Room modes are the collection of resonances that exist in a room when the room is excited by an acoustic source such as a loudspeaker. Most rooms have their fundamental resonances in the 20 Hz to 200 Hz region, each frequency being related to one or more of the room's dimensions or a divisor thereof. These resonances affect the low-frequency low-mid-frequency response of a sound system in the room and are one of the biggest obstacles to accurate sound reproduction. Discrete room modes dominate only at low frequencies. Above a transition known as the Schroeder frequency, the modes overlap so densely that the room response is better treated statistically than as a set of separated resonances. This frequency is commonly approximated by f ≈ 2000 T / V {\displaystyle f\approx 2000{\sqrt {T/V}}} , where T is the reverberation time in seconds and V is the room volume in cubic metres; for typical rooms it falls in the low hundreds of hertz.
Mechanism of room resonances
The input of acoustic energy to the room at the modal frequencies and multiples thereof causes standing waves. The nodes and antinodes of these standing waves result in the loudness of the particular resonant frequency being different at different locations of the room. These standing waves can be considered a temporary storage of acoustic energy as they take a finite time to build up and a finite time to dissipate once the sound energy source has been removed.
Calculating modal frequencies For a rectangular room with rigid walls, the natural (modal) frequencies are given by
f l , m , n = c 2 ( l L x ) 2 + ( m L y ) 2 + ( n L z ) 2 {\displaystyle f_{l,m,n}={\frac {c}{2}}{\sqrt {\left({\frac {l}{L_{x}}}\right)^{2}+\left({\frac {m}{L_{y}}}\right)^{2}+\left({\frac {n}{L_{z}}}\right)^{2}}}}
where c is the speed of sound, Lx, Ly and Lz are the room dimensions, and l, m and n are non-negative integers (not all zero) that identify the mode. Modes are classified by how many of these integers are non-zero: axial modes involve one pair of opposite surfaces (one non-zero index), tangential modes involve two pairs (two non-zero indices), and oblique modes involve all three pairs (three non-zero indices). Axial modes generally carry the most energy and have the greatest influence on the low-frequency response of a room.
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