Compression and Rarefaction
In a longitudinal wave, a compression is a region where particles are squeezed together and a rarefaction is a region where they are spread apart.
Definition
In a longitudinal wave, a compression is a region where the particles are squeezed close together and a rarefaction is a region where they are spread far apart, alternating along the direction of travel much like crests and troughs, except as squeezes and stretches instead of ups and downs, with the distance from one compression to the next equal to one wavelength. Compressions have higher particle density and pressure and rarefactions have lower density and pressure, and sound waves consist of these alternating regions moving through air, water, or solids. They mark the pressure maxima and minima of a longitudinal wave, $\Delta P(x,t) = \Delta P_{\max}\sin(kx - \omega t)$, where $\Delta P_{\max} = B k s_{\max}$ relates pressure amplitude to displacement amplitude through the bulk modulus $B$, the pressure wave leads the displacement wave by $90^\circ$ so particles sit at zero displacement at the center of a compression, and sound intensity is $I = \Delta P_{\max}^2/(2\rho v)$, scaling with the square of pressure amplitude.
Example
When a drum skin pops outward it shoves air molecules together into a compression, and when it snaps back it leaves a rarefaction where the air is thinner; a loudspeaker producing a $500\ \text{Hz}$ tone sends out $500$ compressions per second, and at $343\ \text{m/s}$ successive compressions are $343/500 \approx 0.69\ \text{m}$ apart with a rarefaction halfway between each pair. The threshold of hearing at $1{,}000\ \text{Hz}$ corresponds to $\Delta P_{\max} \approx 2.9 \times 10^{-5}\ \text{Pa}$, about $3 \times 10^{-10}$ of atmospheric pressure, which with $\rho = 1.2\ \text{kg/m}^3$ and $v = 343\ \text{m/s}$ gives an intensity of $(2.9 \times 10^{-5})^2/(2 \times 1.2 \times 343) \approx 1.0 \times 10^{-12}\ \text{W/m}^2$, the standard reference for $0\ \text{dB}$.
Key Insight
A microphone works by feeling these pressure changes: its diaphragm is pushed in by each compression and pulled out by each rarefaction, turning the pattern into an electrical signal. The ear is astonishingly sensitive, since the pressure swing of the faintest audible sound is smaller than the random pressure fluctuations of air molecules hitting the eardrum; evolution tuned hearing right to the edge of thermal noise.