This page assumes you know nothing. Every letter, every squiggle used in the decibel note is unpacked below, in the order that lets each one lean on the one before it.
The picture: imagine filling a bucket with water. The total water is energy. How fast the tap runs — litres per second — is power. A trickle over an hour and a gush over a minute can deliver the same water; they differ in power.
Why the topic needs it: a loud sound isn't about total energy, it's about how much energy arrives per second. That "per second" is exactly power. Every P you see in the parent note is measured in watts. See Wave energy and power for where a wave's power comes from.
Recall Quick check
If a source delivers 6 J of sound energy every 2 seconds, what is its power P? ::: P=6/2=3W.
The picture — why we divide power by area: hold your hand up in the rain. The rate of water hitting your whole hand is like power. But whether it feels heavy depends on how that rate is shared across the skin — that's rate per square metre. A big umbrella catches the same rain spread thin; a thimble catches a fierce trickle concentrated.
Why the topic needs it: intensity is power per unit area, so you must be comfortable with dividing by an area before the formula I=P/A means anything.
The picture: the same 3W of sound landing on 1m2 gives I=3W/m2; spread over 6m2 it gives only 0.5W/m2. Same power, different intensity, because the area changed.
Why the topic needs it:I is the quantity the decibel scale measures. Everything downstream is a comparison of one I against another. The energy itself comes from vibrating air; see Sound waves — pressure & displacement for what is actually moving.
Now we need to know how I changes as you walk away from a source. This is where the geometry of a sphere enters.
The picture — why a sphere at all: a tiny "point" source pumps sound out equally in every direction. After a time, that energy sits on the skin of an expanding ball centred on the source. All the source's power P is smeared over that skin.
So the intensity at distance r is
I=4πr2P.
Why the topic needs it: worked example (d) in the parent note walks a speaker from 2m to 8m. You must know I∝1/r2 to find the intensity ratio before touching decibels.
Recall Quick check
A source reads I at 3m. What fraction of I does it read at 9m? ::: distance ×3 ⇒ intensity ÷32=9, so I/9.
The parent note is drowning in numbers like 10−12. Here is what they mean.
The two rules you actually use:
Multiplying adds exponents: 10a×10b=10a+b.
Dividing subtracts them: 10b10a=10a−b.
Why the topic needs it: the threshold intensity is I0=10−12W/m2, and every intensity ratio is a clash of powers of ten. If you can't subtract exponents in your head, the decibel formula stays opaque.
Powers of ten make big numbers; logarithms count them back.
The picture — a ruler where each tick is ×10:
On an ordinary ruler, steps are added (1, 2, 3). On a log ruler, steps are multiplied (1, 10, 100, 1000) yet they land at evenly spaced positions 0, 1, 2, 3. The log reads off that position. This is why a trillion-fold range collapses into a tidy 0-to-12 spread.
Recall Quick check
What is log10(106)? ::: 6 — because 10 to the power 6 gives 106.
The picture:I0=10−12W/m2 is the faintest sound a healthy ear detects — the "zero line" of loudness. Every sound is quoted as a multiple of that baseline, so 0 dB means "equal to the quietest audible sound", not "no sound at all".
Why the topic needs it: the decibel formula
β=10log10(I0I)
feeds the ratioI/I0 into the log. Skip the reference and you'd be taking the log of something with units — meaningless.
Why the topic needs it: the difference rule Δβ=10log10(I2/I1) uses Δ to compare two situations (two distances, two numbers of violins), and every answer is stamped in dB. Recognising Δ as "the gap between" and dB as "the unit of the level" is essential.
Read it top-down: joules build watts, watts and area build intensity; separately, powers of ten build the logarithm; the two streams meet at the decibel.