This is only a preview of the January 2014 issue of Silicon Chip. You can view 34 of the 104 pages in the full issue, including the advertisments. For full access, purchase the issue for $10.00 or subscribe for access to the latest issues. Items relevant to "Arduino-Controlled Fuel Injection For Small Engines":
Items relevant to "Bass Extender Mk2 For HiFi Systems":
Items relevant to "PortaPAL-D: A Powerful, Portable PA System, Pt.2":
Items relevant to "Build A LED Party Strobe":
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Bass
Extender Mk2
By NICHOLAS VINEN
. . . gives a big bass improvement for little outlay
Want to get deeper bass out of your loudspeakers? Who doesn’t?
But what if you could get more bass without spending much
money? Even better – this Bass Extender can give as much as an
octave more bass from your speakers! So with good quality tower
speakers, you could get extended bass response down to 20Hz or
below!
A
LL LOUDSPEAKERS have a
rapidly falling response below
a certain frequency which is a basic
limitation of their design. This is firstly
a function of the cabinet design but
is also controlled by the bass driver
characteristics, such as free-air cone
resonance and their Thiele-Small
parameters such as Vas.
Typically, a large good-quality hifi
loudspeaker system will be almost flat
down to somewhere between 30Hz
and 50Hz (the -3dB point or corner frequency) and will slope off below that at
20 Silicon Chip
24dB per octave for a vented enclosure
(ie, a bass reflex system) and 12dB per
octave for a sealed enclosure. Smaller
speakers will have a somewhat higher
corner frequency of, say, 60-80Hz.
While a frequency response extending down to around 40Hz may seem
like a good figure, this means that you
will miss out on the lowest bass octave.
So you will miss out on the lowest
fundamental notes from pianos, pipe
organs, double bass, timpani, tuba –
the list goes on. In fact, life probably
won’t be worth living.
Of course, you will still hear the
harmonics of these notes when they
are played but that will be but a thin
shadow of what could have been.
Seriously though, for a lot of music
which really does explore the lower
music registers, the widest possible
bass response is highly desirable.
As a point of reference, the lowest
note on an 88-key piano (A0) tuned
for A4 at 440Hz has its fundamental at
just 27.5Hz – below the -3dB point of
all but the biggest and most expensive
speakers available!
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Bass Extender response, sealed speaker cabinet, -3dB = 30Hz
Simulated speaker response
beyond cut-off (dB)
+6dB
Filter response (dB)
Overall response (dB)
Phase shift (°)
+3dB
Bass Extender response, vented speaker cabinet, -3dB = 30Hz
Simulated speaker response
beyond cut-off (dB)
+6dB
Filter response (dB)
Overall response (dB)
Phase shift (°)
+3dB
0dB
0dB
-3dB
-3dB
-6dB
-6dB
-9dB
180°
-9dB
180°
-12dB
120°
-12dB
120°
-15dB
60°
-15dB
60°
0°
-18dB
10Hz
-18dB
10Hz
20Hz
30Hz
40Hz
60Hz
80Hz
Fig.1: this plot shows the simulated vented loudspeaker
response near its 30Hz -3dB point (green), the frequency
response of the Bass Extender when it’s active (red) and
the combination of these two (blue). This shows that
with the Bass Extender in place and correctly set up, the
speaker’s frequency response becomes much flatter in
the deep bass region; in this case, from about 50Hz and
below. The phase shift introduced is about 60° at 20Hz.
Now we know that few of our readers can afford such grandiose loudspeakers so our Bass Extender is a very
worthwhile accessory and by the way,
since it has a volume control, it can
also double as a very wide range lowdistortion stereo preamplifier.
Principle of operation
The basic idea is simple – if we
know the characteristics of the lowfrequency roll-off of the speakers, we
can design a filter which increases
signal amplitude right at the frequency
where the speaker’s response is dropping off, thus compensating for this
loss in sensitivity at low frequencies.
That assumes that your amplifier
has sufficient headroom to deliver
more power at these lower frequencies.
Generally, this will be the case unless
some combination of the following is
true: your speakers are very inefficient,
your amplifier has a very low power
output or you play music very loudly.
If you typically run your amplifier with
its volume control below the half-way
point on the volume knob, it’s likely
that you have sufficient headroom for
the Bass Extender.
There is also the issue of “frequency
doubling”. As we increase the drive
level to a speaker operating at or
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20Hz
30Hz
40Hz
60Hz
80Hz
0°
Fig.2: same plot as Fig.1 but with a simulated response
for a loudspeaker in a sealed cabinet, also with a -3dB
point of 30Hz. Its roll-off is not as steep and so the Bass
Extender boost is more gentle. The achieved response
is slightly flatter than for a vented enclosure (assuming
the filter is correctly tuned) but doesn’t extend to quite
as low a frequency. The phase shift is slightly higher
and is nearly 90° at 20Hz.
below resonance (which is usually
a frequency near the -3dB point), its
distortion increases and ultimately,
the second harmonic can overwhelm
the fundamental, leading to an apparent doubling in the frequency being
reproduced. But unless you have small
speakers and drive them very hard,
this is unlikely to be a severe problem.
Ultimately, of course, the Bass Extender cannot turn your little bookshelf
loudspeakers into giant high-fidelity
monsters with 15-inch bass drivers but
it can certainly give you a worthwhile
improvement in bass response.
By the way, because the Bass Extender can run from a 12V DC supply,
it’s also suitable for use in car sound
systems. Mind you, you would then
have to very careful about how much
extra bass boost you apply!
Flattening the response
Fortunately, the bass roll-off of a
loudspeaker can be modelled pretty
accurately, based on two parameters:
its construction (sealed or vented)
and its -3dB point. As Neville Thiele
pointed out in his paper “Loudspeakers In Vented Boxes”, Proceedings of
the IRE Australia, 1961 (reprinted in
Journal of the AES, May & June 1961),
sealed enclosures tend have an ulti-
mate -12dB per octave roll-off while
vented (bass reflex) speakers have an
ultimate slope of -24dB per octave.
Most modern hifi speakers are vented because these tend to have a more
extended bass response. If you are
unsure what type of system you have,
check the front and back of the speaker
for ports; front ports may be hidden
behind a grille. If your speakers have
ports, then they are the vented type.
A -12dB roll-off is the same response
as a second-order low-pass filter while
-24dB matches a fourth-order lowpass filter. These are shown in green
on Figs.1 & 2, with the -3dB point at
30Hz in both instances, typical of a
medium-sized tower speaker.
These figures also show the response
of the filter in the Bass Extender Mk2
(red) when it is tuned to compensate
for these specific speaker responses.
The blue curves show the compensated response of the speakers.
As you can see, the improvement in
flatness is considerable, especially for
vented enclosures, and is now almost
completely flat to 20Hz – the small
dip in the 30-50Hz region being just
0.25dB. This is inevitable, as the Bass
Extender’s boost does not perfectly
cancel out the speaker’s roll-off but it
comes pretty close.
January 2014 21
22 Silicon Chip
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CON1a
FERRITE
BEAD
220pF
6.8k
10k
10k
= SIG GND
220pF
6.8k
LOG
VR1b
10k
LOG
VR1a
10k
47k
10 µF
VOLUME
47k
10 µF
A
K
A
K
C
6.8k*
6.8k
Q2 BC337 *
E
B
B
C
BASS EXTENDER MK2
D2 *
1N4004
D1
1N4004
E
Q1 BC327
S2c
S2b
S2d
S2a
POWER
* THESE COMPONENTS ARE NOT INSTALLED FOR DC SUPPLY
COMPONENT VALUES IN RED BRACKETS ARE FOR DC SUPPLY
47k
10 µF
FERRITE
BEAD
= PWR GND
47k
10 µF
6
5
2
3
–15V
7
1
*220 µF
25V
47k
220 µF
25V
IC1b
IC1: LM833
–15V
4
IC1a
8
S1c
470nF
S1b
470nF
BYPASS
470nF
BYPASS
470nF
OUT
GND
GND
OUT
100 µF *
25V
100 µF *
25V
Y
VR3
2k
10k
X
Y
VR2
2k
X
X
10k
X
A
K
A
K
LED1 IS INSIDE S1 BUTTON
LED2 IS INSIDE S2 BUTTON
REG2 79L15 *
IN
IN
REG1 78L15 *
LINK ONLY FOR DC SUPPLY
100nF
6
5
2
3
(LINK)
D4
1N4004
D3 *
1N4004
Y
Y
8
POWER
A
K
1N4004
K
LED2
λ (S2e)
A
7
3.3k
(3.0k)
2.2k
(1k)
IC2b
1
3.3k
(3.0k)
IC2: LM833
–15V
4
IC2a
S1d
2.2k
2.2k
10 µF
10 µF
B
C
–15V
–Vout
BC 32 7 , BC337
K
BYPASS
–Vin
100Ω
47k
+15V
S1a
LED1
λ (S1e)
A
22k
(10k)
220pF
E
47k
100Ω
LEFT
OUTPUT
CON2a
COM
79L15
0Ω
(10k)
IN
GND
OUT
78L1 5
(100 µF
25V)
NOT INSTALLED
NOT INSTALLED
(10k)
RIGHT
OUTPUT
CON2b
RESISTOR VALUES IN GREEN ARE
FOR SEALED ENCLOSURE SPEAKERS
(USE DEFAULT VALUES FOR VENTED ENCLOSURES)
220pF
–15V
100nF
Fig.3: the circuit includes two identical channels, each consisting of an input buffer stage (IC1a & IC1b) followed by an equal component Sallen-Key filter based
on two 470nF capacitors, resistors X & Y and op amps IC2a & IC2b. Trimpots VR2 & VR3 allow the filter frequency to be adjusted.
SC
20 1 4
CON3
15–17V AC
(12–24V DC)
RIGHT
INPUT
CON1b
LEFT
INPUT
+15V
Similarly, for the sealed enclosure,
the response is now down by less
than 2dB at 20Hz and is virtually flat
down to about 23Hz. Either way, this
is a major improvement for very little
investment.
The reason the cancellation isn’t
quite so good for sealed enclosures is
that we have to reduce the amount of
boost we apply to better match their
more gentle roll-off. Note that in both
cases, the +3dB point of the filter in
the Bass Extender is actually slightly
below the -3dB point of the speaker
response. This gives optimal flatness
and is taken into account in the formulas we give below.
The Bass Extender Mk2 can be set
up to suit sealed or vented speakers
with virtually any corner frequency
simply by selecting a few key resistor
values, as described later. By the way,
simply turning up the bass on the tone
controls on an amplifier won’t do the
same job since that usually involves
boosting frequencies well above the
-3dB point of the speakers, resulting
in a ‘lumpy’ response.
Revised circuit
This design is based on a similar
circuit we published in the April 2005
issue but there are several important
improvements. First, the audio performance is a lot better, partly due to
the use of superior op amps but also
due to more carefully chosen component values. Distortion and noise are
an order of magnitude lower and the
high-frequency distortion especially
has been reduced.
We’ve also fitted it into a more attractive case and provided some externally accessible controls – a volume
knob and a bypass switch. The volume
knob means you can use it with an
amplifier that lacks a volume control
without needing a separate preamp.
The bypass switch makes it easier to
determine just how much effect the
Bass Extender Mk2 has, as you can
easily compare the sound with and
without bass boost.
We have also greatly improved the
headroom. With the original unit running off 12V DC and giving a 10dB
peak boost, it could only just handle
a 2V RMS signal without clipping.
However, some CD/DVD/Blu-ray players or DACs will put out more signal
than that.
By contrast, this new unit runs off a
nominal 15-17V AC plugpack which
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Bass Extender Mk.2 Parts List
1 double-sided PCB, code
01112131, 148 x 80mm
1 ABS plastic instrument case,
155 x 86 x 30mm (Altronics
H0377)
1 15-17VAC plugpack rated <at>
100mA or more
1 set front and rear panel labels
1 10kΩ dual-gang logarithmic
9mm horizontal potentiometer
(VR1)
2 2kΩ mini horizontal trimpots
(VR2,VR3)
1 small knob to suit VR1
1 4PDT yellow illuminated latching pushbutton switch (Altronics S1452) (S1)
1 4PDT green illuminated latching
pushbutton switch (Altronics
S1451) (S2)
2 8-pin DIL IC sockets (optional)
2 stereo side-by-side PCB-mount
RCA sockets (Altronics P0213)
1 PCB-mount DC socket (CON3)
2 ferrite beads
4 No.4 x 6mm self-tapping screws
Semiconductors
2 LM833 dual op amps (IC1,IC2)
1 78L15 +15V regulator (REG1)
means better performance and more
headroom – although we have retained
the option to run it off 12-24V DC,
which might be required if you want
to use it in a car, truck, caravan or boat.
Adjustment trimpots have been added which allow the boost frequency to
be fine-tuned to match the speakers;
the previous version required resistors
to be changed and this wasn’t much
fun if you had to make multiple adjustments until you got the right effect.
Overall then, this new Bass Extender
Mk2 is a much better proposition and
can be added to a hifi system without
degrading the sound quality.
Circuit description
The complete circuit diagram for the
new Bass Extender is shown in Fig.3.
CON1 is the stereo RCA input connector. The two halves of the circuit,
for the left and right channel signals,
are identical so we’ll describe the left
channel only.
A 47kΩ resistor provides ground
bias/loading for the driving equipment, in case this is necessary. The
1 79L15 -15V regulator (REG2)
1 BC327 PNP transistor (Q1)
1 BC337 NPN transistor (Q2)
4 1N4004 1A diodes (D1-D4)
Capacitors
2 220μF 25V electrolytic
2 100μF 25V electrolytic
2 10μF 50V electrolytic
4 10μF 50V non-polarised (NP)
electrolytic
4 470nF MKT
2 100nF multilayer ceramic
4 220pF ceramic disc
Resistors (0.25W, 1%)
7 47kΩ
2 3.3kΩ
1 22kΩ
3 2.2kΩ
4 10kΩ
2 100Ω
4 6.8kΩ
1 0Ω
Plus 8 resistors (X, Y) selected to suit
speaker roll-off; see text & Table 2
Changes For DC Power Supply
(1) Add 3 x 10kΩ and 1 x 1kΩ 0.25W
1% resistors
(2) Add 1 x 100μF 25V capacitor
(2) Delete REG1, REG2, D2-D4 and
several passive components (see
Fig.3)
signal is then AC-coupled via a 10µF
non-polarised (NP) capacitor to an
RC filter consisting of a 6.8kΩ series
resistor with a ferrite bead slipped over
one of its leads and a 220pF ceramic
capacitor to ground. This forms a lowpass filter with a -3dB point of just over
100kHz so that any high-frequency
signals above that do not pass on to
the following stages.
Note that the 10µF AC-coupling
capacitor also forms a high-pass filter
in combination with its load resistance
of around 10kΩ, which gives a -3dB
point of 1.6Hz at the low end.
Following the RF filter, the signal
passes to volume control potentiometer VR1 which is shunted by a 10kΩ
resistor. The reason for this is that a
following filter stage (describe later)
has a gain of 2.5 and this way, with
the volume control set to maximum,
the overall gain through the unit is
1. That’s because the 6.8kΩ RF filter
resistor forms a divider in combination with the 10kΩ pot and its parallel
resistor (ie, 5kΩ) and that gives a gain
of approximately 0.42.
January 2014 23
Filter Resistor Selection
To select the appropriate filter resistor values, first you need to know the -3dB
low-frequency roll-off point for your speakers. Usually, this will be in the specifications (if you can find them!) but you need to be careful as the quoted frequency
response isn’t always measured at the -3dB points; in some cases, manufacturers
use the -6dB points.
If you don’t have this information, you will either have to measure it or guess. To
make this measurement, you will need an adjustable-frequency sinewave generator, an amplifier and an accurate sound level meter (or a calibrated microphone
and AC millivoltmeter). This type of measurement was explained in the “How To
Do Your Own Loudspeaker Measurements” article in the December 2011 issue
of SILICON CHIP.
Basically, what you need to do is measure the sound level at a fixed point in front
of the woofer with a relatively high frequency signal being fed into the amplifier
(eg, 200Hz), then reduce the frequency until you get a reading that is 3dB lower.
You can then use that frequency (Fc) in the formula listed below.
If you have (or can generate) an impedance plot for the speaker, you can also
use this to estimate the -3dB point. For the most common (vented) type, there
will usually be two impedance peaks in the bass region. The -3dB point will be at
the lowest point (dip) between these peaks.
For sealed speakers, there will be a single peak (the resonance frequency)
and the -3dB point will be about 10% below this.
Failing that, use the figures in Table 1 as a rough guide. But we must emphasise that this is only a guide and the actual -3dB point will depend heavily on the
driver and cabinet design and may also vary slightly between different samples
of the same speaker.
Having determined the -3dB point (Fc), use the following formula to determine
the required total resistance (R) for resistors X & Y:
R = T ÷ Fc
where T = 585kΩ for vented enclosures and T = 510kΩ for sealed enclosures.
It’s then just a matter of determining which two series X & Y resistors add up to
give a value that’s close to R.
For example, if Fc = 40Hz then R = 585kΩ ÷ 40 = 14.6kΩ. In this case, you
can select Y = 12kΩ and X = 2.7kΩ (close enough). Or you can use Y = 10kΩ
and X = 4.7kΩ.
Note though that typical 470nF capacitors have a tolerance of ±5% at best so
as long as the total is within a few hundred ohms, that’s good enough. Because
this is a stereo unit, you will need eight resistors in all, four of each selected value.
To save time, we have included Table 2 which shows the best resistor values
to use for common -3dB points. If in doubt as to which values to use, err slightly
on the side of a higher corner frequency as you can later adjust it down slightly
using trimpots VR2 & VR3.
From there, the signal on the wiper
of the volume pot is AC-coupled to
the input of op amp IC1a (LM833) via
another 10µF capacitor. This prevents
IC1a’s input bias current from flowing through the pot and causing a DC
voltage to appear across it. While this
voltage would be small, it could be
enough to cause noise or ‘crackling’
as the pot is rotated.
IC1a buffers the signal and provides
a low driving impedance for the following filter network which consists
of two 470nF capacitors, two identical
pairs of resistors (X & Y) and an adjust24 Silicon Chip
ment trimpot. These resistor pairs have
been used to overcome the limited
range of values available in a single
resistor. As far as the circuit operation
is concerned, you can consider each
series pair as a single resistor.
The signal at the ‘output’ end of
the filter is now fed to pin 3 of IC2a
via switch S1c, which is shown in its
normal operating position. IC2a is set
up as a non-inverting gain stage, with
a gain of 2.5 as mentioned earlier. Its
output goes both to output connector
CON2a and to the junction of the two
470nF capacitors at the output of IC1a
via one of the XY resistor pairs. This is
what gives the filter its characteristic
hump shape (see Fig.1 & Fig.2).
Trimpot VR2 allows the filter response to be tweaked without having
to change component values. This is
necessary because the -3dB point of the
speakers you are using is unlikely to be
exactly the same as the manufacturer’s
specification. Turning VR2 clockwise
increases its resistance and shifts the
filter peak lower in frequency while
increasing its amplitude.
IC2a’s 3.3kΩ feedback resistor is
shunted with a 220pF capacitor which
rolls off its frequency response well
above 20kHz. This lowers its output
noise and improves stability without
impacting on the overall frequency
response in the audio band. The output signal is AC-coupled to CON2a
via a 10µF capacitor to remove any
DC offset picked up in the filter. This
capacitor also ensures that no damage
will occur if the output is shorted to a
DC supply rail.
Finally, the output is DC biased
to ground using a 47kΩ resistor (in
case it’s floating), while a 100Ω series
resistor provides some short-circuit
protection for the op amp and also
isolates IC2a’s output from the load
capacitance (eg, cable capacitance) to
prevent instability.
Note that while we have specified
low-noise, low-distortion LM833 op
amps, others such as the NE5532 and
OPA2134 are also suitable.
Bypass function
When S1c is in its alternative position, IC1’a output is fed directly to
IC2a’s pin 3 input, bypassing the filter
network entirely. This switch thus
provides a bypass function and effectively allows the Bass Extender Mk2
to be disabled so that you can check
whether it is having any audible effect.
S1b provides the bypass function
for the righthand channel. Note that
switch S1 is a 4PDT type – its other
two poles (S1a & S1d) switch on its
integral LED (LED1) when the bypass
function is engaged. This LED is driven
via a 22kΩ current limiting resistor at
around 1.3mA (ie, 28V ÷ 22kΩ).
The 10kΩ resistors connected across
switches S1b & S1c are shorted out
during normal operation. These ensure
that input pins 3 & 5 of IC2 do not go
open circuit when S1 is switched,
preventing loud clicks or pops from
being injected into the audio signal
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and making A/B comparisons with the
Bass Extender enabled and disabled
much easier.
A note about the use of electrolytic
capacitors in the signal chain – we
don’t think that this is a problem
and this is backed up by our measurements. However, we have made
provision on the PCB for 1µF MKT
capacitors to be installed instead of
the 10µF electrolytics for those people
who really want to do so. Besides being
more linear, MKT capacitors also have
a longer lifespan than electros but they
cost more and are harder to get.
Power supply
The recommended power supply
is a 15-17VAC plugpack. The unit
can also be run off 12-24V DC with
reduced headroom but the circuit is
shown configured for an AC supply.
Diodes D1 & D2 form a half-wave
rectifier and charge the 220µF filter capacitors to around ±20V via transistor
switches Q1 & Q2. These ±20V rails are
then regulated to ±15V by 3-terminal
regulators REG1 and REG2, to power
the op amps.
The power switching arrangement
is rather unusual and consists of PNP
transistor Q1, NPN transistor Q2,
switches S2a/S2d & S2b/S2c and two
6.8kΩ base resistors. Basically, the two
transistors are there to carry the supply current and the reason for doing it
this way is that we are using a second
4PDT illuminated switch as the power
switch but these are only rated to carry
50mA per contact.
While that’s sufficient current to run
the unit, the switch-on surge current
is much higher at over 1A while the
input filter capacitors charge. Paralleling the switch contacts doesn’t
help since inevitably, one will make
contact before the others and carry the
full surge current.
So Q1 & Q2 do the actual switching
and this arrangement also limits the
inrush current to around 450mA. The
circuit works as follows: when S2 is
switched to the on position (as shown
in Fig.3), it connects the 6.8kΩ base
resistors for Q1 & Q2 to ground. Thus,
when D1 is forward-biased, Q1’s emitter is at the full positive supply voltage
and its base is pulled towards ground
due to the current flowing through its
6.8kΩ resistor. As a result, PNP transistor Q1 switches on and so current flows
from D1 to the 220µF filter capacitor
across the input of REG1.
siliconchip.com.au
Table 1: Typical Loudspeaker Bass Roll-Off Frequencies
Woofer Size (Approx.)
Cabinet Style
Typical -3dB Point
(Approx.)
>30cm (>12-inch)
Tower
25-30Hz
30cm (12-inch) or 2 x 25cm (10-inch)
Tower
28-35Hz
25cm (10-inch) or 2 x 20cm (8-inch)
Tower
35-40Hz
20cm (8-inch) or 2 x 16cm (6.5-inch)
Tower
40-45Hz
18cm (7-inch) or 2 x 13cm (5-inch)
Tower
45-55Hz
16cm (6.5-inch) or 2 x 13cm (5-inch)
Bookshelf
50-70Hz
13cm (5-inch) or 2 x 10cm (4-inch)
Bookshelf
55-80Hz
10cm (4-inch)
Bookshelf
60-100Hz
Table 2: Resistor Values For Typical -3dB Points
-3db point
Vented Y
Vented X
Sealed Y
Sealed X
28Hz
18kΩ
3kΩ
18kΩ
220Ω
30Hz
18kΩ
1.5kΩ
15kΩ
1.8kΩ
35Hz
15kΩ
1.8kΩ
12kΩ
2.7kΩ
40Hz
12kΩ
2.7kΩ
12kΩ
680Ω
45Hz
12kΩ
1kΩ
10kΩ
1.2kΩ
50Hz
10kΩ
1.8kΩ
10kΩ
220Ω
55Hz
10kΩ
560Ω
8.2kΩ
1kΩ
60Hz
8.2kΩ
1.5Ω
8.2kΩ
270Ω
70Hz
8.2kΩ
150Ω
6.8kΩ
470Ω
80Hz
6.8kΩ
470Ω
4.7kΩ
1.5kΩ
90Hz
4.7kΩ
1.8kΩ
4.7kΩ
1kΩ
100Hz
4.7kΩ
1.2kΩ
4.7kΩ
330Ω
Q2 operates in similar fashion.
When D2 is forward biased, Q2’s emitter is pulled to the negative supply rail
and so this NPN transistor turns on and
current now flows through D2’s anode
and charges the 220µF filter capacitor
at the input of REG2.
In operation, the 6.8kΩ resistors
limit the transistor base currents to
around 20V ÷ 6.8kΩ = 3mA. Since a
BC327/337 has a current gain (hFE) of
about 150 under that condition, this
means that the collector currents are
limited to around 3mA x 150 = 450mA.
If power switch S2 is in the alternative position (ie, off), each 6.8kΩ
base resistor is connected back to the
emitter of its respective transistor.
This effectively ‘shorts’ out the base/
emitter junctions and switches both
transistors off. In this condition, the
only current drawn from the supply is
the leakage current through Q1 & Q2
which is very low (typically <100nA).
The 47kΩ resistor between the two
regulator inputs provides a discharge
path and prevents this leakage current
from (very slowly) charging the input
capacitors.
The power LED (LED2, inside S2)
is connected in series with a 2.2kΩ
current-limiting resistor across the
regulator outputs. Diodes D3 & D4
prevent the regulator outputs from
becoming reverse-biased by more
than about 0.5V during power-up or
power-down.
Note that while you may be able
to get away with using a cheaper and
smaller 12VAC plugpack rather than
the 15-17VAC plugpack specified,
it’s a bit marginal. If using a 12VAC
plugpack, you would want to check
that its actual output under light load
is at least 13VAC (and ideally higher)
in order to prevent the regulators
from entering drop-out. Having said
that, even if they do, the performance
should still be quite acceptable.
DC supply
Note that one 10kΩ resistor and one
January 2014 25
15–17V AC SUPPLY VERSION
VR1
100 µF
S1 Bypass
IC2
LM833
2.2k
3.3k
220pF
220pF
VR2
47k
47k
VR3
2k
100nF
10 µF NP
L
R
CON1
Input
47k
R
6.8k
S2
Power
Q2
D1
D2
Bass Extender Mk.2
C 2013
SILICON
CHIP
100Ω
47k
100Ω
L
A
K
337
2.2k
10 µF
NP
REG2
79L15 220 µF
47k
327
6.8k
4004
Y
220 µF
4004
Y
D4
REG1
78L15
4004
470nF
470nF
Y
2k
220pF
D3
4004
X
100nF
X
Q1
100 µF
22k
A
K
X
Y
47k
47k
NP
10 µF
IC1
LM833
6. 8k
10k
6. 8k
BEAD
10k
X
10k
470nF
+
BEAD
10k
470nF
10 µF
+
NP
+
+
10 µF
10 µF
+
220pF
+
3.3k
2.2k
10k
log
01112131
CON2
Output
CON3
Power
Fig.4: follow this layout diagram to build the PCB if you are going to power the unit from a 15-17V AC
plugpack. Note that there’s provision for the PCB to accept 1μF MKT capacitors instead of the 10μF
electrolytics if you don't want to use electrolytics in the signal chain (and different MKT capacitor sizes
are catered for). Resistors X & Y are selected from Table 2, as described in the “Filter Resistor Selection”
panel.
12–24V DC SUPPLY VERSION
VR1
A
K
X
X
Y
220pF
2.2k
3.3k
220pF
10k
10k
VR3
2k
100nF
3.3k
2.2k
2k
S1 Bypass
47k
CON1
Input
10 µF NP
47k
R
100 µF
47k
1k
D1
SILICON
CHIP
100Ω
47k
L
100Ω
NP
S2
Power
Bass Extender Mk.2
C 2013
10 µF
R
A
K
4004
Y
470nF
470nF
Y
47k
L
327
6.8k
X
Q1
220 µF
100nF
IC1
LM833
220pF
47k
47k
Y
VR2
10 µF
10k
470nF
10k
X
NP
6. 8k
BEAD
10k
470nF
10 µF
10k
6. 8k
BEAD
10k
NP
+
+
10 µF
10 µF
+
220pF
+
IC2
LM833
10k
log
01112131
CON2
Output
CON3
Power
Fig.5: this is the layout diagram to follow if you intend running the unit from a 12-24V DC supply.
The differences between this and the AC-supply version of Fig.4 mainly involve the power supply
components at top right plus the current limiting resistors for LED1 & LED2.
26 Silicon Chip
siliconchip.com.au
100µF capacitor (ie, across the 15V
rail) are not installed when using an
AC plugpack. In addition, one resistor
is specified as 0Ω.
For operation from a 12-24V DC
plugpack (higher being better), the
components marked in red on the
circuit must be changed. First, D4 is
replaced with a wire link, so that the
negative supply rail of the op amps is
now connected to the power supply
ground. Second, the LED currentlimiting resistors are reduced to give
sufficient brightness with the lower
operating voltage. And third, we need
to adjust the DC input bias for all four
op amps so that it will be at half supply; eg, with an 18V supply, it must
be at 9V.
That’s done by fitting two 10kΩ
resistors across the supply rail as a
voltage divider, along with a 100µF
filter capacitor to filter any supply
noise. This capacitor is critical because
without it, any ripple or noise from
the plugpack supply would get into
the audio path. Modern plugpacks are
switchmode devices, so there are often
audible harmonics present.
Finally, when operating from DC,
REG1 is linked out since this gives the
op amps maximum headroom and they
should have sufficient supply ripple
rejection to run from an unregulated
DC rail.
Construction
All the parts for the Bass Extender
Mk2 are mounted on a PCB coded
01112131 and measuring 148 x 80mm.
This fits neatly into an ABS plastic
instrument case measuring 155 x 86
x 30mm and is secured to the integral stand-offs in the case using selftapping screws.
Figs.4 & 5 show the parts layout
on the PCB. Follow Fig.4 if you are
building the AC-powered version.
Alternatively, follow Fig.5 if building
the DC-powered version.
Table 3: Resistor Colour Codes
o
o
o
o
o
o
o
o
o
siliconchip.com.au
No.
7
1
4
4
2
3
2
1
Value
47kΩ
22kΩ
10kΩ
6.8kΩ
3.3kΩ
2.2kΩ
100Ω
0Ω
4-Band Code (1%)
yellow violet orange brown
brown black orange brown
brown black orange brown
blue grey red brown
orange orange red brown
red red red brown
brown black brown brown
single black stripe
Start the assembly by fitting all the
resistors, including the eight selected
for X and Y (see “Filter Resistor Selection” panel and Table 2). Note that the
ferrite beads should be slipped over
the two 6.8kΩ resistor leads before
soldering them in place. It’s a good
idea to check each resistor value using
a DMM before fitting it.
Follow with the diode(s) and then
the two IC sockets. Alternatively, if
you aren’t using sockets, solder the
op amp ICs directly to the PCB. Note
that in either case, the notches/dots
at one end of the sockets/ICs must go
towards the top of the PCB.
The two trimpots can go in next, followed by the transistors and regulators
(if fitted). Note that the transistors and
regulators all look the same so be sure
to check their type numbers carefully
before installing them. You may need
to crank their leads out slightly to fit
the PCB pads.
The six ceramic capacitors are
next on the list, followed by the two
slide switches (S1 & S2). Check that
the latter are sitting flush against the
PCB before soldering their pins (it’s a
good idea to re-check this after lightly
soldering the first two pins). The DC
socket, MKT capacitors and electrolytic capacitors can then all go in.
Take care to ensure that the polarised electros are all orientated correctly. The four non-polarised (NP)
10µF electrolytics can go in either
way around.
The PCB assembly can now be completed by fitting the volume pot and
the stereo RCA sockets. Before fitting
the latter, they need to be modified.
As supplied, they are too tall to fit
Table 4: Capacitor Codes
Value µF Value IEC Code EIA Code
470nF 0.47µF
470n
474
100nF 0.1µF
100n
104
220pF NA
220p
221
5-Band Code (1%)
yellow violet black red brown
brown black black red brown
brown black black red brown
blue grey black brown brown
orange orange black brown brown
red red black brown brown
brown black black black brown
single black stripe
January 2014 27
Left: the PCB assembly
is mounted on the lid of
the case and is secured
to integral stand-offs
using four self-tapping
screws.
Right: rear
view of the
completed unit.
It’s installed
between the
preamp and the
amplifier.
into the case so it’s necessary to cut off
the upper projection with the central
screw hole. This can be done using a
rotary cutting tool or a hacksaw but
make sure you don’t damage the lower
plastic housing. You can then fit the
sockets in place, ensuring that they
are pushed all the way down and are
parallel with the edge of the PCB.
The plastic tabs on either side of the
sockets fit into matching holes in the
PCB to help hold them in place.
Having done that, separate the case
halves by removing the front and rear
panels, then fasten the PCB assembly
to the top half using four No.4 x 6mm
self-tapping screws. This means that
when the case is later assembled, the
PCB hangs upside down off the lid.
first, make sure that both switches are
off (push them until they pop out),
then connect the plugpack supply and
switch on.
Next, use a DMM to check the DC
voltage between pins 4 & 8 of one of the
IC sockets (or between pin 4 & 8 of one
of the ICs); you should get a reading
that’s very close to 0V (ie, with power
switch S2 off).
Now push the power switch and
check that both LEDs illuminate. The
Testing
If you fitted IC sockets, leave the
op amps out of circuit for the time
being. Now for some initial checks:
SILICON
CHIP
BASS EXTENDER MK.2
www.siliconchip.com.au
15VAC
28 Silicon Chip
www.siliconchip.com.au
R
Output
L
R
Input
L
Fig.6: these two
artworks can be
copied and used as
drilling templates
for the front & rear
panels. They can
also be downloaded
as a PDF file from
the SILICON CHIP
website.
siliconchip.com.au
Finishing off
Once you are happy with the results,
you can prepare the front and rear pansiliconchip.com.au
0.01
Bass Extender THD+N vs Frequency, 2V RMS in/out
29/11/13 08:57:54
Left channel, 20Hz-80kHz bandwidth
Right channel, 20Hz-80kHz bandwidth
Left channel, 20Hz-22kHz bandwidth
Right channel, 20Hz-22kHz bandwidth
0.005
Total Harmonic Distortion + Noise (%)
voltage between pins 4 & 8 of the IC
socket (or IC) should now measure 30V
DC for an AC supply, or about the same
as the plugpack output voltage if you
are using a DC supply.
Next, if using an AC supply, connect
the black probe to pin 3 of IC1 and
measure the voltage at pin 8 (+15V)
and pin 4 (-15V). For a DC supply,
check the voltage between pins 3 & 4
of IC1; you should get a reading almost
exactly half that between pins 8 & 4.
Assuming this all checks out OK,
press S1 (Bypass) in and check that
its LED switches off, then switch off
and install the two op amp ICs in
their sockets. That done, connect the
unit between a signal source and your
amplifier (turn the volume down first),
switch on and verify that undistorted
audio is passing through the unit, for
both channels.
You can now check whether the
unit is doing its job, ie, extending
the bass response without introducing any dips or peaks in that region.
If you have a speaker measurement
set-up, as described in the December
2011 issue, then you can run this to
plot the frequency response in the
20-200Hz region to check this. If not,
you will have to do it by ear but that’s
far less precise.
The simplest test would be to run a
sinewave frequency sweep and listen
for any obvious peaks or dips. If there
is a peak present that goes away with
the Bass Extender’s defeat switch
activated, that suggests that you have
the roll-off frequency set too high. In
that case, you can turn trimpots VR2
& VR3 slightly clockwise to decrease
the frequency of the bass boost and
re-test the set-up. If necessary, you can
repeat this procedure until the peak
disappears.
If adjusting VR2/VR3 fails to remove
the peak (even when they are set
fully clockwise), then you will have to
change resistors Y and/or X in order
to decrease the roll-over frequency
further. Note that it’s easier to do this
adjustment one channel at a time.
Conversely, if there’s a dip in the
response, that suggests that the rollover frequency is too low and if VR2/
VR3 are set at minimum (fully anticlockwise), the only option then is to
change resistors Y and/or X.
0.002
0.001
0.0005
0.0002
0.0001
20
50
100
200
500
1k
2k
5k
10k
20k
Frequency (Hz)
Fig.7: total harmonic distortion across the audible frequency range with the
unit operating in typical conditions. This shows that the unit is suitable for
use in a hifi system, with distortion below 0.001% over virtually the entire
frequency range (even with a bandwidth of 80kHz, which is used to show
the slight rise of distortion with frequency). With the bandwidth limited to
a more realistic 20kHz, distortion never rises above 0.00065%.
Features & Specifications
Power supply ............................................................ 15-17VAC or 12-24V DC <at> <100mA
Signal handling ............................................................3.88V RMS (+14dBu) (AC supply)
Frequency response (bypass mode) .......................................... 20Hz-20kHz, +0,-0.06dB
Boost corner frequency .........................................................................+3dB at 20-100Hz
Peak boost ........................................................................................approximately +10dB
Suitable speaker types ........................................................................ bass reflex, sealed
Gain adjustment ...........................................................................................................0-1
Total harmonic distortion .............................................. <0.0005% up to 1kHz (see Fig.7)
Signal-to-noise ratio ......................................................................... -113dB, unweighted
Note: measurements taken with 20Hz-20kHz bandwidth, 2V RMS signal and gain = 1.
els. The labels shown in Fig.6 can be
copied and used as drilling templates
(or they can be downloaded in PDF
format from www.siliconchip.com.au
– free to online subscribers). It’s simply a matter of accurately drilling the
three front panel holes and the five
rear panel holes. That’s best done by
first drilling small holes with a pilot
drill (say 2-3mm) and then carefully
enlarging them with a tapered reamer.
Once drilling is complete, de-burr
the holes and then attach the panel
labels (the labels can be printed onto
photographic paper and attached using silicone). The case lid can then
be fitted in position, the front and
rear panels snapped on and the knob
pushed onto the pot shaft.
You can now hook the unit up permanently. It should ideally go between
your input selector/preamplifier and
power amplifier. If you have an all-inone unit, check if it has preamp-out/
preamp-in connections and if so, use
those. Otherwise you will need to connect it between your most commonly
used signal source (eg, CD player) and
the amplifier.
Finally, it may be possible to build
the unit permanently into your stereo
amplifier and run it from a 15-17VAC
secondary tap on the mains transSC
former.
January 2014 29
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