In the middle-frequency range many approximations usually can be made to simplify the analogous circuit of
Fig. 9.3. Because the drive unit is very small, the mass of the diaphragm and the voice coil
M
MD
is very small. This in turn usually means that the compliance of the suspension
C
MS
is large to keep the resonance frequency low. Also, the conductance of the suspension
G
MS
usually is large, and the reactance
ωC
M1 is small. Hence, in this frequency range, the circuit reduces essentially to that of
Fig. 9.4a, where the conductance behind the diaphragm is
With the area-changing and electromechanical transformers removed, we get
Fig. 9.4b, where ...