534 Chapter 16
- Capsule with the diaphragm and counter elec-
trode(s). - Rear inlet.
- Electronic circuit.
The directional characteristics are based on two
different principles:
- In the low-frequency range, tube microphones be-
have as first-order directional receivers. The tube
in front of the capsule can be considered as an
acoustic element with a compliance due to the en-
closed air volume and a resistance determined by
the lateral holes or slits of the tube. The rear inlet is
designed as an acoustic low-pass filter to achieve
the phase shift for the desired polar pattern (nor-
mally cardioid or supercardioid). - In the high-frequency range, the acoustical proper-
ties of the interference tube determine the polar
patterns. The transition frequency between the two
different directional characteristics depends on the
length of the tube and is given by
(16-26)
where,
fo is the transition frequency,
c is the velocity of sound in air in feet per second or
meters per second,
L is the length of the interference tube in feet or
meters.
Referring to Fig. 16-94, if the tube is exposed to a
planar sound wave, every lateral inlet is the starting point
of a new wave traveling inside the tube toward the
capsule as well as towards the frontal inlet. Apart from
the case of frontal sound incidence, every particular wave
covers a different distance to the capsule and, therefore,
arrives at a different time. Fig. 16-94 shows the delay
Figure 16-91. By using a microphone as shown in Fig.
16-89 and superimposing two cardioid patterns (top row),
directional response patterns (bottom row) can be
obtained. Courtesy Neumann USA.
Figure 16-92. A supercardioid interference tube micro-
phone. Courtesy DPA Microphones, Inc.
Figure 16-93. Directional characteristics and frequency
response of a DPA 4017 microphone. Courtesy DPA
Microphones, Inc.
A. Directional characteristics.
B. Frequency response of switching filters.
C. On and off axis response measured at 60 cm (23.6 in).
Figure 16-94. Schematic of an interference tube micro-
phone.
fo c
2 L
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