Добавлен: 03.02.2019

Просмотров: 17272

Скачиваний: 51

ВНИМАНИЕ! Если данный файл нарушает Ваши авторские права, то обязательно сообщите нам.
background image

The design shown in Figure 6–9 resembles a cardioid pattern with a

slightly narrowed contour; its response at 

90 is 12 dB, as compared

to 

6 dB for a first-order cardioid. The physical circuit is shown at A,

and the actual realization is shown at B. Polar plots, both linear and log,
are shown at C.

THE MICROPHONE BOOK

98

FIGURE 6–7

Section view of an 
acoustic lens directional
microphone.

FIGURE 6–6

Details of a parabolic
microphone; section 
view (A); polar response (B);
directivity versus 
frequency (C).

Earg_06.qxd  14/9/04  2:42 PM  Page 98


background image

The design shown in Figure 6–10 resembles a figure-8 pattern with

a slightly narrowed contour, and its response at 

45 is 6 dB, as com-

pared to 

3 dB for the first-order figure-8 pattern. The physical circuit

is shown at A, and the actual realization is shown at B. Polar plots, both
linear and log, are shown at C.

VARIATIONS IN SECOND-ORDER DESIGN

The design of higher-order microphones can be simplified to some degree
by sharing of elements, as shown in Figure 6–11. Here, the two sections
making up the second-order design consist of elements one and two, and
elements two and three. Element two is shared between both sections. In
general, this approach provides a closer overall spacing between ele-
ments of the microphone. Here, note that distance is the same for both
gradient values.

Another design option is to limit the HF range of second-order

action, and letting normal HF pattern narrowing to take over at higher
frequencies, as shown in Figure 6–12. Here, a pair of cardioid elements
are connected for second-order operation up to about 7 kHz. Above that

6: High Directionality Microphones

99

FIGURE 6–8

Principle of the 
second-order microphone;
physical circuit of a 
first-order cardioid 
microphone (A); physical
circuit for a second-order
cardioid (B); polar patterns
for the microphone shown
in B (C).

Earg_06.qxd  14/9/04  2:42 PM  Page 99


background image

frequency the contribution of the rear element is limited, and the front
element’s increasing directivity is allowed to take over response in the
upper octave. The baffle surrounding the front element can be sized and
shaped to optimize the transition from second-order response to beam-
ing first-order response. Above about 12 kHz, the increased beaming of
the front element can be ignored.

THE ZOOM MICROPHONE

The microphone shown in Figure 6–13 is intended to be used with a
handheld video camera with a zoom lens. The microphone “zooms”
electronically in synchronism with the lens system. The microphone
array consists of three first-order cardioid elements whose outputs are
combined in several ways to produce three distinct patterns, including
the intervening patterns. The three primary patterns are:

1. Wide angle: omnidirectional pickup (sum of elements 2 and 3). It is

produced when potentiometers R

1

and R

2

are in position 1.

THE MICROPHONE BOOK

100

FIGURE 6–9

Design data for the 
second-order microphone,
  (0.5  0.5
cos

)(0.5  0.5cos ): 

physical circuit (A);
mechanical circuit (B); polar
response (C).

Earg_06.qxd  14/9/04  2:42 PM  Page 100


background image

2. Medium angle: cardioid pickup (element 1 alone). It is produced

when potentiometers R

1

and R

2

are in position 2.

3. Narrow angle: second-order pickup (sum of elements 2 and 3 with

necessary equalization). It is produced when potentiometers R

1

and

R

2

are in position 3.

There is an overall gain shift of 12 dB throughout the microphone’s

operating range to compensate for distance effects.

6: High Directionality Microphones

101

FIGURE 6–10

Design data for the 
second-order microphone,
  cos

2

: physical circuit

(A); mechanical circuit 
(B); polar response (C).

FIGURE 6–11

Second-order microphone
with shared elements.

Earg_06.qxd  14/9/04  2:42 PM  Page 101


background image

A THIRD-ORDER MICROPHONE

The microphone shown in Figure 6–14A has the polar equation
  cos

3

. The resulting directional response is shown at B. Third-order

microphones have been used primarily in noise canceling applications,
where their immunity to distant sound sources is considerable (Beavers
and Brown, 1970).

THE MICROPHONE BOOK

102

FIGURE 6–12

A combination of first- and
second-order microphone
performance.

FIGURE 6–13

Details of a “zoom” 
microphone. (Data after
Ishigaki et al., 1980.)

Earg_06.qxd  14/9/04  2:42 PM  Page 102