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Updated 00-09-03

Mini Subwoofer
This project has been started in order to try out the principles of
building an active subwoofer. As I would rather make mistakes on a small scale, I decided
to build a small version first using a small 6,5 inch Peerless speaker I once bought on a
sale (thinking it would come in handy one day).
The subwoofer is housed in a 10,5 l sealed cabinet of heavy MFD
plates. The subwoofer uses the small 25 amplifier to power it, and a small electronic
equalizer which extends the output down to 32 Hz.
This is of cause not a "THX ultra" rated subwoofer and it
will not shake the foundation, but it is though suited for many purposes anyway, and is
not smaller than some commercially available types, used for smaller satellite systems.
The circuits and principles shown here can readily be used for
constructing a larger sub-woofer which can deliver the bass foundation of your dreams!
The Woofer
Peerless CSC Series 850116 176 WR 33 90 SD 8 ohm
Technical Specifications:
Znom |
8 ohm |
Sd |
143 cm2 |
Re |
6.1 ohm |
Vas |
28.5 l |
Le |
1.5 mH |
BL |
5.9 N/A |
fs |
36.7 Hz |
Sensitive |
85.5 db |
Qts |
0.59 |
Max Power |
150 W |
Mms |
18.5 g |
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Simulation of the woofer in a 10.5 l sealed enclosure.
As you can see there are usable output down to about 50 Hz which is not too bad but not
good enough to be called a sub-woofer. (Simulation made with PCLoud4).

The parameters for the system is using filling (Rockwool or
Acustilux):
| Vb |
10.5 liter |
| f3 |
55.8 Hz |
| fc |
66.3 Hz |
| Qtc |
0.88 |
| Peak |
0.57 db |
The Bass Equalizers
Equalizer #1
The equalizer used here has been presented by J.E Benson and W.
Marshall Leach Jr. members of AES [1] and dates back to the late 70'th.
Theoretically the overall resonance frequency of the system using a
sealed enclosure and the electronic equalizer can be found by:

Using the figures found by the simulation program we
get a new fc = 44.5 Hz, which is a lot better than without the equalizer. The combined
system will have the of a 4. order Butterworth system (bass reflex) with a 24 db/octave
roll off compared with the sealed systems 12 db/octave roll off.
You can for sure find speakers that are better suited
for this kind of system, but this system is not intended as a main sub for THX system and
an fc of 44.5 Hz is actually not bad at all.
There are no magic here the physical laws still exists,
and the speaker still have to move a lot of air to give a high output at low frequencies.
What we get is the possibility to use a smaller enclosure on the expense of having to use
a larger amplifier! Today this is really not a problem, and you'll see more and more
commercially system like the Sunfire True Sub and systems from Velodyne using a relative
small speaker with extreme stroke capability in very small enclosures, powered by a class
D amplifier of more than 1000 Watt.
Back to our system here we can see that we get an extra
gain at 45 Hz of around 3 db which is really not that much and will not require a colossal
amplifier, so we can still go for the use of the small 25 W amplifier posted on these
pages.
The circuit is based on three opamps configured as two
2. order high pass filters and a modified differential amp.

The components are straight forward to find using the equations
below:







R5 can be freely chosen i.e. 10 kohm

Using the figures fond by the simulation program and choosing R5 to
be 10 k ohm we get the following values (closest 1% values):
| R1 |
4k87 |
C1 |
680 nF |
| R2 |
5k62 |
C2 |
680 nF |
| R3 |
2k05 |
C3 |
680 nF |
| R4 |
14k0 |
C4 |
680 nF |
| R5 |
2k05 |
|
|
| R6 |
2k49 |
|
|
The components can be calculated using this Excel file
download.
A speaker in a sealed box can be simulated in PSpice together with
the bass equalizer. The bass speaker in a sealed enclosure can be simulated as a second
order high pass filter. I have used a Sallen Key configuration for the simulation:

The components can be calculated using the following equations:

Using the Qts and Fc for the Peerless speaker in a 10.5 l box, and
using C = 680 nF gives:
| C5 |
680 nF |
| C6 |
680 nF |
| R7 |
6213 |
| R8 |
2006 |
The components can be calculated using this Excel file
download.
The Spice simulation of the speaker in the sealed box looks quite
the same as was found by the PCLoud simulation tool:

-3 db is at 55,8 Hz exactly as predicted by PCLoud.
The simulation of the whole system can be seen at the figure below:

The red line is the frequency response of the equalizer and the
green line is the result of the whole system (speaker in box + equalizer). -3 db is at 45
Hz as predicted.
The PSpice file for simulating Equalizer #1 can be downloaded
here.
Equalizer #2
In electronics World February 2000 [2] another equalizer was
presented. It only uses one op-amp but has the ability to lower the resonance frequency
almost arbitrary and even when you can also decide on the Q yourself!!! This seams to be a
bit of a wonder circuit.

The circuit has two break frequencies one at Fc and one at Fe. The
circuit can successfully compensate for the peak at Fc caused by a high Qtc. The roll off
under Fe is only of second order as is the case for the sealed box alone. For equalizer
#1
the roll off is of fourth order, the same as for a bass reflex (vented) box. As the roll
off is only of second order the output will still be reasonable at quite low frequencies.
Don't choose the cut off frequency Fe too low, do remember that the physical laws still
works, and a normal 6,5" speaker is not capable of playing 20 Hz tones at crescendo
levels. If you choose a very low cut off frequency you'll not be able to play anything at
a reasonable level, as the speaker will start hitting the back plate with danger of
damaging the speaker and your mood (this doesn't sound good). As a rule of thumb don't
choose the cut off frequency lower than stated in the table below. Of cause there are
speakers which are of the "long throw" types which are capable of quite long
membrane movements (often denoted as Xmax). For such speakers you can choose lower cut off
frequency. No matter what, you can always try it all out, to change the cut off frequency,
is just a matter of changing 9 passive components. It of cause also depends on both the
number of speakers used and the purpose. For a THX system you really want the possibility
of a high output but as a small sub for your computer you don't need much output at all.
| Speaker diameter |
Lowest recommended cut off frequency |
Speaker diameter |
Lowest recommended cut off frequency |
| 6,5" |
40 Hz |
12" |
30Hz |
| 8" |
35 Hz |
15" |
25 Hz |
| 10" |
30 Hz |
18" |
20 Hz |

The components for the second equalizer circuit can be calculated
from the following equations. Decide on the lower 3 db point Fe (we = 2 p Fe), the overall Qe and use Ra as
input (start with 10k ohm).


In practice k must be larger than zero which means


Using standard components the -3 db is at 32,4 Hz (we aimed at
30 Hz) and the gain of the filter at this frequency is 8,9 db (see the the figure above,
the red line is the total system and the green line is the equalizer alone). At 20 Hz the
gain is 12 db.
The components used in the simulation:
| RA1 |
10k |
RC1 |
48k7 |
| RA2 |
10k |
CA |
1uF |
| RB1 |
23k7 |
CB1 |
56nF//5,6nF |
| RB2 |
23k7 |
CB2 |
56nF//5,6nF |
| RC1 |
48k7 |
CC |
180nF |
To get close to the required 62 nF for CB I've used two standard
capacitors in parallel.
The components can be calculated using this Excel file
download.
Choosing the equalizer
Seeing these results and looking at the versatility of this circuit,
I find it hard not choose second equalizer over the first equalizer presented!
For the most "normal" speakers I would choose the second
equalizer for the following reasons:
- The 2. order roll off characteristic is more compliant to the room
response. At lower frequencies the room will act as an natural amplifier. This phenomenon
rolls off with 12 db/octave (second order) toward higher frequencies, so if you choose the
cut off frequency of your sub to match exactly with the room, you would get a flat
response down to almost 0 Hz. This is not so easy as it depends on both the room the
listening position and the position of the speaker in the room.
- The circuit only uses one active component (one opamp) which if you
don't choose very expensive capacitors will make it quit cheap.
- You can choose the cut-off frequency and Q as you like
In some cases I would choose the first equalizer. As an example take
the new Peerless 10" XLS speaker. A speaker specially made for active subwoofer use
in larger systems (in build a bit similar to the speakers used by Sunfire True Sub and
Velodyne). The speaker has an extensive membrane movement capability (Xmax lin = 2,5 cm ~1
inch).
Put this 10" speaker in a 5 l sealed box, use the first
equalizer and get a flat response down to 11 Hz. Bellow 11 Hz the response will fall with
24 db / octave (fourth order), which I would prefer over the 12 db / octave roll off the
second Eq would give, a small protection for all it is worth.
By the way this speaker is more than just interesting, and I'll try
it out as my next subwoofer project. But as it requires a 28 db gain at 20 Hz, it will
require no less than 6300 W to get 100 db output at 20 Hz (not counting in the room
effect)!!!! So a speaker like this will need a little more than my 25 W mini amp!
The circuit used for the mini sub
The input circuit
The input circuit consist of a summing amp to allow a stereo input
to the sub. The input signal can be provided both by a line level from a dedicated
subwoofer output on the preamp or an extra preamp output, or by speaker level taken from
the speaker terminals on the amplifier.
The signal passes a first order high pass filter C1, C2, P1 which
cuts away undesired DC levels on the input. A low pass filter consisting of R3, R4, C3
cuts off frequencies above 10 kHz which is of no use in this construction and would only
bring instability and noise. The summing amp inverts the signal.

The lower cut off frequency can be calculated by:

With the given components this gives a fn = 22,7 Hz. This is ok for
this small speaker but for a larger sub you'll need to get a lower fn using larger C1 and
C2 (2,2uF gives fn = 10,3 Hz).
The low pass filter
From the summing amp the signals goes into a second order low pass
filter, which cuts off frequencies that are handled by the main speakers.
I have chosen a second order filter, as this will match a sealed box
roll off characteristic. If you are using the circuit together with a vented system then
just close the vent (roll a couple of socks and pluck them in the port/vent), this will
give you a sealed box instead.

The filter is the well known Sallen Key filter, for which the
components can be bound by:

Where R1 = R2 = R.
For a Butterworth response Q = 0,707
We would like to be able to shift fc from lets say 30 to 160 Hz with
80 Hz as the center frequency.
With fc = 80 and R1 = R2 = 10k we get C1 = 282,5 nF and C2 = 140,1
nF.
These are not standard but can be obtained by using capacitors in
parallel:
C1 = 100 nF // 150 nF // 33 nF = 282 nF
C2 = 68 nF // 68 nF // 4,7 nF = 140,7 nF
Now by making R variable we can shift Fc. We'll use a 5 k resistor
in series with a 22 k lin potentiometer for R

P2 is used for adjusting the cut-off frequency. By using a 5 kohm
resistor in series with the 22 kohm linear potentiometer the cut-off frequency can be
adjusted between 30 and 160 Hz. By using a linear potentiometer the cut-off scale is
almost logarithmic. On the figure bellow the cut-off frequency has been calculated as a
function of the potentiometer position (blue curve). The purple line equal the logarithm
of the cut-off frequency, for the scale to be logarithmic the line must be linear
(straight). As can be seen this is not far from being true.

If you are using other components you can use the excel sheet for
calculations, just press here to get it.
 |
Using the components shown here, the marking on the
dial should be as follows. You can of cause use more than 5 markings, use the excel sheet
to calculate up to 23 points. |
Phase inverter
The circuit includes a phase inverter, in order to make a better
match with the main speakers that will be placed at a distant from the sub therefore
introducing a delay or phase shift. The phase match is especially important in the cross
over region to get a flat frequency response. The phase inverter is of cause a bit crude
in the sense that only two settings are possible, an adjustable all pass filter would be
far better, but less simple and must therefore wait till another time! You can do a lot in
sense of matching by physically placing the sub in the most optimal way.
Some adjustment must be foreseen!

The circuit for the inverter is straight forward.
Power supply
The equalizer circuit will normally be build in together with the
power amplifier in the sub it self, and the easiest way to power the circuit is of cause
to connect it to the power amplifiers power supply. Op-amps only handles up to 15-18 VDC
and an regulator is therefore necessary, this will also reduce the noise somewhat. The
regulator is build around two transistors and some passive components. It is quite basic,
reducing the number of components, and does not use feed back. We could have used an
integrated circuit such as the LM78xx/LM79xx series but the presented circuit is cheaper
and just as good for this purpose.
R12 and R13 must be calculated to match the input voltage from the
power amp:
To get a stable voltage over the zenner diode we need some thing
like 2 mA running through it so R12 = R13 = (Vin - 10V) / 2 mA
When using the 25 W amp Vin is 25,5 V and R12 and R13 is therefore
7,75 k ohm (~7k87 as 1%).

A simulation of the power supply was conducted, using +-25,5 VDC as
input but with an 2 V AC signal superimposes. The load was put to 500 ohm between Vcc/Vss
and Gnd (which resembles a n output of +-20mA). As can be seen below the signal was
reduced by 62,5 db above 30 Hz for the negative side and by 75,5 db for the positive side.
This is not best possible result, but it's quite respectable and good enough for this
application. Remember that the op-amps are quite insensitive to PSU imposed noise, and the
relative low gain of the circuit together with the relative high input signals (line
level) no hum should be detectable due to the PSU. Better results could be obtained by
using transistors with higher Hfe.

The circuit and part list

Here is a simulation of the whole circuit + the simulation of the
woofer. The resulting system is the orange line V(23). The -3 db points lays at about 33
and 85 Hz, quite close to predicted.

It is seen that the low frequency roll off is of 3. order. This is
because the overall equalizer gives a 2. order roll off but the input capacitor C1/C2
gives an additional 1. order roll off.
Part list
| R1 |
* |
C1 |
1 uF MKT |
IC1 |
TL072*** |
| R2 |
* |
C2 |
1 uF MKT |
IC2 |
TL072*** |
| R3 |
100k |
C3 |
not used |
|
|
| R4 |
100k |
C4 |
68 nF MKT |
T1 |
BD139 |
| R5 |
10k |
C5 |
68 nF MKT |
T2 |
BD140 |
| R6 |
10k |
C6 |
4,7 nF MKT |
|
|
| R7 |
10k |
C7 |
100 nF MKT |
SW1 |
One pole switch |
| R8 |
5k11 |
C8 |
150 nF MKT |
|
|
| R9 |
5k11 |
C9 |
33 nF MKT |
D1 |
10V Zenner |
| R10 |
10k |
C10 |
470 uF E-lyt** |
D2 |
10V Zenner |
| R11 |
1ok |
C11 |
470 uF E-lyt** |
|
|
| R12 |
7k87 |
C12 |
100 uF/16V E-lyt |
P1 |
47k stereo log pot. |
| R13 |
1k |
C13 |
100 uF/16V E-lyt |
P2 |
22k stereo lin pot. |
| R14 |
1k |
|
|
|
|
| R15 |
7k87 |
|
|
|
|
| RA1 |
10k |
CA |
1 uF MKT |
|
|
| RA2 |
10k |
CB1 |
56 + 5,6 nF MKT |
|
|
| RB1 |
23k7 |
CB2 |
56 + 5,6 nF MKT |
|
|
| RB2 |
23k7 |
CC |
180 nF MKT |
|
|
| RC1 |
48k7 |
|
|
|
|
| RC2 |
48k7 |
|
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* R1 and R2 can be calculated when the output power of the connected
power amp is known use the Excel sheet (Input mixer) to find the
needed value. In the case of the 25 W amp R1 = R2 = 133k.
** C10 and C11 must be chosen to withstand the input voltage. With
the 25 W amp chose 35V.
*** A double op-amp has been chosen because there are a lot of types
to choose from (compared to quad or single), if you want to experiment. TL072 is not the
best op-amp but for this use it is a good choice.
To get the Spice simulation file click
here.

Picture of the pcb with components.
The PCB layout is available in post script and HP Laser Jet
compatible printer file (can also be printed on HP Deskjet printers).
When printing the PRN files, just write:
copy "filename".prn lpt1
in a dos command window. This will copy the file to your printer (if
it is connected to lpt1 ..... most likely).
The Enclosure
The enclosure is build with dimensions as a cube. The woofer is
firing downwards, facing a bottom plate instead of the floor itself. The bottom plate
provides protection to the speaker under transport. The enclosure is made of MDF which I
think is both easy to work with (you can have it cut for you at the hardware store) and as
it is quite heavy it also sounds quite good.

The box is glued together, only the bottom plate is fastened with
screws, to allow removal. Make sure the box is completely air tight as this is paramount
in order to make it work as predicted.
Cabinet Part list
| Pieces |
Dimension [cm] |
Thickness [mm] |
Material |
| 3 |
27,5 x 27,5 |
19 |
MDF |
| 2 |
27,5 x 19,3 |
19 |
MDF |
| 2 |
23,7 x 19,3 |
19 |
MDF |
| 4 |
2,5 x 2,5 |
2,5 |
Wood |
Initial Tests
The mini-sub has now been tested, and it has become clear that the
small 6.5" woofer needs more than 25 watt to perform properly. The small amp simply
is not capable of delivering the voltage needed to drive the digraph to the limits. One
should also remember that we have boosted the lowest frequencies by some 12 db's. The
woofer and equalization circuit was tested with a 150 W power amplifier and now the small
woofer was actually capable of quite a lot of bass. A single 6.5" woofer will never
be able to support a THX system but it with a little more power than the 25 W amp it is
capable of supporting a small satellite speaker set.
I think that if the woofer itself was more efficient and maybe
somewhat larger like a 10" woofer, the 25 W amp would actually be quite enough.
This leaves me with the question of getting more power out of the
mini-amp design! I'll get working on that. I think that it could be modified quite easily
to give something like 75 -100 W quite easily, but it would of cause raise the cost as
well, not least for the power supply. ....... stay posted!
References
| Ref. 1 |
J.E Benson: Synthesis of High-Pass Filtered Loudspeaker
Systems, Part 1. JEAS 1979, Volume 27, Number 7/8. W. Marshall
Leach Jr: Active Equalization of Closed-Box Loudspeaker Systems. JEAS 1981, Volume 29,
Number 6. |
| Ref. 2 |
"Adaptable active speaker system" Electronics
World February 2000 (Author not stated!) |
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