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If air compression/expansion were isothermal (constant
temperature
), then, according to the ideal gas law
, the
pressure
would simply be proportional to density
. It turns
out, however, that heat diffusion is much slower than audio acoustic
vibrations. As a result, air compression/expansion is much closer to
isentropic (constant entropy
) in normal acoustic
situations. (An isentropic process is also called a reversible
adiabatic process.) This means that when air is compressed by
shrinking its volume
, for example, not only does the pressure
increase (§B.7.3), but the temperature
increases as
well (as quantified in the next section). In a constant-entropy
compression/expansion, temperature changes are not given time to
diffuse away to thermal equilibrium. Instead, they remain largely
frozen in place. Compressing air heats it up, and relaxing the
compression cools it back down.
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