10 dB ≈ “twice as loud”
Your ears hear a ~10 dB jump as double loudness even though physical intensity is 10×. Slide the dB input from 70 to 80 to watch watts shoot upward.
Decibels are a log scale. For intensity, L = 10·log₁₀(I / I₀) with I₀ = 1×10⁻¹² W/m². For pressure, L = 20·log₁₀(p / p₀) with p₀ = 20 µPa. In a simple plane wave, these two tie together via the characteristic impedance of air: I ≈ p² / (ρ·c), where ρ is air density and c is sound speed.
From dB → intensity: I = I₀ · 10^(L/10) From intensity → pressure: p = sqrt(I · ρ · c) Approx source power P from intensity I at distance r: I ≈ (Q · P) / (4π r²) → P ≈ I · (4π r²) / Q Where Q is a directivity factor (Q=1 free field, Q=2 half-space, Q=4 quarter-space, or Q=10^(DI/10)).
Real rooms add reflections and standing waves; wind, humidity, and temperature also matter. Treat this as a learning tool for intuition, not a lab instrument.
Comparisons vary by environment and equipment. Always follow local hearing-safety guidance for real decisions.
This tool is educational and not a sound-level meter or medical advice. Follow your local guidance for hearing protection and exposure limits.
Your ears hear a ~10 dB jump as double loudness even though physical intensity is 10×. Slide the dB input from 70 to 80 to watch watts shoot upward.
A raging 110 dB concert might radiate just a few acoustic watts—similar to a tiny lamp. Check the “source power” line to see how small it looks in watts.
Doubling distance cuts intensity about 4× (≈6 dB). Change the distance field from 1 m to 2 m and watch intensity and energy totals drop instantly.
120 dB “ear-splitting” sound has only ~20 Pa RMS pressure—like the weight of a postcard on your hand. Peek at “Pressure RMS” to appreciate that scale.
An hour at 95 dB dumps over 10,000 J/m² onto your ears. Increase the exposure time field and see the “Energy over time” value balloon.