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High-power
Ultrasonic
Cleaner
Part 1
By John Clarke
This large, High-power Ultrasonic Cleaner is ideal for cleaning bulky items
such as mechanical parts and delicate fabrics. It’s also quite easy to build
and is packed with features.
Y
ou’ve probably seen the
small, low-cost ultrasonic cleaners available online. They’re
great for cleaning items like jewellery or
glasses, but what if you want something
a bit bigger and more powerful to suit a
wider variety of cleaning jobs?
Cleaning fuel injectors, an old carburettor or any other intricate part is
a messy and time-consuming task, requiring soaking in harsh solvents such
as petrol, kerosene or a degreaser and
then scrubbing with various brushes to
clean up the parts. It is a difficult and
tedious task, and often does not reach
the small apertures that are usually
the essential areas that need cleaning.
28
Our Ultrasonic Cleaner makes this
task so much easier. Just place the components in a solvent bath, press a button and then come back later to remove
the parts in sparkling clean condition.
It will even clean internal areas! It uses
a high-power piezoelectric transducer
and an ultrasonic driver to release the
dirt and grime with ultrasonic energy.
For more delicate parts, the power
can be reduced to prevent damage to
the items being cleaned.
How does it work?
A metal container is filled with a solvent, deionised water, or normal hot
water and a detergent or wetting agent.
The ultrasonic transducer agitates the
contents of the bath; at higher power
levels, the ultrasonic wavefront causes
cavitation, creating bubbles which
then collapse. This is shown in Fig.1.
As the wavefront passes, normal
pressure is restored, and the bubble
collapses to produce a shockwave.
This shockwave helps to loosen particles from the item being cleaned
(Fig.2). The size of the bubbles is dependent upon the ultrasonic frequency
– the higher the frequency the smaller
the bubble.
We are using the commonly available bolt-clamped Langevin ultrasonic transducer, depicted in Fig.3.
Practical Electronics | September | 2021
Features
Drives a nominal 40kHz, 50W or
60W-rated transducer
Adjustable power level
Power level display
Stop and Start buttons with run
operation indication
Auto-off timer from 20 seconds to
90 minutes
Soft start
Over-current and startup error
shutdown and indication
Power level diagnostics
Automatic or manual transducer
calibration
Standing wave minimisation
Supports a resonance frequency
of 34.88Hz to 45.45kHz
It comprises piezoelectric discs sandwiched between metal electrodes. The
centre bolt not only holds the assembly
together, but is critical in ensuring the
piezo elements are not damaged when
being driven. The bolt is torqued to a
pre-determined tension and locked
(glued) in place to prevent it loosening.
The bolt tension ensures the piezo
discs always remain in compression,
even while it is operating, preventing
the discs from breaking apart.
When a voltage is applied to the piezoelectric discs, forces are generated by
the piezo elements that move the two
metal ends closer together and then further apart at the ultrasonic drive rate.
Our Ultrasonic Cleaner drives the
piezo transducer at close to its nominal
40kHz resonant frequency.
Fig.4 shows the power applied versus
frequency for the particular ultrasonic
transducer we are using. It claims to
have a resonant frequency of 40kHz
with a 1kHz tolerance either side of this
frequency. We found that the transducer
resonates at 38.8kHz under load.
The transducer drive frequency
needs to be controlled to within a
fine tolerance to maintain a consistent power level. A small change in
frequency from the resonant point
will reduce the power quite markedly. Additionally, their impedance
varies depending on load. So when
operating in free air, the impedance
is much lower compared to when the
transducer is driving a bath full of
cleaning fluid.
Circuit details
The circuit of the Ultrasonic Cleaner
is shown in Fig.5. It is based around
a PIC16F1459 microcontroller (IC1).
This controls the two MOSFETs (Q1
and Q2) that drive the primary windings of transformer T1 in an alternating
Practical Electronics | September | 2021
The ‘works’ of our
Ultrasonic Cleaner before
the transducer is attached
to the cleaning bath.
Operation is pretty simple:
turn on, set the timer and
push the ‘start’ button!
fashion. T1 produces a stepped-up
voltage of 100V AC (RMS) to drive the
ultrasonic transducer.
IC1 also drives the power LED
(LED1) and level LEDs (LED2-LED6);
plus it monitors the timer potentiometer (VR1) and switches S2 and S3, used
for starting and manually stopping the
cleaner operation.
IC1 also monitors the current flowing through MOSFETs Q1 and Q2 at
its AN11 analogue input, at pin 12.
And it controls the soft-start charging
of the main bypass capacitor using
transistor Q5 and MOSFET Q6.
Transformer drive
A complementary waveform generator
within IC1 is used to drive MOSFETs
Q1 and Q2 in push-pull mode. The
transformer is centre-tapped to allow
this type of drive. IC1’s PWM generator
includes an adjustable dead time, so
that there is time for one MOSFET to
switch off before the other MOSFET is
switched on (Scope1). This prevents
‘shoot-through’, which would otherwise cause the MOSFETs to overheat.
Fig.1 and Fig.2: the sound waves
produced by the Ultrasonic Cleaner
rapidly create and destroy bubbles
in the liquid. When the bubbles
collapse, they generate localised shockwaves. This ‘cavitation’ stirs up the
solvent layer that’s in contact with the dirt, grease and grime, helping to break
it up and more rapidly dissolve it away. You can do this by hand – it’s called
scrubbing – but it’s a tedious job, and it’s hard to get into nooks, crannies and
internal spaces in the parts being cleaned!
29
Scope1: the gate drive to Q1 (top trace, yellow) and Q2
(bottom trace, cyan) measured at pins 5 and 6 of IC1. The
vertical cursors show the dead time when both MOSFETs
are not driven as 2µs. That is for when Q1 switches off
and Q2 switches on; the dead time is the same between Q2
switching off and Q1 switching on.
IC1’s RC5 and RC4 digital outputs
provide the complementary gate drive
signals for MOSFETs Q1 and Q2. Since
these outputs only swing from 0V to
5V, we are using logic-level MOSFETs.
Standard MOSFETs require gate signals of at least 10V for full conduction,
but logic-level MOSFETs will typically
conduct fully at 4.5V, or sometimes
even lower voltages.
With the STP60NF06L MOSFETs we
are using, the on-resistance (between
drain and source) is 14mΩ at 30A with
a 5V gate voltage. They are rated at 60A
continuous and include over-voltage
transient protection that clamps the
drain-to-source voltage at 60V.
Q1 and Q2 are driven alternately
and these, in turn, drive the separate
halves of the transformer primary of
T1, which has its centre tap connected
to the +12V supply. When MOSFET
Q1 is switched on, current flows in
its section of the transformer primary
winding. Q1 remains on for less than
25µs (assuming a 40kHz operating
frequency) and is then switched off.
Both MOSFETs are off for two
microseconds before Q2 is switched
on. Q2 then draws current through
its section of the T1 primary winding
and remains on for the same duration
as for Q1. Both MOSFETs remain off
again for two microseconds before Q1
is switched on again. The gap when
both MOSFETs are off is the ‘dead
time’ and accounts for the fact that the
MOSFET switch-off takes some time.
Without dead time, the two MOSFETs would both be switched on together for a short duration. This would
cause massive short-circuit current
spikes, not only resulting in overheating of the MOSFETs but also drawing
large current spikes from the supply
filter capacitor and DC power supply.
The alternate switching action
of the MOSFETs generates an AC
Fig.3: this shows the construction of the ultrasonic
transducer that we’re using. Two piezoelectric (ceramic)
discs are sandwiched between the two halves of the body,
with electrodes to allow a voltage to be applied across the
piezo elements. The compression of the piezoceramics
due to the tension from the bolt holding the whole thing
together is critical to preventing early failure from the
ultrasonic vibrations.
30
Scope2: the lower trace (cyan) shows the transformer output
voltage when driving the ultrasonic transducer at 39.26kHz.
The top trace shows the current measurement voltage at the
AN11 input of IC1 (TP1). 4.18V represents a 2.98A current
driving the transformer primary with a 12V supply. This
equates to approximately 35.8W delivered to the transducer.
square wave in the secondary winding of transformer T1. With a turns
ratio of 8.14:1 (57-turn secondary
and 7-turn primary), and 12V AC at
the primary, the secondary winding
delivers about 98V AC to the piezoelectric transducer.
Standing waves
Running the Ultrasonic Cleaner at a
constant frequency near resonance is
efficient, since the impedance of the
transducer is almost purely resistive
under those conditions. However, this
is not ideal for minimising standing
waves within the cleaning bath. Standing waves can build up in strength
while the frequency remains constant.
These waves are caused by reflections from the parts being cleaned and
the tank walls being in-phase. This can
damage delicate parts.
Our Ultrasonic Cleaner has the option of reducing the power for use with
Fig.4: the frequency vs power curve for the transducer in
our prototype. Most transducers with a nominal 40kHz
resonance should be similar, but the exact frequency of
the peak will vary, as will the steepness of the slopes.
Hence, our Ultrasonic Cleaner has an automatic
calibration procedure to find this peak; the 100% power
setting runs it at a frequency close to the peak, while
lower power settings are at higher frequencies.
Practical Electronics | September | 2021
SC HIGH POWER
High-power
Ultrasonic
Cleaner
ULTRASONIC
CLEANER
Fig.5: the complete Ultrasonic Cleaner circuit. IC1 produces complementary drive signals to the gates of MOSFETs Q1
and Q2, which in turn drive the primary of transformer T1 in a push-pull manner. This results in around 100V AC at
CON3. Current is monitored via two 0.1Ω shunt resistors at the sources of Q1 and Q2, via amplifier IC2b into analogue
input AN11 of IC1; the power is computed from this and a voltage measurement at analogue input AN8.
delicate parts, but even larger parts can
have delicate sections within them,
especially in thin-walled cavities.
To avoid standing waves, the frequency can change over time to prevent the constant phase of the waveform, which would cause constructive
interference at various locations in the
bath. As the power versus frequency
graph shows, changing the frequency
even by a small amount will drastically
alter the power. So it is not ideal if the
frequency is varied continuously, as it
reduces the cleaning power.
Instead, we operate the transducer
at a fixed frequency for 10 seconds at
Practical Electronics | September | 2021
a time, then run it over a range of different frequencies for a short time before returning to the maximum power
frequency for another 10-second burst.
In the intervening time, the frequency varies in small 37.5Hz steps
over a 2.4kHz range for around
400ms. That means that power is
reduced only about 4% of the time.
The cycling in frequency alters the
phase of the ultrasonic vibrations
in the bath, giving time for standing
waves that occur during the fixed
frequency period to die down, thus
preventing them from building up to
a damaging level.
Over-current protection
The over-current protection for the
MOSFETs is provided in two ways.
Both of the methods rely on current
detection via the voltage across the
0.1 between the sources of Q1 and
Q2 and ground.
The first method uses NPN transistors Q3 and Q4. These have their baseemitter junctions connected across
those 0.1 current-sense resistors.
Over-current starts when the voltage
across the 0.1 resistor exceeds about
0.5V; ie, with more than 5A through
either Q1 or Q2. The associated transistor Q3 or Q4 then begins to conduct.
31
The current flowing from its collector
to its emitter reduces the gate voltage
to the associated MOSFET. This has
the effect of increasing the MOSFET
on-resistance, which then reduces the
current. This protection is a fast-acting,
cycle-by-cycle protection measure.
At the same time, the voltages across
the two 0.1 current-sense resistors
are averaged by a pair of 10k resistors and filtered by a 100nF capacitor.
This averaged voltage is then applied
to non-inverting input pin 5 of op
amp IC2, which amplifies the signal
28 times ((27k ÷ 1k + 1). The averaging effectively halves the sensed
voltage, since only one of Q1 or Q2 is
on at any given time.
So this results in an overall amplification of 14. The output from pin 7 of
IC2b is measured by the AN11 analogue
input of IC1 (pin 12) – see Scope2.
This voltage is converted to a digital
value and processed by IC1. Should
this voltage stay at 4.9V or more over
a 160ms period, the drive to the transducer is switched off.
This voltage represents an average
of 350mV measured across each 0.1
resistor, or a 3.5A average current flow.
That’s calculated as (4.9V÷14) ÷ 0.1.
An over-current error is indicated
by flashing LED2, LED4 and LED6 on
the front-panel level display. When
this happens, the power will need to
be switched off and restarted to resume
cleaning. If the problem persists, the
cause will need to be found.
Power control
The current measured at the AN11
input is also used for controlling the
power applied to the ultrasonic transducer. The maximum power rating of
the transducer is 50W, but this is not a
continuous rating. The recommended
continuous power is 43W. We limit
power to a more conservative 36W. For
a 12V supply, the current required for
this level of power is 3A.
During operation, the current is monitored via AN11 and the drive voltage is
also sampled, via a resistive divider, at
analogue input AN8 (pin 8). This allows
the micro to calculate the power flowing
into the transformer as the frequency
is adjusted, so that it can maintain the
power at the required level.
IC1’s instruction clock is derived
from its internal oscillator, and thus
the PWM output frequencies are derived from this as well. The internal
oscillator can be adjusted in small
steps using the OSCTUNE register.
This can vary the internal oscillator
frequency over a 12% range in 128
steps. For the 40kHz drive to the ultrasonic transducer, this allows a 4.8kHz
control range in steps of 37.5Hz.
32
levels use a frequency above resonance
that has the transducer producing a
lower power.
Nine power levels are available,
ranging from 100% (36W) down to
10% (about 3.6W). Depending on the
transducer characteristics, the lowest
power level may not be available.
The 40kHz transducer is available
online. Remember that if you do buy
online you need to make sure you
get a 40kHz type – there are other
frequencies available and they look
pretty much identical. (See the NOTES
in the Parts list opposite).
The 37.5Hz-step resolution is sufficiently small to drive the ultrasonic
transducer at the desired power level.
However, the OSCTUNE register does
not have sufficient frequency range
to ensure we can drive an ultrasonic
transducer that is resonant outside the
range of 37.6kHz to 42.4kHz.
To widen the operating range, the
unit calibrates itself automatically
(it can also be initiated manually).
This finds the approximate resonant
frequency of the transducer using a
coarser adjustment. Fine-tuning is
then done via OSCTUNE; this allows
a variety of different transducers to
be used.
This coarser calibration is performed using the PR2 register, which
sets the period and thus the frequency
of the PWM drive waveform. For our
circuit, this provides steps of approximately 540Hz. We restrict the
coarse adjustment range to be from
34.88kHz to 45.45kHz. This range
caters for all transducers that have a
nominal 40kHz resonance.
So the transducer’s resonance is
found to within 540Hz by adjusting
PR2, and this value is stored in nonvolatile Flash memory. OSCTUNE
can then vary the frequency at least
1.8kHz above and 1.8kHz below the
value initially set by the PR2 register
(1.8kHz 2.4kHz − 540Hz).
Different power levels are available
by adjusting the drive frequency. The
highest power is at the frequency closest to resonance, while lower power
LED indicators
LEDs 2-6 indicate which of the nine
power levels is selected, with LED2 lit
to indicate the lowest power level. The
next step up is with LED2 and LED3 lit,
then LED3 and so on until LED6 only
is on, showing the highest power level.
The power level is adjusted by
holding down the Start switch. It
will then cycle up through the nine
possible levels to the maximum, then
down again. The switch can then be
released at the desired level setting.
The transducer is not driven during
power level adjustments.
The On/Run LED (LED1) shows
when power is applied to the circuit.
This LED also acts as an operation indicator. The LED goes out during transducer calibration and then lights when
the required value for PR2 is found.
This takes a few seconds, unless
there is something wrong, such as when
there is no transducer connected.
Once running, LED1 only lights
when the transducer is being driven at
the required power setting; it acts as an
‘in lock’ indicator.
When the Stop switch is pressed, the
drive to the transducer ceases, the level
LEDs go off and the power LED turns
on. LED1 then goes out when the main
power source is switched off via S1, or
if the supply itself is disconnected or
switched off.
Cleaning timer
VR1 is the timer control. The voltage
from its wiper is applied to the AN9
analogue input of IC1 (pin 9), and it
varies between 0V and 5V. This corresponds to a timer range from 20 seconds
through to 90 minutes.
The timer starts when the Start
switch is pressed. After the selected
period, the transducer drive stops.
Switches S2 and S3 connect to the
RA0 and RA1 inputs of IC1 respectively. The inputs are held high (at 5V)
by 10k pull-up resistors. A closed
switch is detected when it is pressed
as the input is pulled to 0V.
Note that we are using pushbutton
changeover switches that have common
(C), normally closed (NC) and normally
open (NO) contacts.
The pins on the switch are in a line,
with the common pin at one end, NO
in the middle and NC at the other end.
Usually, that means that you would
Practical Electronics | September | 2021
Parts list – High-power Ultrasonic Cleaner
1 double-sided PCB coded 04105201, 103.5 x 79mm
1 double-sided PCB coded 04105202, 65 x 47mm
Both PCBs available from the PE PCB Service
1 panel label, 115 x 90mm (see text)
1 diecast aluminium box, 115 x 90 x 55mm (Jaycar HB5042)
1 50/60W 40kHz ultrasonic horn transducer (resonance
impedance 10-20) [see NOTES below]
1 12V DC 60W switchmode supply or similar
[Jaycar GH1379, Altronics MB8939B] OR
1 12V battery (10Ah or greater) with 5A+ rated twin lead
1 EPCOS ETD29 13-pin transformer coil former,
B66359W1013T001 (T1)
[RS Components 125-3669, element14 1422746]
2 EPCOS ETD29 N97 ferrite cores, B66358G0000X197 (T1)
[RS components125-3664, element14 1422745]
2 EPCOS ETD29 clips, B66359S2000X000 or equivalent (T1)
[RS components 125-3668, element14 178507]
1 6A SPST mini rocker switch (S1)
[Altronics S3210, Jaycar SK0984]
2 SPDT momentary push button switches (S2,S3)
[Altronics S1393]
2 switch caps for S2 and S3 [Altronics S1403]
1 5A PCB-mount barrel socket, 2.5mm ID (CON1)
[Jaycar PS0520, Altronics P0621A]
1 5A barrel plug, 5.5mm OD x 2.5mm ID
[Jaycar PP0511, Altronics P0165] (optional)
1 vertical 2-pin pluggable header socket with screw terminals
(CON2) [Jaycar HM3112+HM3122]
1 2-way PCB mount screw terminal with 5.08 spacing (CON3)
[Jaycar HM3130, Altronics P2040A]
1 14 pin box header (CON4) [Altronics P5014]
1 14 pin IDC plug (for CON4) [Altronics P5314]
1 14-pin IDC transition plug (CON5) [Altronics P5162A]
2 3AG PCB-mounting fuse clips (F1)
1 4A 3AG fuse (F1)
1 10k 16mm linear potentiometer (VR1)
1 knob to suit potentiometer
1 20-pin DIL IC socket (for IC1)
1 8-pin DIL IC socket (for IC2)
3 TO-220 silicone washers and bushes
4 stick-on rubber feet
Transducer housing parts
1 50mm length PVC DWV (Drain, Waste and Vent) fittings; end
cap and adaptor or 1 40mm length of 50mm ID pipe
1 cable gland for 3-6.5mm cable
Neutral cure silicone sealant (eg, roof and gutter)
Epoxy resin (eg, JB Weld)
Parts for testing
1 100mm length of 0.7mm tinned copper wire
4 9mm-long M3 tapped spacers
4 M3 x 6mm machine screws
extra length of 0.63mm diameter enamelled copper wire
need to orient the switch correctly on
the PCB for correct operation.
However, we have designed the PCB
pattern so that either orientation will
work by wiring the C and NC connections together on the PCB.
Power supply
12V DC power for the circuit is fed in
via CON1. It needs 4A minimum. If
using a 12V battery, it should be rated
at 10Ah or more. Power is switched
Practical Electronics | September | 2021
Cables, wiring and hardware
1 M3 x 6mm machine screw (for REG1)
3 M3 x 9mm machine screws (for Q1, Q2 and Q6)
4 M3 hex nuts
1 cable gland for 3-6.5mm diameter cable
1 800mm length of 1mm diameter enamelled copper wire
(T1 primary)
1 3.6m length of 0.63mm diameter enamelled copper wire
(T1 secondary)
1 1m length of 0.75mm square area dual sheathed cable or
figure-eight wire (for transducer connection)
1 160mm length of 5A (1mm2) hookup wire
1 200mm length of 14-way ribbon cable
8 PC stakes
1 30mm length of 5mm heatshrink tubing (for S1 connections)
1 roll of electrical insulating tape
Semiconductors
1 PIC16F1459-I/P microcontroller programmed with
0410520A.hex (IC1)
1 LMC6482AIN CMOS dual op amp (IC2)
1 7805 5V 1A linear regulator (REG1)
2 STP60NF06L logic level N-Channel MOSFETs (Q1,Q2)
3 BC547 NPN transistors (Q3-Q5)
1 SUP53P06-20 P-channel MOSFET (Q6)
1 13V 1W zener diode (ZD1)
1 1N5404 3A diode (D1)
1 1N4004 1A diode (D2)
6 3mm LEDs (red or green) (LED1-LED6)
Capacitors
1 4700µF 16V low-ESR PC electrolytic
2 100µF 16V PC electrolytic
2 10µF 16V PC electrolytic
1 470nF MKT polyester
4 100nF MKT polyester
Resistors (0.25W, 1% unless specified)
1 1M
2 100k
1 27k
1 20k
8 10k
7 1k
2 47
2 0.1 1W (SMD 6432/2512-size; Panasonic ERJL1WKF10CU or
similar) [RS Components 566-989]
NOTES: The transducer is rated at 50W and designed for 40kHz
operation. At the time of publication, eBay.co.uk part number
283977349993 is suitable (ensure you choose the 50W/40kHz
option). Otherwise, a search on line for ‘50/60W 40kHz ultrasonic horn
transducer, resonance impedance 10-20’ will yield further options.
You can get the remaining electronic parts for this project from
the usual suspects (for purchasers outside Aus/NZ, the Jaycar/
Altronics references provide sufficient information for choosing
parts); use element14, Digi-Key or RS Components for the more
specialised parts.
The PVC components for the transducer housing are readily
available from hardware and DIY stores.
by S1, which is wired back to the
PCB using a plug-in screw connector and socket (CON2). Power then
passes to the 5V regulator (REG1) via
reverse-polarity protection diode D2.
Linear regulator REG1 provides the 5V
required by IC1 and IC2.
12V DC also goes to MOSFET Q6
via fuse F1. This MOSFET is used as
a soft-start switch to charge the large
4700µF low-ESR bypass capacitor
slowly. Without soft starting, charging
the 4700µF capacitor would cause a
substantial surge current. This can
blow the fuse or cause a 12V switchmode supply to shut down.
When power is first applied, Q6 is
off and the 4700µF capacitor is not
charged. When the Start switch is
pressed, the RC3 output of IC1 goes
to 5V and this switches on transistor
Q5. The gate voltage of P-channel
MOSFET Q6 then begins to drop
towards 0V as the 10µF capacitor
33
Reproduced by arrangement with
SILICON CHIP magazine 2021.
www.siliconchip.com.au
(Above) If I knew you were comin’ I’d’ve baked a cake...
these are some of the stainless steel containers we found at
a kitchen supply shop which would be ideal for this project.
Choose the size and depth which best suits your application.
(Left) This shows what the completed Ultrasonic Cleaner
will look like when we cover the construction and testing
side next month. We’ll also show you how to set up your
ultrasonic cleaning bath using cheap ‘cooking’ containers.
charges via the 100k resistor to the
collector of Q5).
As the MOSFET begins to conduct,
it slowly charges the 4700µF capacitor.
After half a second, the gate charging is
stopped by switching off Q5 and after
a 250ms delay. The voltage across the
4700µF capacitor is then measured
using the AN8 analogue input of IC1.
If the voltage across the capacitor
is under 9V (3V at AN8), all the level
LEDs flash twice per second. This indicates that either the 4700µF capacitor is leaky, or there is a short circuit
causing the capacitor to discharge.
Power can then be switched off, and
the fault investigated.
If there is no error, Q5 is switched
back on, to continue charging the
gate of Q6. It takes one second for the
gate to drop 7.5V below the source,
at which time Q6 is almost fully on.
After a few more seconds, the gate
voltage will be very close to 0V, leaving the full 12V between the gate and
source. Zener diode ZD1 protects the
gate from over-voltage by limiting the
gate-source voltage to −13V.
Reverse polarity protection for the
power section of the circuit is via a
4A fuse F1, diode D1 and the integral
reverse diodes within MOSFETs Q1
and Q2. These diodes conduct current, effectively clamping the supply
voltage at −0.7V and protecting the
4700µF electrolytic capacitor from
excessive reverse voltage. This current will quickly blow the fuse and
cut power.
The bath
The ultrasonic transducer needs to be
attached to the outside of a suitable
container. This can be made from
stainless steel, aluminium or plastic
34
so that the ultrasonic vibration is efficiently coupled to the fluid. Stiffer
materials couple the ultrasonic waves
with fewer losses.
Ideally, the bath should have a flat
side or base where the transducer can
be attached. The bath material also
needs to be compatible with the epoxy
resin used to glue the transducer to the
bath. For our transducer, metals are the
most compatible material.
We found a series of ‘gastronorms’
(kitchenware tray/container) at a
kitchen supply shop that are ideal.
These are the types of food containers you often see at buffets. They
slot into steam tables that keep the
food warm, and they are available in
various shapes and sizes, with several
good options at or near the ideal 4L
(four-litre-volume) capacity.
You can get them made from stainless steel, polycarbonate or polypropylene with the first two options being
the best.
Just do a quick search in Amazon or
eBay for ‘gastronorm container stainless steel, 4 Litre,’ or similar.
We recommend either a 150mmdeep ¼ gastronorm tray (capacity 4L),
a 100mm-deep 1/3 gastronorm tray
(capacity 3.7L) or a 100mm-deep ¼
gastronorm tray (capacity 2.5L).
The 150mm-deep ¼ gastronorm tray
is tall and rectangular while the 100mm deep 1/3 tray is more square and
shallow. The other tray is in-between
the other two.
You can also get stainless steel or
clear or black polycarbonate lids to
suit all these, which would be a good
idea if you’re cleaning with a strongsmelling solvent (especially if you
plan to leave the solvent in the bath
when you aren’t using it).
Larger-sized baths with more liquid
will have a reduced cleaning effect
compared with smaller containers
with less fluid.
The fluid used in the bath can be tap
water with a few drops of detergent
as a wetting agent. Other fluids that
can be used include deionised water,
alcohol (methylated spirits, isopropyl
alcohol), acetone or similar solvents.
Cleaning effectiveness is greatly
enhanced when the fluid is warmed.
Filling with around four litres is ideal
for the power available from the ultrasonic transducer.
With deeper containers, it might be
possible to fill them with less liquid
for cleaning smaller items.
However, you would need to recalibrate the unit after each fluid level
change, and you might find that it
would shut down with less liquid in
the tank due to the transducer impedance dropping, and the power delivery
going above 40W.
This approach would require some
experimentation for successful use.
The recalibration procedure will be
described later. Note also that you
would need to mount the transducer
quite low on the container (or on the
base) to allow different fluid levels
to be used.
Conclusion
Next month, we will present the construction details, including how to
wind transformer T1, the PCB assembly steps, wiring it up, encapsulating
the transducer, case preparation and
final assembly.
We’ll also describe the testing and
calibration procedures, plus give some
hints on how to use the Ultrasonic
Cleaner most effectively.
Practical Electronics | September | 2021
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