0 dB = unity (no gain or loss)
Practical Examples
The standard cutoff frequency of any filter — output is at half power and 70.7% of input voltage.
Voltage ratio: 0.707×, Power ratio: 0.5×
A −20 dB attenuator reduces signal amplitude by exactly 10× — essential in RF and measurement setups.
Voltage ratio: 0.1×, Power ratio: 0.01×
+6 dB is the gain of a simple non-inverting op-amp with equal feedback and input resistors (gain = 2).
Voltage ratio: 2.0×, Power ratio: 4.0×
10·log vs 20·log — the one thing everyone trips over
This is the question that brings most people to a dB calculator. Power ratios use 10·log₁₀(P₂/P₁). Voltage and amplitude ratios use 20·log₁₀(V₂/V₁). The factor of 20 isn't arbitrary: power goes as voltage squared, and log(V²) = 2·log(V), so squaring inside the log pulls a 2 out front and turns the 10 into a 20.
The consequence is the part people get wrong. +6 dB is roughly ×2 in voltage but ×4 in power. +3 dB is ×2 in power but only ×1.41 in voltage. If you ever mix the two up you'll be off by a factor of two in dB — it's the single most common dB mistake there is. Use 20·log when you're measuring a signal with a scope or talking about gain; use 10·log when you're dealing with watts.
Why voltage uses 20 and power uses 10
Power: dB = 10·log₁₀(P₂/P₁)
Voltage: dB = 20·log₁₀(V₂/V₁) (because P ∝ V²)A non-inverting amp with Av = 10. Express it in dB.
20·log₁₀(10) = 20 dB
Output power drops to 50% — the classic filter cutoff condition.
10·log₁₀(0.5) = −3 dB
A power amplifier delivering 100× the input power.
10·log₁₀(100) = 20 dB (same dB number, but it's ×10 in voltage, not ×100)
Absolute dB scales: dBm, dBV, dBu
Regular dB expresses a ratio. Absolute dB scales pin one end of that ratio to a defined reference level:
| Scale | Reference | Used in | Example |
|---|---|---|---|
| dBm | 1 milliwatt (into 50Ω or 600Ω) | RF, telecom, wireless | +30dBm = 1W transmitter; −100dBm = weak received signal |
| dBW | 1 watt | Broadcast, radar | +10dBW = 10W; 0dBW = 1W = 30dBm |
| dBV | 1 V RMS | Audio, electronics | 0dBV = 1V RMS; −20dBV = 100mV RMS |
| dBu | 0.775 V RMS (1mW into 600Ω) | Professional audio | +4dBu = line level; −10dBu = consumer line level |
| dBFS | Full-scale digital | Digital audio (DAW, ADC) | 0dBFS = maximum sample value; −6dBFS = half amplitude |
| dBi | Isotropic antenna | Antenna gain | +6dBi antenna doubles power vs isotropic in that direction |
Converting between scales requires knowing the impedance. At 50Ω: 0dBm = 224mV RMS = −13dBV ≈ −10.8dBu. At 600Ω: 0dBm = 775mV RMS = 0dBu = −2.2dBV.
Quick dB mental math
A few values are worth memorizing to do instant estimation without a calculator:
| Change | Power | Voltage | How to remember |
|---|---|---|---|
| +3dB | ×2 | ×1.41 | Double power = 3dB |
| +6dB | ×4 | ×2 | Double voltage = 6dB |
| +10dB | ×10 | ×3.16 | One order of magnitude in power |
| +20dB | ×100 | ×10 | One order of magnitude in voltage |
| −3dB | ÷2 | ×0.707 | Filter cutoff point |
| −6dB | ÷4 | ×0.5 | Half voltage |
| −20dB | ÷100 | ÷10 | 10× attenuator |
| −60dB | ÷10⁶ | ÷1000 | Filter stopband rejection (typical) |
These are additive: a +20dB amplifier followed by a −6dB attenuator gives a net +14dB. A +33dB system has +20dB + +10dB + +3dB = ×10 voltage × ×√10 × ×√2 ≈ ×45 voltage gain.
Formula Reference
Decibel (dB) conversion formulas
Power ratio: dB = 10 × log₁₀(P2/P1)
Voltage ratio: dB = 20 × log₁₀(V2/V1)
Current ratio: dB = 20 × log₁₀(I2/I1)
Inverse:
P2/P1 = 10^(dB/10)
V2/V1 = 10^(dB/20)
Reference levels:
dBm: 0 dBm = 1mW into 50Ω → V = 0.224V rms
dBV: 0 dBV = 1V rms
dBu: 0 dBu = 0.775V rms (600Ω reference, audio)
dBFS: 0 dBFS = full scale digitalAdditional Examples
dB = 20 × log₁₀(100) = 20 × 2 = 40 dB. This is a common gain for sensor amplifiers and audio preamps.
Gain: 40 dB
At f₀ of an RC filter: Vout/Vin = 1/√2 = 0.707 → 20×log(0.707) = –3.01dB. Power is halved: 10×log(0.5) = –3.01dB. This defines the –3dB bandwidth.
Voltage ratio: 0.707× · Power ratio: 0.5×
Design tip
–3dB = half power = 0.707× voltage — memorize this.
Every doubling of distance: –6dB (free space), –3 to –6dB (indoor RF).
Audio: human ear perceives +10dB as 'twice as loud' (logarithmic perception).
RF: every 3dB of antenna gain doubles the effective radiated power.Related: convert an amplifier's resistor ratio straight to gain with the op-amp gain calculator, or work in watts with the power calculator. Reference: Decibel (Wikipedia).
Did you know? The decibel was named after Alexander Graham Bell. A 3 dB increase in power corresponds to doubling the power, while a 10 dB increase is a 10× power increase. The human ear perceives a 10 dB increase as roughly twice as loud.