Microphones 533
phone to the source distance requires an increase in the
gain of the amplifying system to produce the same
output level. This is accompanied by a decrease in SNR
and an increase in environmental noises including
reverberation and background noise to where the indi-
rect sound may equal the direct sound. The wanted
signal then deteriorates to where it is unusable. Distance
limitations can be overcome by increasing the sensi-
tivity of the microphone, and the effect of reverberation
and noise pickup can be lessened by increasing the
directivity of the pattern. The interference tube micro-
phone has these two desirable qualities.
The DPA 4017 is a supercardioid shotgun micro-
phone. It is 8.3 in (210 mm) long and weighs 2.5 oz
(71 g), making it useful on booms, Fig. 16-92. The polar
pattern is shown in Fig. 16-93.
The difference between interference tube micro-
phones and standard microphones lies in the method of
pickup.
An interference tube is mounted over the diaphragm
and is schematically drawn in Fig. 16-94.
The microphone consists of four parts as shown in
the schematic:
- Interference tube with one frontal and several
lateral inlets covered with fabric or other damping
material.
Figure 16-88. Neumann U-87 microphone. Courtesy
Neumann USA.
Figure 16-89. Neumann U-89 microphone. Courtesy
Neumann USA.
Figure 16-90. Circuit of the Neumann U-87 condenser
microphone with electrically switchable direction
characteristic. Courtesy Neumann USA.
60 V to +60 V
1G 7
8 0
A
DC B
E
+
60 V 0 V +60 V
+
0 V
+60V
1G 7
G
D
1G 7 S
C