Model sound decay from any reference point. Choose spherical, cylindrical, or custom absorption settings here. Get clear dB predictions for outdoor and indoor projects.
This calculator combines geometric spreading, air absorption, and simple extra losses:
L₁ = Lref + DI + CLspread = k · log₁₀(d₂/d₁), where
k=20 (spherical), k=10 (cylindrical), or k=10·n (custom).
Lair = α · (d₂ − d₁)Lextra = Lground + LbarrierL₂ = L₁ − Lspread − Lair − LextraNotes: This is a practical estimator. Complex environments may need frequency-band models or standards-based methods.
Tip: Keep distances consistent, and treat extra losses as conservative if unsure.
| Reference level | Reference distance | Model | Air absorption | Target distance | Predicted level |
|---|---|---|---|---|---|
| 90 dB | 1 m | Spherical | 0.6 dB/km | 10 m | ≈ 70.0 dB |
| 90 dB | 1 m | Spherical | 0.6 dB/km | 50 m | ≈ 56.0 dB |
| 90 dB | 1 m | Spherical | 0.6 dB/km | 100 m | ≈ 49.9 dB |
| 90 dB | 1 m | Spherical | 0.6 dB/km | 200 m | ≈ 43.9 dB |
| 90 dB | 1 m | Spherical | 0.6 dB/km | 500 m | ≈ 35.7 dB |
These examples assume no barrier/ground losses and no corrections.
This tool estimates how sound level (in dB) changes as the receiver moves away from a reference point. It combines geometric spreading, optional air absorption, and simple losses like barriers and ground effects. Use it for planning, comparison, and “what-if” checks when you have a known reference level.
For a point source in free field, spherical spreading predicts about 6 dB drop for each distance doubling (20·log10). A line-like source trends closer to 3 dB per doubling (10·log10). These rules help you confirm whether your inputs and results are in a realistic range.
A common starting point is a measured level at 1 m or 3.28 ft. If you only have a datasheet level at a different distance, enter that distance as the reference. The calculator then scales to any target distance using the chosen spreading model and losses.
Air absorption is entered as α in dB/km or dB/m and is applied over (target − reference) distance. For short runs like 10–100 m, air loss is often small; for hundreds of meters it can become noticeable. Use the presets as rough ranges, then replace with your own verified values.
Directivity index (DI) adds a directional boost when the source aims toward the receiver. A positive DI increases predicted level at distance, while a negative correction can represent unfavorable wind, shielding by geometry, or conservative safety margins. Keep corrections small unless you have strong evidence.
Barrier loss models the insertion loss from a wall, berm, or screen, commonly ranging from a few dB to tens of dB, depending on height and placement. Ground loss is highly site-dependent; treat it as a simplified adjustment that helps compare scenarios rather than an exact acoustics simulation.
Besides predicting level at a distance, you can compute the required source level to meet a target at a receiver location, or solve the maximum distance where a target level is still achieved. These modes help with compliance checks, venue planning, and selecting quieter equipment.
Suppose 90 dB at 1 m with spherical spreading and α=0.6 dB/km. At 50 m, spreading is 20·log10(50/1)=33.98 dB and air loss is 0.6·(49/1000)=0.029 dB, so the estimate is about 56.0 dB before extras. Add a 10 dB barrier and you would expect about 46.0 dB.
No. It is a practical estimator for planning and comparison. For compliance work, use standards-based methods, banded frequency models, and site measurements where required.
Use spherical for point-like sources in open space. Use cylindrical for long, line-like sources. Use custom n when you want to match observed decay between these cases.
Because α is often expressed per kilometer and the tool applies it only over the extra distance beyond the reference. Over 10–100 meters, the air-loss term can be a fraction of a dB.
DI adds a directional gain at the reference level before attenuation. If the source is aimed toward the receiver, DI can increase predicted level; if not, use DI=0 or a conservative correction.
You can approximate near-field decay, but reflections and reverberation can dominate indoors. For rooms, combine distance spreading with room acoustics measures or dedicated reverberation models.
Use measured insertion loss if available. Otherwise, run multiple scenarios (for example 0, 5, 10, 15 dB) to bracket outcomes and choose conservative values for planning.
Use the distance at which your reference level was measured or specified. Many sources use 1 m, but any positive distance works as long as the reference level matches it.