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AUDIO
OUT
AUDIO OUT
L
R
By Jake Rothman
Switching in audio equipment – Part 3
L input
+
100µF
+
I
finished off last month promising to move on to
electronic switching in this month’s Audio Out, and we
will make a small start, but first there are a few odds and
ends to polish off in the mechanical audio switching section.
L output
–
100kΩ
Mono
‘Soft’ bypass
Mono switch
22kΩ
Out
Fig.53. Traditional mono switch circuit.
it cancels out across the left and right channels. In more
sophisticated units, a little bit of gain is introduced via
a proper summing amplifier (Fig.54) to counteract the
attenuation. A typical ‘fudge value’ being +4.5dB.
‘Juggler’ switch
It is sometimes necessary to switch the order of two processing
blocks. A common dilemma facing music engineers is ‘do we
have the EQ followed by the compression or the other way
round?’ It sounds very different depending on which way you
+
100µF
47Ω
22kΩ
Mono
S1a
L output
0V
+
100kΩ
100µF
47Ω
–
5kΩ
22kΩ
Mono gain
0V
100µF
0V
Mono
100µF
S1b
47Ω
+
R input
Stereo
–
+
In
R output
0V
+
In
EQ
620Ω
100kΩ
+
Output
100µF
–
1.5kΩ
Out
+
+
This is an essential test switch for music producers to
listen for phase problems in stereo mixes, accomplished
by mixing the left and right channels. This must be done
using resistors, since it can be dangerous if the left and
right channels are simply joined together. Imagine if there
were two out-of-phase 10Vrms signals from two op amps
(not impossible in audio) and their outputs were joined.
The ‘electronic smell of death’ from burning epoxy would
soon fill the air. The simple resistive summing circuit
shown in Fig.53 leads to a halving of the voltage
level (−6dB) if only one channel has a signal on
L input
it. It remains the same if it’s the same signal on
both channels, say a vocal in the middle of the
mix. This means material in the (stereo) middle
22kΩ
is louder relative to sources panned left or right
when ‘mono-ed’. This is fine for checking mixes,
but if one really does want to listen to stereo
mixes in mono it’s not ideal, and compensating
for this is complex. However Hi-Fi buffs with
old record collections also like a mono button
for playing mono records with a stereo pickup.
This reduces the surface noise because some of
R input
Stereo
0V
+
A ‘soft’ bypass, as opposed to a hard bypass shown in Fig.51
last month, is an arrangement that works well for internal
bypassing in systems where the input is driven from a low
impedance. However, it does not work well for self-contained
units such as guitar pedals where the high-impedance guitar
signal is loaded by the input stage at all times, pulling the
impedance down. A typical place where this is used is in
Hi-Fi preamplifiers to bypass the tone control – see Fig.52.
Input from lowimpedance drive
620Ω
–
R output
Stereo
22kΩ
Bass
Treble
0V
Fig.52. Alternative bypass circuit where the
processor’s input is always connected, such as in
this Hi-Fi preamplifier configuration.
48
Fig.54. Mono switch circuit with a bit of gain tweaking to equalise the
volume difference between mono and stereo.
Practical Electronics | August | 2024
Fig.56. Interior of
an Arcam 65 Plus
amplifier. It used
a microcontroller
employing a
rotary encoder to
accomplish full
remote control.
Too high tech for
me, I couldn’t fix
it. (Lovely Douglas
Self power
amplifier though!)
The thick white
wires are a bypass
‘bodge’ from the
Aux input sockets
to the tone control
inputs.
ended up bypassing the whole selector
section, reducing it to a single-input
computer amplifier.
A real benefit of electronic
switching can be had by removing
easily corrupted small-signal wiring
Electronic switching
connected to mechanical switches at
That’s i t f or me c h a n i c a l a u d io
the front panel and confining it to the
switching; now we can move on to
PCB at the rear. The DC control signals
the important topic of electronic audio
can then go anywhere around the front
switching, which offers the possibility
panel for the most ergonomic layout.
of remote control that has become
This means there is no need to worry
an essential marketing tool today. I
about hum when placing a switch next
don’t rate it that highly as I’m always
to the mains switch.
losing ‘remotes’ and I don’t think a
The simplest and highest quality
sedentary lifestyle is so wonderful. If
way of implementing DC control is
I’m going to select a new source, I see
to use relays, but it is debatable if
no problem in getting up to operate a
this is truly ‘electronic’ – more like
switch. A modern amplifier following
‘electromechanical’. On the other
this tradition is the Arcam 65 Plus
hand, I tend to view relay control as
shown in Fig.56. This design uses a
electronic because it involves electrical
rotary encoder and a microcontroller
control signals. Again, the relays can
to control the electronic switching.
be located at the back and only the
Unfortunately, the micro died in mine
DC control wires need to go to the
and could not be replaced thanks to
front panel switch. Relays are most
proprietary programming/silicon. I
commonly available with
dual change-over contacts
and have to be used in the
special circuit shown in
FX A
S1b
In
Out
Fig.57 to achieve a fourA then B
position input selector. A
S1a
possible problem with this
Input
Output
approach is that the signal
has to go through more than
B then A
FX B
In
Out
one contact. If the relays
S1c
are well-sealed (better still
hermetic) with gold-alloy
contacts then this is not
an issue. Relay control is
Fig.55. A ‘juggler’ switch swaps over the order of two
still the choice in most
circuit blocks. S1 is a 3PDT device. An alternative
top tier Hi-Fi systems and
approach could use a 4053 logic IC or latching relay.
do it. One option is quite a convoluted
circuit called a ‘juggler’ using three
ganged change-over switches (3PDT)
as shown in Fig.55.
Practical Electronics | August | 2024
Input 1
RL1a
Input 2
RL2a
Input 3
RL1b
Input 4
1
2
V+ coil
voltage
0V
1
0V
NC
2
Input
select
3
4
Fig.57. Four input selector switch using
DPDT relays. Duplicate for stereo use.
Suitable relay is Relpol R8M822N,
Rapid 61-6018.
V+
S1
Off
Push to break
NO NC
RL1
S2
On
Push to make
0V
Fig.58. Latching relay circuit.
49
Debouncer section monostable
S1
S1
Push to 100nF
make
1MΩ
–
+
To switch
sections
CD4013a
CD4001a
10nF
D
CD4001b
100kΩ
741
V–
100nF
1.5MΩ
V+
V+
Push to
make
0V
10nF
1MΩ
+5 to 15V
R
S
Q
Output
(inverted)
Q
Output
100kΩ
Output +10V until S1
pressed then –10V
220kΩ
10kΩ
10kΩ
0V
Fig.60. Op amp latching circuit. Avoids the use
of unreliable CMOS chips and give higher output
voltage as well.
100kΩ
4.7kΩ
Low-current
LED, on when
S1 pushed
0V
Fig.59. CMOS switch debouncer and flip-flop. Ideal for controlling 4066
chips. Shown using single-rail supply, but could use a dual-rail supply.
test gear. My Audio Precision analyser takes the number of
relays to extremes, and many can be heard clicking away as
it runs through various test routines. This mechanical noise
is annoying and strangely reassuring at the same time. Relay
coils consume relatively high levels of power at 100mW or
more, and can generate high back voltages when turned off.
It is vital to use clamping diodes, an independent power rail
and an independent earth to avoid clicks and bangs.
Control logic
One of the great advantages of using electronic control is that
latching/maintained switches can be replaced by cheaper
momentary types. Gold-plated contacts are not needed
either since we are dealing with switching DC rather than
low-level signal currents, sometimes called ‘dry switching’.
However, we need to generate a latching action to hold the
selected position. It is possible to use a spare contact on a
relay to do this job (Fig.58), but it is more convenient to use
a latching logic element, such as a flip-flop/bi-stable to do
this. This can be done with standard logic ICs such as the
4013 dual D-type flip-flop. A common problem affecting
counting logic when controlled by mechanical switches is
switch bounce. This can cause erratic operation, such as
jumping a few steps randomly. A monostable made with a
couple of NOR gates makes a good de-bouncer to feed the
flip-flop, as shown in Fig.59. It’s also possible to make a
latch with an op amp using a circuit that appeared
in Elektor Summer Circuits (July 1983) as illustrated
in Fig.60. I have found this arrangement useful since
it can use a standard op amp power supply. It is
also a good use for old spare op amps that are too
noisy for audio, such as 741s. A drawback is the
problem of an uncertain state upon switch-on. One
way round this is to have some kind of capacitive
delay on one side of the bi-stable. Fig.61 shows a
discrete bi-stable used in Boss effects pedals.
Next month
That was a very brief start to electronic audio switching.
Next month, we will dive properly into this important and
fascinating topic.
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470pF
100kΩ
100kΩ
56kΩ
Output
Output
BC549B
1kΩ
470pF
Foot switch
push to
make
10nF
56kΩ
56kΩ
BC549B
470pF
0V
Fig.61. Good old discrete flip-flop; still used in Boss guitar pedals.
50
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Practical Electronics | August | 2024
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