Speaker Systems

The best reproduction of sound is obtained using a different speaker for the low-, mid-, and high-frequency regions. Although Of the three speakers, it is normally the largest. The mid-range speaker is typically smaller in size and covers the range from about 100 Hz to 5 kHz. The tweeter, as it is normally called, is usually the smallest of the three speakers and typically covers the range from about 2 kHz to 25 kHz. There is an overlap of frequencies to ensure that frequencies aren't lost in those regions where the response of one drops off and the other takes over. One popular method for hooking up the three speakers is the crossover configuration of [Fig. 1]. Note that it is nothing more than a parallel network with a speaker in each branch and full applied voltage across each branch. The added elements (inductors and capacitors) were carefully chosen to set the range of response for each speaker. Note that each speaker is labeled with an impedance level and associated frequency. This type of information is typical when purchasing a quality speaker. It immediately identifies the type of speaker and reveals at which frequency it will have its maximum response. For now, however, it should prove interesting to determine the total impedance of each branch at specific frequencies to see if indeed the response of one will far outweigh the response of the other two. Since an amplifier with an output impedance of 8 Ω is to be employed, maximum transfer of power to the speaker will result when the impedance of the branch is equal to or very close to 8 Ω. Let us begin by examining the response of the frequencies to be carried primarily by the mid-range speaker since it represents the greatest portion of the human hearing range. Since the mid-range speaker branch is rated at 8 Ω at 1.4 kHz, let us test the effect of applying 1.4 kHz to all branches of the crossover network.
For the mid-range speaker: and In [Fig. 2(a)], the amplifier with the output impedance of 8 Ω has been applied across the mid-range speaker at a frequency of 1.4 kHz. Since the total reactance offered by the two series reactive elements is so small compared to the 8-Ω resistance of the speaker, we can essentially replace the series combination of the coil and capacitor by a short circuit of 0 Ω. We are then left with a situation where the load impedance is an exact match with the output impedance of the amplifier, and maximum power will be delivered to the speaker. Because of the equal series impedances, each will capture half the applied voltage or 6 V. The power to the speaker is then At a frequency of 1.4 kHz we would expect the woofer and tweeter to have minimum impact on the generated sound. We will now test the validity of this statement by determining the impedance of each branch at 1.4 kHz.
For the woofer: and which is a poor match with the output impedance of the amplifier. The resulting network is shown in Fig. 2(b).
The total load on the source of 12 V is and the current is The power to the 8-Ω speaker is then or about 1 W.
Consequently, the sound generated by the mid-range speaker will far outweigh the response of the woofer (as it should).
For the tweeter: and which, as for the woofer, is a poor match with the output impedance of the amplifier. The current The power to the 8 Ω speaker is then or about 1.3 W.
Consequently, the sound generated by the mid-range speaker will far outweigh the response of the tweeter also.
All in all, the mid-range speaker predominates at a frequency of1.4 kHz for the crossover network of [Fig. 1].
Just for interest sake, let us now determine the impedance of the tweeter at 20 kHz and the impact of the woofer at this frequency. For the tweeter: with Even though the magnitude of the impedance of the branch is not exactly 8 Ω, it is very close, and the speaker will receive a high level of power (actually 4.43 W).
For the woofer: with which is a terrible match with the output impedance of the amplifier. Therefore, the speaker will receive a very low level of power ($6.69 mW = 0.007 W$). For all the calculations, note that the capacitive elements predominate at low frequencies, and the inductive elements at high frequencies. For the low frequencies, the reactance of the coil will be quite small, permitting a full transfer of power to the speaker. For the high-frequency tweeter, the reactance of the capacitor is quite small, providing a direct path for power flow to the speaker.