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Soft
SoftStarter
Starter – tames
Are you alarmed by the juicy “splattt” from your mains power point
when you plug in something like a large plasma TV set? Do you sometimes burn out light and power point switches because of the surge
currents at switch-on? Or perhaps you occasionally trip circuit breakers
because of appliance switch-on surge currents. This is a very common
problem but there is a simple cure: our SoftStarter. It tames those nasty
surge currents while having no effect on appliance performance.
By NICHOLAS VINEN
T
his project was triggered by a number of readers experiencing problems with switch-on surge currents.
The first was a school teacher who wanted to
switch on banks of laptop computers in a language laboratory. Each time he attempted to do so it would trip out the
mains circuit breakers. The breakers would trip out even
though the total power drain of the laptops was far less
than the breaker’s rated current.
Eventually he found that the only way to switch on
without tripping the breakers was to switch on the laptops
in groups of three or four.
The second instance was a reader who fitted a large number of 10W compact fluorescent lamps to a large chandelier
– he was trying to toe the government line by not using
those nasty (but attractive candle style) incandescent lamps.
He found that each time he switched on the chandelier, it
tripped the 10A breaker.
We have a similar problem in the SILICON CHIP offices
with computer workstations comprising two monitors
and a desktop PC. Each combination has around 1.15µF
of capacitance at the mains plug and it can draw in well
excess of 100A when switched on!
Worse, one of our staff members measured the input capacitance of his current model Panasonic 50-inch plasma
TV at 1.3µF, between Active & Neutral (with its mains
switch off). Add in the capacitance of a DVD player and
VCR used to feed the Plasma set and you can start to see
there is a major problem.
All of the above problems relate to appliances which
have switch-mode power supplies. In essence, these look
and behave like a large capacitor being switched across
the 230VAC mains supply. No wonder you get a big splat
from the power switch.
Fig.1 shows the essentials of a switch-mode power supply. There is typically a 470nF capacitor connected directly
between the Active and Neutral leads followed by a bridge
rectifier feeding a 470µF 400V electrolytic capacitor to develop around 325V before the switch-mode circuitry itself.
No wonder these circuits generate such big surge currents.
We did a simulation of this circuit to get a handle on how
big these currents can be. Fig.2 tells the story. Depending
on the moment of actual switch-on, the peak current can
easily be more than 200A and this is backed up by some
scope measurements which tell the same story.
+
A
RSOURCE
~
N
Mains
Supply
E
GPO
470nF
250VAC
X2
~
470F
400V
Switchmode
Circuitry
RESR
.34
RLOAD
DC Output(s)
–
Fig.1: the configuration of a typical switch-mode power supply. An X2 capacitor (typically 100-470nF) is connected
between Active and Neutral to reduce the amount of switching noise that couples from the switching circuitry back into
the mains leads. The 230VAC is then rectified and filtered to produce around 325V DC and this is converted to lower
regulated DC voltages by the switch-mode module. Also shown is typical capacitor bank ESR (equivalent series resistance)
and the mains source impedance due to cabling etc, both of which affect the unit’s peak current draw at start-up.
28 Silicon Chip
siliconchip.com.au
the surge current menace!
Here’s the
SoftStarter in
the form we believe
will be the most popular
– in line with a 4-way powerboard which means four different
devices (computer, monitor, modem
and CFL desk lamp for example) all can
have their switch-mode supplies “tamed”.
Note that some switch-mode power supplies have active
power factor correction (active PFC) which involves extra
circuitry. This reduces the in-rush current but there is still
an initial surge as the storage capacitor(s) charge.
And while no switch-mode circuitry is involved, a similar
surge current problem can occur when large transformers
are followed by bridge rectifiers and large capacitors.
Think about the reader who built a very large power
amplifier with a 1kVA toroid power transformer. Switching it on could also trip a circuit breaker or cause the room
lights to momentarily flicker.
The SoftStarter solution
We actually tried several different approaches before
coming up with the SoftStarter. Perhaps the simplest and
most obvious approach is just to wire a high current NTC
(negative temperature coefficient) thermistor in series with
the 230VAC mains supply, eg, inside a power board.
WARNING!
This Soft Start circuit is powered directly from the 230VAC
mains and operates at lethal voltages. DO NOT TOUCH
ANY PART OF THE CIRCUIT WHILE IT IS PLUGGED INTO A
MAINS OUTLET OR CONNECTED TO MAINS WIRING and do
not operate the circuit outside its plastic case or without
the lid screwed onto the case.
These devices initially have a fairly high resistance which
drops quickly as they heat up. The high initial resistance
limits the in-rush current and after a shortt period, this
drops enough to allow normal current to flow into the load
after the initial surge.
The problem is that they run really hot – up to 228°C or
higher! This is unavoidable since they rely on the heat to
Switchmode Supply Power-on Simulation (RSOURCE = 0.5, RLOAD = 100) with 10 NTC
Switchmode Supply Power-on Simulation (RSOURCE = 0.5, RLOAD = 100)
+100
50
20
0
10
-100
-200
1
-300
200
+200
Potential (Volts)
Potential (Volts)
100
Mains At Socket
Capacitor Bank
Mains Current
Mains Current (Amps) - logarithmic
200
+200
100
Mains At Socket
Capacitor Bank
Mains Current
+100
50
20
0
10
-100
-200
1
Mains Current (Amps) - logarithmic
+300
+300
-300
0
5
10
15
20
25
30
0
5
10
15
20
25
30
Time (milliseconds)
Time (milliseconds)
Fig.2: SPICE simulation of Fig.1. Mains source impedances
are set to 0.5Ω and the load resistance is 100Ω. Inrush
current peaks at over 200A, limited by the mains source
impedance, bridge rectifier impedance and capacitor bank
ESR. The capacitor bank charges almost completely in
the first half-cycle. The high current distorts the mains
waveform both during the initial in-rush and at the voltage
peaks where some “flat-topping” is visible.
Fig.3: SPICE simulation with the same circuit as shown
in Fig.1 but with a 10Ω 15A NTC thermistor connected in
series between the mains socket and suppression capacitor/
bridge rectifier. The capacitor bank charges more slowly,
over several cycles and peak current is reduced to around
30A (close to our measurements). Note how the bridge
conducts for a longer period, even after the capacitor bank
has charged.
siliconchip.com.au
April 2012 29
ACTIVE
OUT
ACTIVE
IN
RLY1
S 4162A (10A) OR
JQX-105F-24 (20A)
1
TH1
SL32 10015
2
+24V
150nF*
250VAC X2
(FOR 10A
RELAY)
10M
1W
470 1W
*OR 330nF
250V AC X2
(FOR 20A RELAY)
D1
1N4004
A
EARTH
D5
1N4004
D2
1N4004
1M
A
K
D4
1N4004
A
A
ZD1
24V
1W
220F
35V
B
C
Q1
BC547
E
C
B
47F
16V
4
10M
Q2
BC547
E
10M
3
CON1
A
K
K
D3
1N4004
A
NEUTRAL
K
K
K
NOTE: ALL CIRCUITRY AND
COMPONENTS IN THIS PROJECT
MAY BE AT MAINS POTENTIAL.
CONTACT COULD BE FATAL!
0V
BC547
SC
2012
SOFT STARTER
1N4004
A
K
ZD1
A
B
K
E
C
Fig.4: the complete circuit diagram of the SoftStarter. NTC thermistor TH1 limits inrush current and after about two
seconds, it is shorted out by relay RLY1 for minimal heat generation and power loss. NPN transistors Q1 & Q2 drive the
relay coil and their switch-on is delayed by the 47µF capacitor. The +24V rail is derived from mains using an X2 series
capacitor, bridge rectifier and zener diode.
lower their resistance and allow enough current to flow.
Plainly, they run too hot to be installed inside a plastic
power board; they would melt the plastic! Apart from that,
it’s a waste of power. Depending on the load current, dissipation could be in excess of 5W.
Our solution is simple – we use a relay to short out the
thermistor after a few seconds. The voltage drop across the
relay is very low and so there’s virtually no power loss apart
from that required to keep the relay energised. In the case
of our SoftStarter, this is less than half a watt.
The proof that it works is in Fig.6. This shows the same
computer set-up as in Fig.5 being switched on with the
SoftStarter connected in series. The inrush current is now
limited to around 25A.
Note that the current waveform is much smoother and
lacks the big initial spike. Note also that the power supply
capacitors charge over many more mains cycles than they
would without the SoftStarter connected.
A number of scope screen grabs in this article reinforce
the story: without the SoftStarter you get big in-rush currents and splats from the power switch. Those splats, by
the way, are not just annoying: each one is responsible
for just a little more of the switch contacts melting and
wearing away.
Fig.5: current for a computer workstation over the first few
mains cycles after power is applied The initial draw of
103.6A is due to the initial charging of the capacitor banks
in the switchmode supplies. The second half-cycle peak is
much lower.
Fig.6: the same situation as Fig.5 but with the SoftStarter
in use. Maximum current draw is much lower at 25.3A for
the first half-cycle and 14.1A for the second. The capacitor
banks charge more gradually, over five full mains cycles or
so (100ms).
30 Silicon Chip
siliconchip.com.au
Here are the two versions of the SoftStarter – on the left the PCB is attached to the base of a standard electrical junction
box (in this case an Arlec 9071 but it could be a Clipsal, HPM etc). This version has the 20A relay but again, it could be the
10A relay. On the right is the same board (with 10A relay) placed inside a standard UB3 Jiffy box, as shown in the photo
at the start of this article.
With the SoftStarter everything is sweetness and light
and there is no drama at switch-on.
Two versions
The SoftStarter can be built in two different ways. First,
its PCB can be housed inside a UB3 jiffy box in-line with
a standard power board, extension lead or equipment
mains lead. It also fits into a standard electrical junction
box so that it can be permanently wired into, say, a lighting
circuit. It can handle loads of up to 10A or 2300W. That’s
the maximum load rating of a typical residential power
point (or GPO – which stands for General Purpose Outlet).
Circuit description
Refer now to Fig.4, the complete circuit diagram. Incom-
Fig.7: current flow for a 300VA toroidal transformer
charging a large capacitor bank through a bridge rectifier,
at switch-on. Peak current draw is 24A on the first cycle
and 14A on the second. It could be much higher with a
larger transformer.
siliconchip.com.au
ing mains power is wired to the ACTIVE IN and NEUTRAL
terminals while the load is connected to the ACTIVE OUT
and NEUTRAL terminals.
NTC thermistor TH1 is permanently connected between
the incoming Active line and the load.
This is an SL32 10015 thermistor has a nominal resistance at 25°C of 10Ω, falling to 0.048Ω at 228°C, which
is its sustained body operating temperature with a load
current of 15A. That is its rated maximum steady state
current and it takes around four minutes to reach operating temperature under full load conditions.
In our application, this will never happen as it’s shorted
out after about two seconds by the contacts of relay RLY1.
NTC thermistors have a few advantages over power
resistors in this role.
Fig.8: the toroidal transformer based power supply, this
time with the SoftStarter connected up. The inrush is much
lower with a peak of 14A on the first cycle and 11A on the
second. Current is drawn over a larger portion of the mains
cycle.
April 2012 31
TH1 SL32 10015
SILICON
CHIP
© 2012
SoftStarter
RLY1
S4162A
D3
4004
4004
BC547
Q1
10M
10M
1M
24V
ZD1
D4
470 1W
10M 1W
(330nF X2)
BC547 Q2
47F
+
NEUTRAL
150nF X2
EARTH
4004
ACTIVE IN
D5
ACTIVE OUT
(JQX-105F-24)
220F
+
CON1
35V
WARNING:
230V AC!
D1
4004
D1-D5
1N4004
4004
D2
Fig.9 the component overlay for the SoftStarter with
a straight-on shot of the PCB at right for comparison.
Take care with the mains wiring and NEVER operate the
SoftStarter with the lid off the case – it bites!
Firstly, they are rated to handle the very high (~250W)
initial dissipation. Secondly, their natural drop in resistance as they heat up provides a gradual increase in current.
Finally, they are much more compact than a typical
power resistor of equivalent current rating.
There are no timer ICs or oscillators in this circuit. Instead, the relay time delay of two seconds is provided by
the low-pass filter formed by the 1MΩ resistor and 47µF
capacitor, in combination with the base-emitter voltages
of NPN transistors Q1 & Q2.
At switch-on, the 220µF capacitor is initially charged
to 24V and the 47µF capacitor starts out discharged. After
a couple of seconds, when the charge across the 47µF capacitor reaches about 1.5V, the Darlington formed by NPN
transistors Q1 and Q2 turns on and energises the relay. Its
contacts short out the NTC thermistor, applying the full
230VAC to whatever is being switched.
After that, the full load current passes through the relay
until such time as incoming mains power is switched off.
After a second or so, the 220µF capacitor discharges and
the relay switches off. Diode D5 protects Q1 & Q2 from the
resulting inductive voltage spike.
After switch-off, the 47µF capacitor discharges via its parallel 10MΩ resistor (also via Q1’s base-emitter junction and
the 1MΩ resistor). After about 30 seconds it’s sufficiently
discharged for the unit to be switched back on again with
close to the normal two-second delay.
If it’s switched back on earlier, the delay will be shorter
but should still be sufficient.
Power supply
The 24V rail is derived from the 230VAC mains using
a capacitor/zener regulated supply. Diodes D1-D4 form a
bridge rectifier feeding the 220µF filter capacitor and 24V
zener diode ZD1 limits the voltage across this capacitor
to around 24V.
If we simply connected the full 230VAC mains to the
input of the rectifier, it and the zener diode would burn
32 Silicon Chip
out in spectacular fashion due to the virtually unlimited
current flow.
This is similar to the problem we are trying to avoid with
the SoftStarter! We need limit this current to a safe level.
The obvious way to do this is to use a resistor but then
that resistor would have about 200V across it and its dissipation would be high, making the circuit very inefficient.
So instead of using resistance we use the reactance of a
capacitor to limit the current. We simply choose one with
an impedance of around 20kΩ at 50Hz.
The formula for capacitor impedance is:
1
(2 π f C)
so for a 150nF capacitor at 50Hz we get 21.2kΩ. This gives
a much higher efficiency; over 50%.
This process is illustrated in Fig.6, the output of SPICE
simulation of the power supply circuit (using a 220nF
capacitor but the principle is the same).
The dashed green trace shows the voltage across the X2
capacitor and the difference between it and the mains voltage waveform (red trace) is the voltage across the rectifier,
which is limited to around ±25V due to the zener diode.
The dashed mauve trace shows the current flowing
through this X2 capacitor while the dotted blue trace shows
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Parts List – SoftStarter
1 PCB, code 10104121, 58 x 76mm
(available from SILICON CHIP for $10 + P&P)
1 6-position, 4-way PCB-mount terminal barrier
(CON1) (Jaycar HM3162, Altronics P2103)
2 M3 x 15mm machine screws with flat washers,
star washers and nuts
1 Ametherm SL32 10015 NTC thermistor
(Element14 1653459)
1 10A 24VDC coil SPDT relay
(Altronics S4162A or equivalent) or
1 JQX-105F-24 20A SPDT relay, 24V DC coil
(Futurlec JQX-105F-24 or equivalent)
1 UB3 jiffy box or mains junction box (eg Arlec 9071)
Semiconductors
2 BC547 100mA NPN transistors (Q1, Q2)
1 24V 1W zener diode (ZD1)
5 1N4004 1A diodes (D1-D5)
Capacitors
1 220µF 35V/50V electrolytic
1 47µF 16V electrolytic
1 150nF X2* (Element14 1215452) (for 10A relay) or
1 330nF X2* (Element14 1200831) (for 20A relay)
(* X2 capacitors will have their value printed on them)
Resistors (0.25W, 5%)
1 10MΩ 1W (code: brown black blue gold)
2 10MΩ
(code: brown black blue gold)
1 1MΩ
(code: brown black green gold)
1 470Ω 1W (code: yellow violet brown gold)
Additional parts for Jiffy box version
2 cord-grip grommets to suit 7.4-8.2mm cable
(Jaycar HP0716, Altronics H4270)
1 short length 2.5mm diameter heatshrink tubing
1 power board
1 small cable tie
Additional parts for junction box version:
4 No.4 x 9mm self-tapping screws
the product of this current with the mains voltage, ie, the
instantaneous power.
This power figure is positive when the current and voltage are in phase and this represents power drawn from the
mains while when it is negative, the current and voltage
are out of phase and it represents current flowing back
into mains.
As you can see, power tends to be drawn from the mains
when the X2 capacitor is charging, ie, when the voltage
across it is increasing in absolute terms. It is returned to
the mains when this capacitor is discharging. There is also
the additional current flow which is that consumed by
the circuit being driven which is on top of the capacitor
charge/discharge currents.
The actual power consumed is the difference between
that flowing into and out of the circuit. As you can see from
the figure, the area under the curve representing the power
drawn from mains is slightly larger than that returned and
the simulation gives the difference in this case as 421mW.
This is the real power drawn by the circuit.
34 Silicon Chip
A straight-on pic of the alternative mounting,
the mains junction box. This is actually on the
baseplate; the box fits over the top when the
baseplate is mounted (eg, to a joist).
The apparent power is calculated by multiplying the
RMS current by the RMS voltage (ie, 230V). The RMS current is 15.6mA; therefore the apparent power is 3.59VA.
This gives a power factor of 0.421 / 3.59 = 0.12. This may
seem low but given how little actual power the circuit
draws, it isn’t a problem.
If we re-run the calculations using a 150nF capacitor, we
get a real power of 210mW, an RMS current of 10.7mA, an
apparent power of 2.46W and a power factor of 0.085. This
agrees almost exactly with our measurements.
The 10MΩ resistor has negligible effect on the operation of the circuit and simply serves to discharge the X2
capacitor once the unit is unplugged (so you won’t get a
shock if you open up the box). The 470Ω resistor limits the
inrush current when the X2 capacitor is initially charged
to a maximum of 0.5A. Both of these resistors are 1W types
since these are generally rated for use with mains voltages.
An important aspect to note is that while 24V zener diode
ZD1 limits the voltage across the filter capacitor (220µF)
to 24V initially, once the relay is actually energised, the
voltage will drop to around 15-16V and ZD1 no longer
conducts.
The reason for this is that the voltage divider formed by
the reactance of the X2 capacitor, the 470Ω series resistor
and the relay coil resistance (around 1600Ω) limits the
filter capacitor voltage to around 15.8V. This is enough to
keep the relay reliably energised but reduces the power
consumption of the circuit.
Relay & X2 capacitors
One of two specified relays can be used: one is rated
siliconchip.com.au
Capacitor/Zener Mains Power Supply (SPICE Simulation)
20
Power In
Power Out
100
10
0
0
-100
-10
-200
-20
-300
Power (W)
200
Potential (V)
30
Mains 230VAC Input
X2 Capacitor Charge
Current Draw
Power Draw
Current (mA)
300
-20
0
5
10
15
Time (milliseconds)
20
Fig.10: SPICE simulation output showing how the X2
capacitor/zener power supply works. The X2 capacitor
charges and discharges with each mains half-cycle,
dropping the 325V DC peak voltage from mains to 24V.
The extra energy from the higher voltage is stored in the
capacitor and returned to the grid later in the half-cycle.
to switch 10A – it can be an Altronics S4162A or JQC21FF-024. The other is physically larger and is rated at
20A (7200VA) and has type number JQX-105F-24.
We have specified a 150nF X2 capacitor for use with the
10A-rated relay and a 330nF X2 capacitor for the 20A-rated
relay because its coil resistance is lower, at 660Ω.
Construction
The SoftStarter is built on a 58 x 76mm PCB, coded
10104121. It is double-sided with plated through-holes,
so the top layer can carry some of the load current.
Start by fitting the three smaller resistors. Use the colour
code table or a DMM to check their values. Follow with
the five standard diodes and the zener diode, orientated
as shown on the overlay diagram (Fig.9). All diodes have
their cathode stripes facing either the right side or bottom
of the PCB. You can then fit the two 1W resistors, again
using referring to the colour codes table or a DMM.
Crank the leads of the two BC547 transistors to suit the
PCB mounting holes, using small pliers, then solder them
in place. Follow with the small and then larger electrolytic
capacitors. In both cases, the longer positive lead goes in
towards the right side of the board.
The X2 capacitor and relay go in next. Use 150nF for
the 10A relay or a 330nF for the 20A relay. You may need
to turn up your soldering iron temperature to solder the
relay as it connects to a large copper area. Then fit the
thermistor, making sure it is pushed down as far as it will
go before soldering its leads. It will also need a hot iron.
Attach the terminal barrier using two M3 x 15mm machine screws. Place flat washers under the heads and star
washers between the nuts and PCB, then tighten them
down. Check the terminal barrier is parallel to the edge
of the PCB and then solder its pins, again with a hot iron.
Housing
As already noted, the SoftStarter PCB can be installed in
either a UB3 jiffy box in-line with a standard 4-way 230VAC
power board or extension cord, or in a standard junction
box if the device is to be permanently wired into a circuit.
We will deal with installation in a UB3 jiffy box first.
Originally we designed the PCB to snap into the moulded
side rails of the UB3 box but the thermistor is quite tall and
interfered with the lid, so we have made the final board
narrower and it simply sits in the bottom of the case. It can
be glued in place after it has been wired up and tested, so
it can’t move and put stress on the wiring.
Start by drilling a hole centred in each end of the box,
4-5mm at first, then enlarge them to 14mm using a tapered
reamer or stepped drill bit. It’s better to make the holes
slightly too small and enlarge them later if necessary since
if they are too big, the cord-grip grommets will be loose
and you will have to get a new box and start again.
The holes can then be elongated with a file in one direction, making a 14 x 15.9mm opening (flat sides, rounded
ends), to prevent the grommets from rotating. The correct
profile is shown on page 244 of the Altronics 2011-2012
catalog (Type B).
Now cut the power board cord. We cut ours about 23cm
from the power board so that the SoftStarter unit sits close
to the board. Strip 75mm of the outer insulation, then
expose 7mm of copper from the Active and Neutral and
Earth wires. At the other (plug) end, strip 130mm of the
INPUT
NEUTRAL
WIRE
24V
MAINS
OUTPUT
LEAD
4004
INPUT
EARTH WIRE
OUTPUT
ACTIVE WIRE
+
CORD
CLAMP
GROMMET
INPUT
ACTIVE WIRE
+
MAINS
INPUT
LEAD
SILICON
CHIP
© 2012
SoftStarter
NOTE: ALL CIRCUITRY AND COMPONENTS IN THIS PROJECT MAY BE AT MAINS POTENTIAL. CONTACT COULD BE FATAL!
NYLON
CABLE TIE
OUTPUT
EARTH WIRE
OUTPUT
NEUTRAL WIRE
CORD
CLAMP
GROMMET
Fig.11: here’s how to wire it inside the UB3 Jiffy box. We placed it in line with a standard 4-way powerboard – at about
$2.50 each they’re the cheapest way to get a mains plug, cord and (four!) sockets.
siliconchip.com.au
April 2012 35
outer insulation, then the inner wires the same as before.
Place one of the cables inside a cord-grip grommet, with
the narrower part towards the exposed wires and a small
amount of the outer insulation protruding beyond the grommet. If you’re lucky enough to have a grommet insertion
tool you can use that but otherwise, squeeze it together
hard with a large pair of pliers and then push it into one
of the holes in the jiffy box. This requires quite a bit of
brute force and co-ordination but if you do it right, the
grommet will go in and it won’t be possible to pull it out.
If it won’t fit, enlarge the hole slightly and try again.
Give the cords a firm tug to check they are anchored properly – you must not be able to pull them out or move them.
Now twist the exposed strands of the Active and Neutral
wires and screw them into the appropriate locations on
the terminal barrier. Refer to the wiring diagram of Fig.11.
The two Neutral wires go into the location marked “N”
and should be twisted together.
The Active wire from the power board goes to the
terminal at the opposite end (“ACTIVE OUT”) while the
Active wire from the plug goes next to that (“ACTIVE IN”).
Twist the two earth wires together tightly and attach them
to the terminal marked E. In each case, ensure that the
screw is done up tightly and that there are no exposed
or stray copper strands.
You can then place cable ties to hold the Active and
Earth wiring in place (see photo). Secure the PCB into the
bottom of the box using hot melt glue or silicone sealant
and fit the lid.
Junction box
We also designed the board to fit in an Arlec 9071 junction box (other brands such as Clipsal and HPM are very
similar). The PCB’s four mounting holes line up with those
in the base of the junction box and the rounded corners
leave enough room to access the other mounting holes, so
you can screw it to a ceiling joist or whatever.
The 230VAC mains wires can enter the box lid from
the side, using one or two of the knock-out sections.
Note that if it is to be installed in permanent wiring, the
task should be done by a licensed electrician or suitably
qualified person.
Check the wiring
Going back to the version in a UB3 Jiffy box, before powering up, it’s a good idea to do some basic tests. Measure
the resistance between the incoming and outgoing Active
wires – it should be close to 10Ω which is the cold resistance of the NTC thermistor. If it is much lower than this,
you may have a short circuit somewhere.
Also check the resistance between each Active line and
the Neutral line. The reading should be around 15MΩ.
Again, if it is low, check carefully for shorts.
Finally, check for continuity (ie, 0Ω) between the Earths
of the in-going and out-going power cord. Then apply
power (it isn’t necessary to attach a load). After about
two seconds you should hear the click as the relay turns
on. Remove power and the relay will click again within
a second or so, as it releases.
Assuming all is well, repeat the test with a load and this
should confirm that it is working properly. For best results,
once you have switched off power to the SoftStarter, wait
sc
at least 30 seconds before turning it back on.
36 Silicon Chip
Why is the 50Hz AC
E
veryone knows that the 50Hz AC mains waveform
is a sinewave, right?
Well, in theory it is a sinewave but in practice
it is distorted because the peaks have been clipped off.
For years now our scope screen grabs have shown this
but we have not dwelled on the reasons why.
Recently though, we have had emails from readers
who have sent photos of their scope screens showing
the classic flat-topping of the mains waveform. And they
want to know why this is happening.
You can blame this gross distortion of the mains
waveform on two factors: gas discharge lighting and
switch-mode power supplies.
Gas discharge lighting refers to all lighting systems
which use an electric current through a gas to generate
light. It applies to all high and low-pressure sodium
lamps, mercury vapour lamps and fluorescent lights.
In each of these cases, the gas discharge draws current
from the AC mains supply only when the actual voltage
across the lamp exceeds about 100V. So the current is
only drawn from the peaks of the waveform and this
inevitably loads down or clips off the peaks.
In recent years the situation has become much worse
for the electricity generators and distributors with the
widespread use of switch-mode power supplies in virtually all electronic appliances.
It more or less started with the advent of PCs and their
adoption of the more efficient switch-mode rather than
conventional mains transformer-driven power supplies
which are much heavier, bulkier and more expensive.
Switch-mode power supplies were naturally also used
in laptop supplies, then TV sets, DVD players etc. Now
they are used in virtually all electronic equipment with
the sole exception of high performance audio amplifiers
(such as our own Ultra-LD amplifier series).
Naturally all those large power-hungry Plasma TVs
(albeit these days not quite so power-hungry) and large
screen LCD TV sets use switch-mode supplies.
The reason why switch-mode power supplies are such
a problem is that they all essentially consist of a bridge
rectifier and a big capacitor, followed by the switch-mode
circuitry itself. It is the bridge rectifier and big capacitor
which is the problem because current only flows into
the capacitor at the peaks of the 50Hz mains sinewave.
All of the power drawn by the appliance is drawn
from the mains during the peaks of the waveform – not at
the other times (unless they are fitted with active power
factor correction and relatively few are).
Have a look at the simulation of Fig.2 on the second
page of the SoftStarter article. This set of curves depicts
what happens: large pulse currents which coincide with
the peaks of the mains waveform.
The simulation is for a 100Ω load which will draw a
nominal 529 watts from 230VAC mains. But the current
drawn from the mains is not a nice sinusoidal 2.3A but
is a pulse waveform with peaks of about 15A!
No wonder the peaks of the waveform are being
clipped off.
siliconchip.com.au
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