Audio Crossover Circuit

1. Field of the Invention

The present invention relates to audio crossover circuits for use with audio speakers, and more particularly to an audio crossover circuit including "fast acting" circuitry for achieving a low-pass crossover slope in excess of 30 dB/octave within one-half octave of the crossover frequency using only four electrical components.

2. Description of the Prior Art

Audio crossover circuits divide audio signals into different frequency bands or ranges for driving two or more speakers in a speaker system. The crossover circuits apportion the frequency spectrum in such a way that each speaker operates in its optimum frequency range and the entire speaker system reproduces sound with a minimum of distortion.

The frequency at which an audio crossover circuit delivers signals to two speakers operating at adjacent frequency ranges is called the crossover frequency. An audio crossover circuit passes a selected frequency range or band of signals to each speaker and attenuates frequencies that are beyond a speaker's crossover frequency. In this way, each speaker reproduces audio signals only in its optimum frequency range and then "rolls off" near the crossover frequency.

The rate at which a crossover circuit attenuates frequencies delivered to a speaker beyond the crossover frequency is called the crossover slope. Crossover slopes are measured in dB of attenuation per octave and are categorized by their magnitude or "steepness".

Audio crossover circuits typically include high-pass and low-pass filter networks having a plurality of capacitors and inductors. The steepness of an audio crossover circuit's crossover slope is primarily determined by the number of capacitors and inductors used. For example, audio crossover circuits having crossover slopes of 6 dB/octave generally have one inductor or capacitor for each filter network. Audio crossover circuits having crossover slopes of 12 dB/octave generally have two inductors or capacitors for each filter network. In general, each additional component adds approximately 6 dB/octave to the crossover slope.

Crossover circuits with steep crossover slopes are desirable for several reasons. For example, crossover circuits with steep crossover slopes attenuate frequencies that are beyond a speaker's effective operating range more rapidly so that the speaker audibly reproduces only audio signals in its optimum frequency range, reducing distortion from signals outside the range. In other words, crossover circuits with steep crossover slopes prevent distortion from too much treble energy being delivered to a low frequency range speaker or woofer and prevent distortion from too much bass energy being delivered to higher frequency range speakers such as mid-range speakers or tweeters.

Another reason audio crossover circuits with steep crossover slopes are desirable is because they allow the operating ranges of the speakers to be extended. Since audio crossover circuits with steep crossover slopes attenuate frequencies that are beyond a speaker's effective operating range rapidly, the "rolloff" point where audio signals delivered to the speaker are attenuated by the crossover circuit can be moved closer to the range limit, thus allowing an individual speaker to operate over a wider range of frequencies.

A further reason audio crossover circuits with steep crossover slopes are desirable is because they reduce or eliminate interference between speakers operating at adjacent frequency ranges. Since frequencies that are beyond a speaker's effective operating range are attenuated rapidly by these crossover circuits, the speakers reproduce audio signals in their optimum frequency ranges only without reproducing signals in the frequency ranges of adjacent speakers. This reduces interference between adjacent speakers.

Applicant has discovered that it is also advantageous to produce an audio crossover circuit that is "fast-acting". Applicant defines "fast acting" as the amount of time that it takes a crossover circuit to reach its maximum crossover slope. Prior art crossover circuits reach their maximum slope in approximately one octave. Applicant has discovered that a crossover circuit that reaches its maximum crossover slope in one half octave improves speaker performance because frequencies outside of the speaker's optimum operating range are attenuated twice as rapidly. Therefore, all the benefits of a steep crossover slope, as discussed above, are doubled.

A "fast acting", steep crossover slope is especially important on the low-pass side of the crossover because a speaker's natural acoustic output typically does not rolloff above the usable frequency range, rather it begins to distort. Conversely, on the high-pass side of the crossover, the natural acoustic output typically rolls off immediately below the usable frequency range, providing the opportunity to naturally augment the crossover slope and speed, and make unnecessary a fast-acting, high slope on the high-pass side. Therefore a cost-effective high-performance crossover design can be achieved by a fast-acting, steep slope on the low-pass side of over 30 dB/octave within one half octave, and using a lower slope, such as 12 dB/octave, on the high-pass side. This asymmetrical circuit design uses the natural rolloff below the crossover frequency to augment both the speed and slope of the speaker output, thus resulting in an effective high-pass slope of the speaker output that is symmetrical with the low-pass speaker output. In addition, this design increases the useful range of each speaker on the high-pass side because the crossover point can be moved closer to the natural rolloff than in prior art symmetrical circuit designs where high-pass and low-pass slopes are the same.

Prior art attempts to produce audio crossover circuits with steep crossover slopes have been limited by competing interests of cost and performance. To produce economical speaker systems, most audio crossover circuits only utilize a few inductors and capacitors that achieve crossover slopes of 24 dB/octave or less, and because of size limitations, the typical crossover slope is 12 dB/octave or less. Additionally, these prior art audio crossover circuits have not addressed the objective of reaching the maximum crossover slope rapidly, and thus don't reach their maximum slope until more than a full octave. As discussed above, such slow-acting crossover circuits with low crossover slopes result in poor speaker performance since frequencies outside of the speaker's optimum operating range are attenuated too slowly and speakers operating at adjacent frequency ranges interfere with one another.

On the other hand, prior art attempts to produce audio crossover circuits with crossover slopes in excess of 24 dB/octave have been impractical due to high costs and excessive weight. To achieve crossover slopes in excess of 24 dB/octave, the accepted practice is to use a combination of five or more inductors and capacitors per filter. These additional electrical components increase the cost and weight of the crossover circuits and thus limit their utility. Moreover, these prior art audio crossover circuits have not addressed the objective of reaching the maximum crossover slopes rapidly, and thus don't reach their maximum slope until more than a full octave.

Another limitation of prior art audio crossover circuits is their size. It is often desirable to have small speakers to meet tight space requirements of many of today's audio systems. Speaker manufacturers' attempts to build smaller and lighter speakers have been somewhat limited by the relatively large size of prior art audio crossover circuits. Prior art audio crossover circuits are large because of the number of components and because the inductors are spaced to reduce electrical and magnetic interference therebetween. The spacing of components fails to take advantage of mutual coupling of inductors and results in a larger crossover circuit.

Accordingly, there is a need for an improved audio crossover circuit that overcomes the limitations of the prior art. More particularly, there is a need for an audio crossover circuit that achieves a low-pass crossover slope in excess of 24 dB/octave without the use of a great number of inductors and/or capacitors. Additionally, there is a need for an audio crossover circuit that reaches its maximum crossover slope in less than an octave of the crossover frequency. Finally, there is a need for an audio crossover circuit that achieves these objectives without requiring a great deal of space within a speaker cabinet.

The present invention overcomes the problems outlined above and provides a distinct advance in the state of the art. More particularly, the present invention provides a fast-acting audio crossover circuit that achieves a low-pass crossover slope in excess of 30 dB/octave within one half octave of its crossover frequency. Furthermore, the low-pass crossover circuit utilizes only four electrical components and the entire circuit fits on a standard 12 dB/octave circuit board.

The preferred audio crossover circuit includes a low-pass filter network operable for passing a selected range of audio signals from an audio signal source to a speaker and for attenuating other frequencies at a rate in excess of 30 dB/octave. Those skilled in the art will appreciate that a plurality of filter networks may be provided for driving a plurality of speakers.

The low-pass filter network includes a pair of inductors and a pair of capacitors. The inductors are electrically coupled in series between the audio signal source and the speaker and are inductively coupled together. The inductors are also electrically connected so that the windings of their coils are reversed with respect to one another so that at any given time current is flowing in opposite directions in the inductor coils.

One of the capacitors is electrically coupled in parallel between the junction of the inductors, and the other capacitor is coupled in parallel between the inductors and the speaker.

As described in more detail in the Detailed Description, the inductors and the capacitors cooperate for passing a selected range or band of frequencies of the audio signals to the speaker and for attenuating other frequencies at a rate in excess of 30 dB/octave. Moreover, the preferred audio crossover circuit reaches its maximum crossover slope within the first half octave of the roll-off point.

By providing a crossover circuit constructed as described above, numerous advantages are realized. For example, by providing a fast-acting audio crossover circuit having a low-pass crossover slope in excess of 30 dB/octave, unwanted frequencies are attenuated more than twice as rapidly as prior art crossovers. Therefore, interference between speakers operating at adjacent frequency ranges is reduced or eliminated. Additionally, the effective operating range of each speaker can be extended, while containing frequencies within the range and reducing distortion.

A more particular advantage of the preferred audio crossover circuit is that it achieves a low-pass crossover slope in excess of 30 dB/octave faster than prior art crossover circuits with only 2 inductors and 2 capacitors. Applicant has discovered that by electrically connecting the inductors in series and inductively coupling the inductors together, low-pass crossover slopes in excess of 30 dB/octave are achieved within the first half octave without the use of additional electrical components.

Finally, by taking advantage of natural coupling of inductors, the present audio crossover circuit fits on a standard 12 dB/octave circuit board, thus reducing the cost, weight and space requirements of the crossover circuit and thereby increasing its utility.

A preferred embodiment of the present invention is described in detail below with reference to the attached drawing figures, wherein:

FIG. 1 is a top view of an audio crossover circuit constructed in accordance with a preferred embodiment of the invention;

FIG. 2 is a detail view of a portion of one filter network of the audio crossover circuit illustrating the placement and winding of the inductors;

FIG. 3 is an electrical schematic diagram of the audio crossover circuit illustrated in FIG. 1;

FIG. 4 is a graph illustrating the amplitude vs. frequency response of prior art audio crossover circuits; and

FIG. 5 is a graph illustrating the amplitude vs. frequency response of the audio crossover circuit of the present invention.

FIG. 1 illustrates audio crossover circuit 10 constructed in accordance with the preferred embodiment of the invention. FIG. 3 illustrates audio crossover circuit 10 in electrical schematic form. Preferred audio crossover circuit 10 receives audio signals from audio signal source 12 for driving a plurality of speakers.

Preferred audio crossover circuit 10 broadly includes first filter network 14 for driving speaker 16, second filter network 18 for driving speaker 20, and third filter network 22 for driving speaker 24. Each filter network is operable for passing a selected range or band of audio signals from audio signal source 12 to its respective speaker and for attenuating other frequencies. Those skilled in the art will appreciate that additional filter networks may be provided for driving additional speakers. As illustrated in FIG. 1, the individual components of filter networks 14, 18 and 22 are preferably mounted to a single housing such as a conventional circuit board 26.

In more detail, audio signal source 12 generates audio signals for delivery to the input terminals of crossover circuit 10 and may include a conventional stereo receiver, amplifier or other audio component. Speakers 16, 20 and 24 receive selected frequency ranges or bands of the audio signals from their respective filter networks and convert the audio signals to acoustic energy.

Speaker 16 is preferably a low frequency "woofer" type speaker that reproduces low-frequency audio signals such as a Model No. 832757, 4-ohm, 6.5" speaker manufactured by Peerless. Speaker 20 is preferably a "mid-range" type speaker that reproduces mid-frequency audio signals such as a Model No. 821385, 8-ohm, 4.5" speaker manufactured by Peerless. Speaker 24 is preferably a "tweeter" type speaker that reproduces high frequency audio signals such as a Model No. T90K, 8-ohm, 30 mm speaker manufactured by Focal.

Those skilled in the art will appreciate that the selection of audio signal source 12 and speakers 16, 20 and 24 is a matter of design choice. Other audio components may be substituted without varying from the scope of the present invention.

First filter network 14 is operable for passing low-frequency range audio signals from audio signal source 12 to speaker 16 and for attenuating other frequencies. First filter network 14 includes inductors L1 and L2 and capacitors C1 and C2.

Inductors L1 and L2 are electrically coupled in series between audio signal source 12 and speaker 16. As illustrated in FIGS. 1 and 2, inductors L1 and L2 are inductively coupled together by stacking one inductor on top of the other and are electrically connected so that current is flowing in their coils in opposite directions at any given time (see FIG. 2). Alternatively, the two inductors may be wound together rather than stacked. Inductors L1 and L2 preferably have values of 1.9 mH and 1.0 mH, respectively.

As described in more detail below, it has been discovered that by electrically connecting inductors L1 and L2 in series, inductively coupling the inductors together, and reversing the flow of current in the coils of the inductors, low-pass crossover slopes in excess of 30 dB/octave are achieved within the first half octave without the use of additional components. This reduces the cost, weight and space requirements of crossover circuit 10 and thereby increases its utility.

Capacitor C1 is electrically coupled in parallel between the junction of inductors L1 and L2. Capacitor C2 is coupled in parallel between inductor L2 and speaker 16. Capacitors C1 and C2 preferably have values of 100 uF and 33 uF, respectively.

Inductors L1 and L2 and capacitors C1 and C2 cooperate for passing low frequency range frequencies of the audio signals to speaker 16 and for attenuating other frequencies at a rate in excess of 30 dB/octave within one half octave. Filter network 14 as described above has a low-pass crossover frequency of approximately 460 Hz. Those skilled in the art will appreciate that the crossover frequency can be varied by selecting different values for L1, L2, C1, and C2 using standard 24 dB/octave solutions.

Second filter network 18 is operable for passing mid-frequency range audio signals from audio signal source 12 to speaker 20 and for attenuating both low range frequencies and high range frequencies. Second filter network 18 includes a high-pass filter made up by inductor L3 and capacitor C3, and a low-pass filter made up by inductors L4 and L5 and capacitors C4 and C5.

To make up the high-pass filter portion of second filter network 18, inductor L3 is electrically coupled in parallel with audio source 12 and preferably has a value of about 1.5 mH. Capacitor C3 is electrically coupled in series with audio source 12 and preferably has a value of about 80 mF. Inductor L3 and capacitor C3 cooperate for passing mid-range and above frequencies of the audio signals to speaker 20 and for attenuating other frequencies. The preferred second filter network 18 has a high-pass crossover frequency equal to the low-pass crossover frequency of first filter network 14, which is approximately 460 Hz.

To make up the low-pass filter portion of second filter network 18, inductors L4 and L5 are electrically coupled in series between audio signal source 12 and speaker 20. As illustrated in FIG. 1, inductors L4 and L5 are inductively coupled together by stacking one inductor on the top of the other and are electrically connected so that current is flowing in their coils in opposite directions at any given time. Inductors L4 and L5 preferably have values of 0.72 mH and 0.32 mH, respectively.

Capacitor C4 is electrically coupled in parallel between the junction of inductors L4 and L5. Capacitor C5 is coupled in parallel between inductor L5 and speaker 20. Capacitors C4 and C5 preferably have values of 16 uF and 4 uF, respectively. Inductors L4 and L5 and capacitors C4 and C5 cooperate for passing mid-range and below frequencies of the audio signals to speaker 20 and for attenuating high range frequencies. The preferred second filter network has a low-pass crossover frequency of approximately 2100 Hz.

Third filter network 22 is operable for passing high frequency range audio signals from audio signal source 12 to speaker 24 and for attenuating both low and mid-range frequency audio signals. Third filter network includes inductor L6, capacitor C6 and resistors R1 and R2.

Inductor L6 is electrically coupled in parallel with audio signal source 12 and preferably has a value of 0.5 mH. Capacitor C6 is electrically coupled in series with audio signal source 12 and preferably has a value of 12 mF. Inductor L3 and capacitor C3 cooperate for passing high range frequencies of the audio signals to speaker 24 and for attenuating other frequencies. Resistors R1 and R2 are provided for reducing the overall output level of the high-frequency speaker 24. Resistors R1 and R2 preferably have values of about 10 ohm and 30 ohm, respectively. The preferred third filter network 22 has a high-pass crossover frequency of approximately 2100 Hz.

In operation, filter networks 14, 18, and 22 of audio crossover circuit 10 divide audio signals delivered by audio signal source 12 into different frequency bands for driving speakers 16, 20, and 24, respectively. Crossover circuit 10 divides the frequency spectrum among speakers 16, 20, and 24 so that each speaker operates in its optimum frequency range and the speakers together reproduce sound with a minimum of distortion.

The low-pass filter components of audio circuit 10, namely inductors L1 and L2 and capacitors C1 and C2 of first filter network 14, and inductors L4 and L5 and capacitors C4 and C5 of second filter network 18, cooperate for passing selected low frequency bands or ranges of the audio signals to their respective speakers and for attenuating other frequencies at a rate in excess of 30 dB/octave. It has been discovered that by electrically connecting two inductors in series, inductively coupling the inductors together, and reversing the flow of current in the inductors, low-pass crossover slopes in excess of 30 dB/octave within the first half octave are achieved without the use of additional components. This reduces the cost, weight and space requirement of crossover circuit 10 and thereby increases its utility.

First and second filter networks 14 and 18 achieve low-pass crossover slopes in excess of 30 dB/octave within the first half octave because of the cooperation between the series connected and inductively coupled inductors. Below the filter networks' crossover frequencies, the inductors do not significantly cancel or augment each other even though the directions of their windings are reversed. However, above the crossover frequencies, the phase of the signals within the inductors begins to shift, resulting in a cancellation effect because of the reversal of their windings. The cancellation effect increases the low-pass crossover slopes of first and second filter networks 14 and 18 and the speed at which the crossover slopes reach their maximum crossover slope. Applicant has discovered that if the inductors are not connected in series, inductively coupled, and coupled so that their windings are reversed, no cancellation occurs, thus reducing the crossover slope and the speed of the crossover circuit.

The use of less components and the stacking of the inductors also saves space on circuit board 26. The preferred crossover circuit 10 requires a platform measuring only 4" by 7". This allows the entire crossover circuit 10 to fit on a standard 12 dB/octave circuit board.

FIGS. 4 and 5 illustrate the advantages of achieving a steep crossover slope rapidly. FIG. 4 illustrates a prior art crossover circuit having a low-pass crossover slope of 24 dB/octave. The points labeled "a" are the rolloff frequencies of two speakers operating at adjacent frequency slopes. FIG. 5 illustrates the crossover circuit of the present invention, which achieves a low-pass crossover slope of greater than 30 dB/octave within the first half octave. The points labelled "b" are the rolloff points of the same speakers in FIG. 4. On the high-pass side of the crossover, the natural acoustic output typically rolls off immediately below the usable frequency range, providing the opportunity to naturally augment the crossover slope and speed, and make unnecessary a fast-acting, high slope on the high-pass side. Therefore a cost-effective, high-performance crossover design can be achieved by increasing the slope on the low-pass side to over 30 dB/octave within one half octave, and using a lower slope, such as 12 dB/octave, on the high-pass side.

Although the invention has been described with reference to the preferred embodiment illustrated in the attached drawing figures, it is noted that equivalents may be employed and substitutions made herein without departing from the scope of the invention as recited in the claims. For example, four filter networks and three corresponding speakers are illustrated and described for purposes of disclosing a preferred embodiment of the invention. However, as those skilled in the art will appreciate, more or less filter networks and speakers may be provided. Additionally, the low-pass filter portions of the first and second filter network are illustrated and described as including only four electrical components. However, if crossover slopes of greater magnitude are desired, additional electrical components can be added to the filter networks in a conventional manner.