Assistive Listening Systems 1549
impedance characteristic and falling loop current will
complement the rising sensitivity characteristic of the
T-coil, Fig. 33-7. Too high an impedance at high
frequencies will result in too low current, producing
poor response and degraded SNR.
A wire size that can handle the required current with
an acceptable heat rise is selected from Table 42-1. The
impedance is then calculated at several frequencies such
as 100 Hz, 1 kHz, and 10 kHz. The following equations
are useful:
(42-4)
where,
L is the inductance in henrys,
r is the radius of the loop in inches,
n is the number of turns,
d is the diameter of the conductor in inches
(this is a simplification of Wheeler’s equation);
and
(42-5)
where,
Z is the loop impedance,
R is the dc resistance of the length of the coil,
f is the frequency of interest,
L is the inductance of the loop from Eq. 42-4.
An example of the calculations required to determine
the impedance of a one turn 20 ft × 20 ft loop of AWG
#20 wire at 1 kHz is
If this is connected to a 1:4 autotransformer, the
amplifier will see 4.84:
Throughout this design procedure there is a certain
amount of approximation involved; for instance, Eq.
42-4 applies to round loops. Error is introduced in
calculating the inductance of a square or rectangular
loop, however, this error is not great enough to seriously
affect the results.
42.2.2.3 Electronic System
The power amplifier is selected that can supply the
required current to the loop. The power required is
determined with the basic equation
(42-6)
The adjustment of the output current is determined
by the equation
(42-7)
An autotransformer or other suitable impedance
matching device is used to match the amplifier to the
loop. In the absence of an impedance meter, the loop dc
resistance may be used for matching to the amplifier
because at the minimum impedance point (low frequen-
cies), the impedance is largely resistive.
A typical loop system diagram is shown in Fig. 42-8.
In very large halls, a delay unit may be required in the
more distant loops in order to avoid excessive time
delays between the loop signal and the acoustic signal.
Equalization is desirable to compensate for any
frequency response irregularities. The equalizer is
adjusted to provide a natural sound quality with a
typical receiver and to insure that power is not trans-
mitted outside the power bandwidth of the receiver.
A compressor is needed to insure that the system
does not produce excessive distortion at high signal
levels, either from clipping the amplifier or from over-
loading the hearing aid T-coil. The compressor should
Figure 42-7. Sensitivity of typical inductive coil. (From
Reference 1.)
Loaded with 2000 7
Open circuit
20
10
0
10
¾
20
30
100 200 500 1 K 2 K 5 K 10 K
dB
Frequency
L
rn^2
13.5
---------- 2.8r
d
= log----------
ZR
2
2 SfL 10
6–
u
2
+=
L^ 10 ftu12 ft^1
2
u
13.5
--------------------------------------------- 2.8 10 ft^ u12 inches
0.03196
= log-----------------------------------------------------
=143 H
Z 80 10.15
1000
©¹§·u-------------
2
2 Su 103 143 uu 10 6–
2
= +
=1.21 :
PI=^2 Z
I E
Z
=---