Microphones 493
16.1 Introduction
All sound sources have different characteristics; their
waveform varies, their phase characteristics vary, their
dynamic range and attack time vary and their frequency
response varies, just to name a few. No one microphone
will reproduce all of these characteristics equally well.
In fact, each sound source will sound better or more
natural with one type or brand of microphone than all
others. For this reason we have and always will have
many types and brands of microphones.
Microphones are electroacoustic devices that convert
acoustical energy into electrical energy. All micro-
phones have a diaphragm or moving surface that is
excited by the acoustical wave. The corresponding
output is an electrical signal that represents the acous-
tical input.
Microphones fall into two classes: pressure and
velocity. In a pressure microphone the diaphragm has
only one surface exposed to the sound source so the
output corresponds to the instantaneous sound pressure
of the impressed sound waves. A pressure microphone
is a zero-order gradient microphone, and is associated
with omni-directional characteristics.
The second class of microphone is the velocity
microphone, also called a first-order gradient micro-
phone, where the effect of the sound wave is the
difference or gradient between the sound wave that hits
the front and the rear of the diaphragm. The electrical
output corresponds to the instantaneous particle velocity
in the impressed sound wave. Ribbon microphones as
well as pressure microphones that are altered to produce
front-to-back discrimination are of the velocity type.
Microphones are also classified by their pickup
pattern or how they discriminate between the various
directions the sound source comes from, Fig. 16-1.
These classifications are:
- Omnidirectional—pickup is equal in all directions.
- Bidirectional—pickup is equal from the two opposite
directions (180°) apart and zero from the two direc-
tions that are 90° from the first. - Unidirectional—pickup is from one direction only,
the pickup appearing cardioid or heart-shaped.
The air particle relationships of the air particle
displacement, velocity, and acceleration that a micro-
phone sees as a plane wave in the far field, are shown in
Fig. 16-2.
16.2 Pickup Patterns
Microphones are made with single- or multiple-pickup
patterns and are named by the pickup pattern they
employ. The pickup patterns and directional response
characteristics of the various types of microphones are
shown in Fig. 16-1.
Figure 16-1. Performance characteristics of various microphones.
Microphone Omnidirectional Bidirectional Directional Supercardioid Hypercardioid
Directional Response
Characteristics
Voltage output
Random energy
Efficiency (%)
Front response
Back response
Front random response
Total random response
Front random response
Back random response
Equivalent distance
Pickup angle (2 Q
for 3 dB attenuation
Pickup angle (2 Q
for 6 dB attenuation
E = E 0 E = E 0 cos Q E = E^0 (1 + cos Q
E ;
cos Q=E E cos Q
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E =