Solution. From
Eq. (9.9) the optimum throat area is
which from
Eq. (9.11) gives a maximum efficiency of
Solution. Then we obtain the efficiency from
Eq. (9.8), which gives
which is still quite good. If we set the depth
d of the front cavity to
d
=
1
mm so that
V
F
≈
dS
D
=
1.32
cm
3, we obtain the high-frequency resonance from
Eq. (9.21), which gives
which is fairly optimal for a flat frequency-response with a smooth roll-off. Finally, from
Eq. (9.13) we obtain the following lower cutoff frequency with an ideal infinite horn:
Of course this is unrealistic in practice as the lower cutoff frequency is more likely to be determined by the characteristics of the horn, which we shall examine in the next section. The full frequency response is plotted in
Fig. 9.5.