You may not be familiar with the sonic benefits of open
baffle speakers from direct experience and therefore hesitate to launch into
building the PHOENIX. After all, such project would take a major commitment of
your time and money. Instead, you might want to try first a less costly design,
but something still indicative of what ultimately can be achieved.
A - Open-baffle woofer - PW1
A - Open-baffle woofer - PW1
The woofer cabinet is essentially only a sound barrier between the output from the front and rear radiating 12" drivers. The sketch below shows the cabinet dimensions in inch. Construction materials are not critical. You may want to add mass on top or bottom of the cabinet to reduce its movement, which is caused by the force of the drivers' moving masses. The movement is not critical as long as it is non-resonant, because the radiating surfaces are small and act as dipoles. Also, place the cabinet on felt pads to avoid rattles. Two of these woofers are need, since otherwise output and distortion performance are marginal.
At the opening of the cabinet you can measure a frequency response that has not been affected by dipole cancellation, because the microphone is so close to the source. As you move the microphone away, the response will decrease progressively as frequency goes down and more of the rear output cancels the sound at the microphone. This must be equalized to obtain a flat woofer response.
The woofer is equalized only down to 30 Hz to limit cone
excursion demands. Below 30 Hz and below Fs of the driver the response
ultimately approaches an 18 dB/oct roll-off slope.
The woofer crossover/eq response is obtained from a
passive line level network between preamplifier and power amplifier. The
disadvantages of this solution are 1) a high insertion loss, and 2) the exact
transfer function can only be approximated.
B - Woofer crossover to existing midrange - PXM1
The woofer equalization network above already includes a
100 Hz, 12 dB/oct lowpass filter for the acoustic crossover to the midrange. On
the midrange side a 12 dB/oct acoustic highpass filter is need. There are
3 - Neither of the two cases above apply. You might try a
single capacitor in conjunction with the variable attenuator to form a 6 dB/oct
highpass, if the midrange exhibits already some roll-off at 100 Hz.
C - Mini open-baffle speaker - PMT1
There is a practical limit to the smallest size of an open baffle speaker, if it is expected to reproduce a balanced full range sound spectrum. The PMT1 represents this case. The speaker might be used for a stereo system in a small room or for side and rear speakers in an audio surround setup. I have little experience with home theater, but expect that it would perform especially well as a center speaker, because of its well behaved and wide polar response. The lack of magnetic shielding might be an issue.
The design is a 2-way loudspeaker with a passive crossover between a Vifa P21WO-20-08 woofer and a Vifa D26TG-35-06 soft dome tweeter. I am sure some of you have preferences for different drivers and so you might use this design as a starting point for your own experimentation. An alternative tweeter could be the silk dome D27TG-45-06, but I have observed some variability with the supplied units.
The cabinet design follows the concepts of the PHOENIX main panel. The dimensions are slightly different to reduce size. The hole cutouts and recesses must be adjusted to the Vifa drivers and the gasket materials used.
The on-axis frequency response shows the inevitable dipole roll-off at 6
dB/oct towards low frequencies. To maintain perceived spectral balance the high
end is rolled off slightly to compensate for the low end behavior. It is
possible to use some low frequency equalization, but as this increases the cone
excursions, the 8" driver will sooner begin to distort.
Note, if this speaker will be used with separate woofers, ideally dipole woofers, then you want to avoid the compensatory high frequency roll-off. Use a slightly different midrange/tweeter crossover and add a crossover of your own design for midrange and woofer. This is best accomplished actively, since the woofer already requires active equalization.
Reversal of the tweeter polarity and the ensuing depth of the notch indicate the accurate addition of midrange and tweeter output through the crossover region in normal mode.
The passive crossover is relatively simple, though unusual for the midrange as it corrects for some of the dipole behavior. The 3.3 mH inductor should have low DC resistance (<0.2 ohm). The 48 uF capacitor can be formed by the series connection of two 100 uF electrolytics (Panasonic HF-Series). The terminal impedance has a minimum of 5 ohm between 100 Hz and 200 Hz.
Quick and messy looking crossover. The electrons don't mind as long as the fields don't couple..
The line level equalizer below uses a bridge type network to increase the rate of frequency response change around 200 Hz. This avoids causing a bump in the speaker output response.
The identical frequency response could be obtained with an active network, but since equalization is of questionable value due to cone excursion limitations, I will not present it. The PMT1 speaker should only be used where its somewhat limited output capability is acceptable. There it will show the benefits of the box-less approach, namely open, uncolored and transparent sound reproduction. - Top
D - Main panel with passive crossover to tweeter - PMTM1
This prototype uses the same main
panel as the PHOENIX except for slightly different hole diameters, recesses
and spacing of the spine to accommodate two Vifa P21WO-20-08 and a D27TG-45-06
driver. The crossover between midrange and tweeter is passive to avoid an
additional power amplifier and active line level electronics. The response is
equalized to 50 Hz at the low end with a passive line level network as for the
PMT1 above. No additional woofer is required, if the system is used in small
rooms and at moderate sound levels.
Starting with a measurement of the drivers on the baffle, you notice that the midrange slopes down towards lower frequencies from a peak at 400 Hz. To remove the peak and to move the roll-off an octave lower, the crossover must attenuate the signal seen by the 8" drivers. This in turn requires that the tweeter highpass filter has insertion loss to match its acoustic output level with that of the midrange.
The midrange lowpass filter in the crossover has an unusual topology to correct for the peak and extend the flat region of the response. The dc resistances of the two coils in the lowpass section are included in the resistor values shown.
The necessary electrical driving voltage response is measured across the driver terminals. The slopes of the midrange and tweeter filters are different. The steeper slope for the tweeter provides additional phase shift in the crossover region to delay the electrical signal and to bring the acoustic output in phase with the midrange.
Since the tweeter is mounted forward of the midrange the added electrical delay gives better summation of the two acoustic outputs. The graph below shows the on-axis response. To obtain an idea about the very important off-axis behavior of the PMTM1 review the response curves for the PHOENIX on the System Test page.
The low frequency response can be extended with the same passive line level equalizer network as for the PMT1 speaker above. For a closer look at the corrected response the time data record for the FFT is increased to 120 ms. The resulting frequency response is no longer anechoic and includes reflections from surroundings of the outdoor test site. The ripples in the response are an indication of this and may have been caused by objects as far as 60 feet away.
Equalization with the simple circuit is not completely
effective, because the roll-off is not only due to the 6 dB/oct dipole behavior,
but also due to the low Qts (~0.33) of the 8" drivers at their 30 Hz
resonance. The compound slope is steeper than 6 dB/oct.
The crossover input impedance is greater than 7.5 ohm at all frequencies and an easy load to drive for a solid state power amplifier. The impedance peak at 500 Hz can be leveled with a R-L-C Zobel network at the input of the crossover. Also, a R-C network might be added to terminate the speaker cable into 10 ohm for frequencies above 50 kHz. Otherwise the cable might act as a resonant antenna in the AM frequency band. Strong radio signals applied to the output of the power amplifier can lead to a degradation of sound quality in some circumstances. - Top
E - Crossover/Equalizer for passive dipole woofer
A passive crossover with built-in 6 dB/oct equalization can be approximated with a simple L-C lowpass network. A potential problem is the low impedance that this circuit presents to the power amplifier. A surprising number of amplifiers have difficulty to drive sufficient current into such load. The 10 mH inductor must have very low resistance and a laminated steel core to keep distortion low and avoid saturation.
Used with PHOENIX or H-frame style woofers the XO/EQ can provide frequency extension down to about 40 Hz for the PMTM1. Such fully passive crossover, 3-way open baffle speaker requires a solid-state amplifier capable of delivering at least 75 W into 4 ohm simultaneously to both channels. Active, line-level equalized woofers would require their own amplifiers, but have much less serious power demands. - Top
F - Transition to fully active systems
In addition to the active equalization of the PMTM1
low frequency response, the crossover to the tweeter could be made active.
Further, with an active crossover to the PW1 dipole woofer, the PMTM1 will turn into a lower cost
version of the PHOENIX (FAQ7, FAQ11).
The woofer may be needed to reduce distortion due to large excursions
of the 8" drivers when more bass output level is desired.