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=20
=20
=
=20
=20
Switchmode=20
Power Supply For Car Audio =20
=20
The=20
Audio Pages
Elliott Sound =
Products
Project=20
89
Switchmode Power Supply For Car Audio Sergio=20
S=E1nchez Moreno and Rod Elliott
Foreword =20
This contributed project is a result of considerable collaboration =
between=20
Sergio and myself, and should not be seen as necessarily a complete =
project in=20
itself, but a stepping stone to understanding switching power supplies, =
how they=20
work, and what you can do with them.
Be warned - there is considerable risk. Because of the =
extremely high=20
current available from a car battery, a tiny mistake may easily lead to=20
catastrophic failure. All electronic components are said to =
contain smoke=20
(wire contains an enormous amount), and a slip of the soldering iron can =
liberate an unbelievable quantity. Seriously though, the risk of =
severe=20
burns and the possibility of causing a fire in your car are very real, =
and=20
should not be underestimated. 300A from a car battery can do a =
vast amount=20
of damage in a few milliseconds - should the fuse not blow (you=20
will use a fuse, won't you?), then the damage can be =
extensive.=20
At various points in Sergio's part of the article, I have added some =
of my=20
own information. This is shown in indented small font text.
Please see the special=20
note at the end of this article for important information about the=20
project.
Introduction =20
The difficulties of installing an HI-FI system in a car are many, =
although=20
there is no doubt that the most important is the limitation of the =
vehicle=20
supply voltage. As most readers already know, the nominal voltage of a =
car=20
battery is 12V, reaching about 13.8V when charging (i.e., engine =
running).
The maximum RMS. audio power from a given voltage V is somewhat less =
than:=20
Pmax =3D ( V / ( 2 x 2=20
) )2 / R
=85=20
where RL is the speaker nominal =
impedance.=20
Thus, for a 13.8V system, this power is limited to about 6W on a 4 =
Ohm load.=20
Note that the lower the resistance of the speaker, the higher the =
maximum power=20
(this is the reason most audio speakers have a 4 Ohm nominal impedance =
instead=20
of the more common 8 Ohm in home systems).
This may be simplified to some extent =
... =20
P =3D (V / 3) 2 / RL
and a typical calculation =
based on a=20
13.8V supply gives =20
P =3D (13.8 / 3) 2 / 4 P =3D=20
4.6 2 / 4 =
=3D 5.29=20
Watts
This allows for standard losses, and is =
acceptably accurate=20
at this voltage - the only real way to know is to measure the amp, =
since the=20
losses vary depending on the topology of the output stage in=20
particular.
Power output can be increased by a factor of nearly 4 by using =
bridging=20
techniques, explained in more detail in ESP project 14, so we can obtain =
up to=20
about 24W on a 4 Ohm speaker. This can be enough for the midrange and =
high=20
frequencies, but is obviously very limited for a subwoofer application, =
for=20
example. (moral: distrust of "4 x 45W" head units is well advised, for =
they=20
certainly aren't talking about RMS power).
So, what can be done to increase available audio power? The answer is =
a=20
simple derivation of the above formula - either decrease load impedance =
or=20
increase supply voltage. The lower the impedance, the more current is =
needed,=20
making the construction of low impedance output stages more difficult =
(there are=20
some other practical limits), so let's increase supply voltage.
Switch Mode Power Supply Basics =20
The vast majority of high-powered audio amplifiers use SMPS (Switch =
Mode=20
Power Supplies) to generate higher voltages from the available 12 (13.8) =
volts.=20
An extensive theoretical explanation on how these things work is beyond =
the=20
scope of this article, but these are some fundamental ideas you should =
know=20
about switch mode power supplies (SMPS) for car amps:
The DC voltage at the battery has to be switched in some form to =
generate=20
an AC waveform suitable for a transformer. As you already know, a =
transformer=20
basically converts the AC voltage in its "primary" to a scaled version =
of it=20
in its "secondary", the scale factor being the turns ratio of the =
primary to=20
the secondary . (Again, take this as an extreme simplification). A =
transformer=20
doesn't allow DC voltages to pass, and there is electrical (galvanic)=20
isolation between both windings.
The AC waveform is usually a square wave that is relatively easy =
and
efficient to generate. The frequencies usually fall between 25kHz and =
100kHz=20
or more, thus allowing smaller transformers than the used in main =
appliances=20
(its construction is also different, their cores are not laminated, =
but made=20
from ferrites or "iron powder"). The switching elements have to be =
capable of=20
high currents and must also be fast and have low switching losses. =
Usually,=20
power MOSFETs or high speed bipolar transistors are used (some SMPS =
designs=20
use SCRs but these are in the minority).
Once this waveform is stepped-up by the transformer, it has to be
rectified again and filtered back to DC, since that is what we want. =
For=20
audio applications, we usually need a symmetrical supply, +/-35V, for =
example.=20
The rectification is done with a diode bridge, as it would be using a=20
conventional transformer at 50 or 60 Hz. Note that for the frequencies =
we are=20
talking about, fast or ultra-fast diodes are needed.
If we need a regulated power supply, some kind of feedback must be
provided from the output rails to a controller that can change some
parameters of the AC waveform at the primary of the transformer. This =
is=20
normally accomplished with PWM (pulse width modulation). We will =
explain this=20
later, in the "regulation" paragraph.
Always keep in mind that no energy is created =85 given a (total) =
rails to=20
battery voltages ratio, the current drawn from the output will be (at =
least)=20
be multiplied at the 12V input by the same ratio, thus the total power =
stays=20
the same (assuming 100% efficiency, and that is never the case). A =
generic=20
transformer "transforms" the voltage by a factor of Tr, current by a =
factor of=20
1/Tr, and impedance at the secondary by a factor of 1/sqr(Tr), Tr =
being the=20
turns ratio. Impedance is of little importance in this =
context.
A well built SMPS can reach 90% efficiency. So, if you expect to =
produce=20
+/-35V at 6A (per rail) supply (this supposes 35x6 + 35x6=3D360W) then =
be=20
prepared to draw more than 30A from the battery! Fortunately, when =
talking=20
about audio amps reproducing music, power requirements are always much =
lower=20
than with pure sine waves. At this point, the reader should =
realise the=20
magnitude of the currents involved in a high power SMPS for a car =
amplifier, and=20
that extreme caution should be taken especially when connecting "the =
creature"=20
to the car electrical system.=20
The system =20
The present project describes the construction of a flexible SMPS =
capable of=20
delivering powers in the order of 350W continuously, depending on the=20
transformer used. The output voltage depends mainly on the turns ratio =
of the=20
primary and secondary windings, but may be adjusted to a somewhat lower =
value=20
using regulation. This should be enough to power a 200W subwoofer =
amplifier plus=20
perhaps 2 stereo amps for the mids and highs.
It is part of a complete car amp that I have built, with 6 power =
stages based=20
on National's LM3886 Overture Amplifier. They can be combined into one=20
>250W/4 Ohm subwoofer channel plus 2 x 65W/4 Ohm mid+high channels,=20
alternatively into 2 x 120W/4 Ohm + 2 x 65W or even to form a =
multichannel 6 x=20
65W/4 Ohm amplifier, so it is an extremely flexible and high-powered =
system=20
without renouncing sound quality. The parallel bridging techniques =
needed to do=20
this will be possibly described in another project.
Construction of the SMPS =20
The complete schematic of the SMPS is shown below.
Note: This is Sergio's original version of the =
supply, the=20
one shown in Figure=20
9 is likely to be the most commonly used, as it is somewhat simpler, =
but has=20
virtually identical performance. [esp]
Figure 2 - Switchmode Controller=20
Schematic
There are three main blocks described below ...
A - Switching MOSFETs and transformer B - Rectification and =
filtering=20
C - Control circuitry
A - Switching MOSFETs and Transformer The selected =
switching=20
topology is called a "push-pull" converter, because the transformer has =
a double=20
primary (or a "centre-tapped" one, if your prefer). The centre tap is=20
permanently connected to the car battery (via an LC filter to avoid =
creating=20
peaks in the battery lines, which could affect other electronic =
equipment in the=20
car). The two ends of the primary are connected to a pair of paralleled =
MOSFETs=20
each that tie them to ground in each conduction cycle (Vgs of the =
corresponding=20
MOSFET high).
These MOSFETs should be fast, able to withstand high currents (in =
excess of=20
30A each if possible) and have the lowest possible Rds(on). The proposed =
On-Semiconductor=92s MTP75N06 can withstand 75Amp and has a Rds(on) =
below 10=20
milliohm. This is important, because the lower this resistance is, the =
less=20
power they are going to dissipate when switching with a square waveform. =
Another=20
alternatives are MTP60N06, or the more popular BUZ11 and IRF540.
Although the schematics show a previous bipolar push-pull stage, you =
can also=20
connect the gate resistor directly to the output of the controlling IC, =
leaving=20
out the transistors, as the SG3525 is capable to drive up to 500 mA=20
(theoretically), more than enough to switch the MOSFETs fast.
B - Rectification and Filtering If one looks to the =
secondary side=20
of the SMPS, it resembles exactly the scheme of a typical mains PSU, =
with one=20
fundamental difference - the switching diodes have to be FAST or =
ULTRAFAST, if=20
you use a standard diode bridge the system will simply blow up (and this =
can be=20
very impressive, believe me!) Although a diode bridge is represented, it =
can be=20
made with discrete diodes as well. Use high current (10 A minimum and a =
suitable=20
voltage rating) diodes. I recommend using 4 x TO220 double diodes that =
can be=20
paralleled to form a single one in each package.
You may be surprised that the capacitors aren't too big. This is due =
to the=20
high switching frequency. It is important that they are good quality =
ones and=20
must be rated for 105 degrees operation. Ripple current rating and low =
ESR=20
(equivalent series resistance) is very important for any switching =
supply. In my=20
opinion, 5000uF per rail is enough.
C - Control Circuitry The controller IC is an SG3525. It =
comprises=20
all the necessary subsystems to generate a fixed frequency, compare with =
a=20
reference to modulate its pulse width and drive two outputs without =
overlapping.=20
It works from 8 to 35V and filtering in the supply is recommended, as =
shown. As=20
stated above, you can connect the outputs directly to the gate resistors =
of the=20
MOSFETs if you don't want to include the bipolar stages.
The resistor RT and capacitor CT fix the oscillation frequency.
Experimentation showed me that about 35kHz produces good results with =
my=20
transformer. Another capacitor, Css fixes the "slow start" time - when =
you turn=20
on the system, the pulse width increases from 0 up to the steady value, =
thus=20
limiting the "inrush" current, a very good feature to avoid "thumps" in =
the=20
speaker and protect the electrical installation. It has also a shutdown =
pin that=20
allows control of the SMPS from an external signal (REMOTE from the head =
unit,=20
for example).
In this project, layout is critical, incorrect track widths or =
excessively=20
long traces can have high inductances and produce peaks that can make =
the=20
MOSFETs blow up. ESP will probably offer a suitable PCB layout if there =
is=20
enough interest in it.
Transformer Construction Details =20
This is the most critical part of the design, and you have two =
options,=20
buying a commercial unit with the required power rating and turns ratio =
(hard to=20
find, only a single supplier found at the time of writing), or wind your =
own.=20
If you choose to wind your own transformer (as if you have much =
choice), you=20
have to decide which shape of core to use. The preferred material is =
ferrite,=20
which has high permeability (ability to "conduct" magnetic flux) or iron =
powder,=20
which has a lower permeability, but is less likely to saturate. Most =
commercial=20
transformers use ferrite, and iron powder is generally the best material =
for=20
filter chokes (inductors) that carry substantial DC.
For example, with a standard ETD39 core you could theoretically build =
a >=20
350W supply. Winding this type of cores is not very difficult, but you =
will have=20
to follow some guidelines I provide below in order to have good results. =
Another possibility is using a toroid. You can extract it from a BIG =
power=20
inductor. As a guide, a 4cm diameter toroid with a section of about=20
1cm2 can be used for a > 250W SMPS. Winding =
is a=20
little bit more complicated than with ETD cores but with a little =
practice is=20
not too difficult either.
Toroidal cores
ETD-type cores
Toroid from ITL 100 inductor (Wilco Corp). =
(Remove the thick wire before winding! =
:-)
These are a few general winding guidelines for all types of cores: =
You MUST use enamelled copper wire for all the windings. Keep also =
in mind=20
that when working with high frequencies, the effective section of the =
wire is=20
much smaller than the physical one, due to the "skin" effect (the =
current=20
concentrates only in the outer part of the wire). As high currents are =
involved here, the section of the wire is very important, (if you =
don't want=20
the enamel to fuse due to the heating produced by the resistive losses =
of the=20
wire and short all the windings). A good practice is to use several =
thinner=20
wires in parallel rather than a single thick one. This also eases =
winding. For=20
example, six 0.4mm diameter wires can form a suitable primary for a =
300W=20
supply. The same applies to the secondary, although the current is =
reduced so=20
you can use less wires (3 or 4, for example). From now on, I will =
refer to=20
each composite wire as "winding", and to each thin wire as =
"wire".
The wires must be tightly wound. You must wind the primary first, =
trying=20
to cover all the surface of the core, and then the secondary over it =
in the=20
opposite direction, to maximise inter-winding coupling.
A good starting point is using 4 turns for each primary (that is, =
4 turns,=20
centre tap and another 4 turns IN THE SAME DIRECTION). To calculate =
the number=20
of turns of the secondary winding, multiply by the turns ratio. For =
example,=20
if you want to build a +/-30V supply, the turns ratio is 30/13.8=3D2.2 =
approx,=20
so wind 2.2 x 4 =3D 8.8 turns (better 9 turns, to overcome the diode =
losses) for=20
each secondary (that is, again, 9 turns, centre tap and another 9 =
turns IN THE=20
SAME DIRECTION).
To start winding, take the number of thin wires you have decided =
to use
(6, for example) in the primary, all together. Leave about 3 or 4 cm =
out of=20
the core to ease connection to the board and start winding. When you =
have=20
wound 4 COMPLETE turns, go out the core and cut at 3 or 4 cm. Now you =
have the=20
first primary. Then start again IN THE SAME DIRECTION winding the =
other 4=20
turns and at the end leave another 3 or 4 cm for connection. Twist =
together=20
the thin wires of each winding at the ends, to ease =
soldering.
The varnish of the wire is intended to provide electrical =
isolation, so
you have to remove it at the ends to make the connections to the =
board. Be=20
sure to remove about 1cm to the end in ALL the wires you use. You can =
do that=20
using a special solvent or with sandpaper and a lot of patience BEFORE =
winding. The following are photos of two models of =
transformers. The=20
left one is a toroidal I wound myself using the core from a big inductor =
from=20
Wilco Corporation (ITL-501), and the right one is a commercial unit from =
a US
manufacturer (2x3:1, 350W). Both worked similarly.=20
=20
Left - Home Made =
Transformer. =20
Commercial Transformer - Right
Other remarks
The relay allows disconnecting of the power supply with the REMOTE =
(or=20
"Electrical Antenna" from the head unit. Power consumption when off is =
then=20
only the gate currents of the MOSFETs (A few nA) and the base current =
of the=20
transistor that controls the relay (a few uA). Nothing to worry about, =
certainly.
Connect a big choke in series with the supply, as this will =
eliminate the=20
switching noise that could interfere with other electrical equipment. =
You can=20
use the toroid that filters the +5V output of a old PC supply. (see =
figure=20
below)
=20
My system's input choke, obtained from an old =
PC power=20
supply.
All the wiring, especially the primary side must be heavy gauged, =
in order=20
to minimise losses and avoid over-heating of the conductors. The PCB =
tracks=20
should be thick enough, as short as possible, and reinforced with a =
generous=20
tin layer and possibly with soldered wire.
Put two fuses in the rails outputs, as they can save you a lot of
headaches when you short them to ground, etc. I used two standard =
6.3A
fuses.
Mount the rectifier diodes and the MOSFETs on a decent heatsink, =
and keep=20
in mind that they must be electrically isolated. Follow the usual =
heatsink=20
mounting recommendations (thermal grease, etc.). TO220 packages are =
easy to=20
handle.
=20
Detail of the MOSFET =
arrangement
Note the insulation pad (one for all) and the thick supply =
wires. =20
Individual insulation pads may be used with no loss of =
performance. Use of=20
a clamping bar will give improved thermal conduction to the heatsink =
bracket,=20
but do not over tighten, or the bracket will bend.
Tests =20
This project handles quite large powers, so it is well worth the pain =
of=20
step-by-step testing before you regret blowing all your work up in a=20
microsecond.
For the tests, use a big 12V to 13.8V power supply, with current =
limiting if=20
possible and capable of delivering at least 10 to 20 amperes (see =
project 77).=20
If you don't have that, a PC computer PSU will work (although you won't =
get more=20
than 80-90W, but it is enough for testing purposes and almost =
indestructible).=20
Don't connect the SMPS to a car battery the first time you test it (it =
can be=20
really dangerous!). A 10A fuse in series with the 12V supply is also a =
good
idea. (You don't know to what extent! ;-)
The cables from the supply to the amp should be as short as possible =
and=20
heavy gauged, to minimise losses. First time I tested the amp I had a 1 =
volt of=20
difference from one side to the cable to the other in only 1.5 metres: =
the cable=20
itself was dissipating more than 15W!!!. So, when calculating =
efficiency, always=20
measure input voltage just at the input of the SMPS to account for this. =
First of all, with only the SG3525 chip and its associated =
components (no=20
MOSFETs), check that you have a very clean 12V square wave in each =
output=20
(180=BA out of phase and they do not overlap EVER). Check also that =
when you=20
turn-on the power, it starts from 0% to 50% duty cycle in about a =
second or=20
two.
Once you have this, you can mount the MOSFETs. Do it on a =
heatsink, but be=20
aware that the tabs are connected to the Drain, so provide insulation =
(mica +=20
plastic washers, the usual stuff). Then solder the transformer and =
watch the=20
primary waveform with an oscilloscope (use a 10:1 probe just in case =
you have=20
large spikes in order to avoid damaging the instrument). You should =
have a=20
square wave of about 25-26V peak to peak and the smallest peaks =
(overshoot) as=20
possible. It they are higher than 30V (from ground), you may try to =
re-wind=20
the transformer to improve coupling. You can also reduce the =
overshoots using=20
the snubber network shown in the schematic, although they will =
dissipate a bit=20
of power (use 2W resistors and 100V capacitors), so mount them only if =
necessary.
Once you have a clean waveform, you can solder the rectifier and =
output
capacitors and see what you have in the positive and negative rails. =
You=20
should have the same voltage in both, and it should be similar to what =
you=20
calculated.
Now try to load it with power resistors. Start with low power =
consumption=20
(about 20W) and observe the mosfets, rectifiers and transformer =
carefully to=20
see that they don't heat up. Also watch the current drawn from the 12V =
supply.=20
The power (V x I) should be only a bit higher than that at the output =
load.=20
(Expect a 80% efficiency or so).
If everything goes well, increase the load (decrease its =
resistance
value). The mosfets should get warm after a while with heavy loads =
(about=20
100W), and the efficiency should maintain high (always above =
75-80%).
When you are completely sure that everything works as expected, you can =
proceed=20
to connect it to the car electrical wiring (see "installation =
procedures"=20
paragraph). First time you will notice an spark due to the sudden charge =
of the=20
big input capacitor, unless you connect a resistor in series first (very =
good=20
practice) to allow it charging slowly and then remove it for normal =
operation.=20
Installation procedures =20
For your car and own safety, it is VERY IMPORTANT that you pay =
special=20
attention when installing the power supply (and amplifier) in your car. =
These=20
are some recommendations that everyone should follow carefully:
The supply MUST be taken directly from the battery, not to the =
radio or=20
other +12V cables, as you will just blow or burn them, with the risk =
of a fire=20
in the car. The supply wire must be of adequate section, about 5 mm =
diameter=20
(excluding the plastic cover) minimum.
A fuse MUST be connected in series with the supply wire, as near =
the
battery as possible, because otherwise, in case of a collision, the =
wire can=20
be shorted to ground, which WILL produce a fire. This is not a joke! =
The=20
battery can produce in excess of 300 A that can burn virtually =
anything in a=20
fraction of a second.
Another fuse should be put at the +12V input of the amplifier, in =
order to=20
protect it from over current. My recommendation is to put a smaller =
value than=20
the definitive and test the amp for a few days to see if it overheats, =
etc.=20
For example, a 10-15A fuse can be suitable.
The FIRST connection you have to make to the amp is Ground, and =
that must=20
be firmly screwed to the car chassis as near the amp as possible with =
thick=20
wire. Notice that, if you connected, for example, the signal RCA =
cables first=20
and then the +12V wire, the input capacitors would try to charge =
returning to=20
ground via the audio cables, possibly ruining the preamplifier of the =
head=20
unit.
Regulating the Power Supply =20
The project itself has excellent load regulation, and the rails =
voltage is=20
almost only determined by the turns ratio, but it has inherently zero =
line=20
regulation (basically, it "simply" multiplies the input voltage by the =
turns=20
ratio), although this is not a problem in a car, where the battery =
voltage=20
remains essentially constant.
If the obtained output voltages are very high and you can't (or don't =
want=20
to) modify the windings, you can use regulation to lower them a bit. For =
example, I use a 3:1 transformer that would give about +/-38V without =
regulation=20
that is unacceptable for my LM3886 stages to be safe, so I have =
regulated to=20
+/-26V. The MOSFETs will suffer more, however, so regulate the supply =
only if=20
strictly necessary.
You can install the feedback potentiometer and set it in order to =
have zero=20
reference voltage to deactivate regulation, or increase its value to =
regulate to=20
the desired voltage.
NOTE: Regulation will work better with output inductors just between =
the=20
rectifier diodes and the output capacitors. 10 to 100 uH with iron =
powder core=20
and at least 8A current rating can be adequate. (I don't use them and my =
supply=20
works reliably, although I never put it to the power limits). You can =
also=20
improve safety by paralleling more MOSFETs, so the current through them =
is=20
shared. This also improves efficiency a bit, as the total Rds(on) is =
reduced.=20
Obtaining +/-12V from the SMPS for Preamplifiers =20
If you need to power opamps for a crossover, equaliser or =
preamplifier, you=20
can obtain a symmetrical +/-12V (for example) from the main supply =
rails, simply=20
with a resistor, zener and capacitor. (see Figure 1 of Project 27). =
Remember to=20
use 1 or 2W resistors and zener diodes. You can obtain about 25-50 mA =
from this=20
without problems.
Additional Information =20
The following material is from ESP - there are some suggestions and
additional information, as well as a simplified version of the SMPS. =
Although my version of the switcher is simplified, this does not =
imply that=20
performance is lower than Sergio's original, but is the result of my own =
experiments and tests. We may be on opposite sides of the planet, =
but=20
there was considerable collaboration during the development of the =
supply, and I=20
have built and tested the version shown below.
MOSFETs and Thermal Runaway =20
It has been claimed that MOSFETs are immune from thermal runaway, =
since they=20
have a positive temperature coefficient for their "on" resistance. While =
this=20
may be partially true for a Class-AB power amplifier, it is completely =
false for=20
a switching supply.
For example, a push pull SMPS using one IRF540 MOSFET a side draws =
30A at=20
full load. If we check the data sheet, we find that Rds(on) is 0.044 Ohm =
(44=20
millohms) at 25 degrees C, then we know that it will generate
P=3DI2 x R =3D =
302 =20
x 0.044 =3D 900 x 0.044 =3D 39 W peak (per transistor). At =
50 degrees=20
(not uncommon in a car that has been in the sun for some time), Rds(on) =
will be=20
about 1.25 times the value at 25 degrees (this is from the datasheet), =
or 0.055=20
ohms. Power dissipation will now be 49W, so the heatsink has to dispose =
of more=20
heat. We can guarantee that the extra heat will cause the heatsink =
temperature=20
to rise further, which will increase Rds(on), and that will make the =
heatsink=20
hotter, and =85 BANG=20
Ensuring that you use parallel devices and a good heatsink will =
reduce the=20
likelihood of this dramatically. Two MOSFETs sharing the load will =
dissipate 1/4=20
the power (each) of a single device, and have a lower thermal resistance =
to the=20
heatsink as well.
P=3DI2 x R =3D =
152 =20
x 0.044 =3D 225 x 0.044 =3D 9.9 W peak (per transistor) - 19.8 W for=20
both The power shown per transistor is the peak - actual =
(RMS) power=20
(per device) is half that calculated. The total power =
dissipated by=20
both transistors (or sets of transistors in the case of paralleled =
devices) is=20
the full value shown, since when one device is "on", the other is "off" =
and vice=20
versa.=20
Naturally, the maximum dissipation will only occur at maximum =
(continuous)=20
amplifier power - the real life requirements are usually somewhat less, =
however,=20
it is essential that the design is capable of continuous "worst case"=20
dissipation to ensure an adequate safety margin.
I strongly recommend that you do the calculations yourself, and make =
sure=20
that you understand the implications.
Regulation =20
Normally, one would expect regulation as shown in Figure 1, however, =
using=20
the feedback input of the controller IC relies rather too heavily on the =
impedance of the DC supply lines. Normally, output inductors are =
used=20
(with an additional "flyback" diode) to provide a pulse width to voltage =
converter. The majority of commercial systems seem to use a =
non-regulated=20
converter, so I would consider that this will be quite acceptable in=20
practice. Tests so far have shown that with a load of about 150 =
Watts, the=20
regulation was almost entirely dependent on the voltage drop in the =
supply line!=20
As well as being unregulated, there are a couple of other changes in =
the=20
circuit. R8 (100 Ohms) is connected between the timing capacitor =
and=20
discharge pins of the controller IC. This introduces a "dead time" =
where=20
both outputs are turned off, and the reason for this is to ensure that =
the power=20
MOSFET pairs can never be switched on at the same time - should this =
happen, a=20
very large current will flow (albeit for only a microsecond or =
less). =20
Since I did not use the extra switching transistors and used higher =
value gate
resistors, the dead time is important.
I also increased the switching frequency. As shown, the =
internal=20
oscillator runs at approximately 50kHz (my prototype actually runs at =
54kHz),=20
where Sergio's original was designed for 35kHz switching. The =
difference=20
is determined by the resistor on the RT pin of the controller, in my =
case, 12k.=20
Regulation will obviously make the circuit much more complicated, and =
as=20
stated above, my version is unregulated. This will maintain =
maximum=20
efficiency, and also reduces the dependence on the output filter =
capacitors -=20
they are effectively fed with almost pure DC from the rectifier at all =
loads, so=20
storage time is not an issue. Relatively small filter capacitors =
can be=20
used, and the output will still be quite clean.
Not surprisingly, the turns ratio is very important if regulation is =
not=20
used. Assume an input voltage of 12V to allow for losses. To =
obtain=20
+/-24V, the turns ratio is 1:2 - for each turn on the primary, there =
will be 2=20
turns on the secondary. This is the same as Sergio's description, =
and the=20
same rules apply. Unlike a normal mains transformer supplied with =
a=20
sinewave, the switching waveform is a squarewave, so the peak and RMS =
values are=20
the same (in other words, there is no 1.414 conversion as would be the =
case with=20
a mains frequency transformer). The problem with this is that the =
12V=20
assumed at full load will be 13.8V under light or normal loading, so the =
voltage=20
will be higher than expected. Using the same transformer as above =
(1:2=20
turns ratio) the no-load output voltage will be 27.6 volts - make sure =
that you=20
do not exceed the voltage rating of the amplifier!
Figure 9 - Simplified Version of =
Switching=20
Supply
Since the transformer is relatively easy to wind, it is not a =
difficult task=20
to dismantle it and add (or remove) secondary turns to get the voltage=20
right. My prototype transformer used 5+5 turns for the primary, =
and I used=20
3 strands of 0.8mm winding wire twisted together. There is plenty =
of room=20
in the recommended core, so it would be easy to use 5 strands instead =
for lower=20
losses.
Note that in the above (Fig. 9), the the heavy leads shown carry =
substantial=20
current, and must be sized accordingly. I do not recommend PCB =
traces be=20
used, since the current involved is simply too high. Given that =
the=20
suggested current density for PCB tracks is 4.0 A for a 100 "thou" (0.1" =
or 2.54=20
mm) track, then for 30A you need a track 0.75" (19 mm) wide! This =
is=20
difficult to accommodate on any printed board.
I also eliminated the relay, but at the cost of a small current when =
the unit=20
is not operating. The SG3525 has a shutdown pin for just this=20
purpose. A signal from the remote head amp will turn on Q1, and =
remove the=20
shut down signal from the controller. It behaves in exactly the =
same=20
manner as if power had just been applied, and the unit will become fully =
operation in about 2 seconds or less. Current drain when turned =
off will=20
be about 1 to 2mA - considerably less than the clock in the car. =
Battery=20
discharge will not occur as a result of this very small current, which =
may be
ignored as insignificant.
Construction =20
I recommend that an EDT39 ferrite core is used. These are easy =
to wind,=20
and are capable of around 350W output. Bear in mind that this =
represents a=20
considerable battery current at full power, in the order of 30 to 35=20
Amperes! Heavy transformer windings and supply cables are =
essential, and=20
the input filter must be capable of withstanding this current without =
saturating=20
the core.
The former for these cores is rather large, and you may decide to cut =
the=20
mounting sections off completely. Do remember that the transformer =
must be=20
mounted somehow though, so I suggest that you have a plan. At this =
stage,=20
I am only experimenting, and do not have a plan. I will provide =
details of=20
the solution when I actually have one.
All of Sergio's previous comments apply to this version, so make sure =
that=20
you read his material thoroughly. I do not propose to cover the =
same=20
instructions again, since Sergio has already done an excellent job.
Prototype Testing =20
I have done some initial tests, but have not yet connected the bridge =
and=20
output capacitors. With what was intended to be 12+12 turns on the =
secondary, I obtained an acceptably clean waveform with some overshoot =
with the=20
secondary unloaded. Output voltage was about 38V peak, so I =
obviously had=20
one more turn than I thought I did (input voltage was 14V DC). I =
cannot=20
stress highly enough that the winding process is critical to the success =
of your=20
transformer, and you should expect to have a couple of attempts before =
you get=20
it exactly right. The small number of turns needed makes this much =
easier=20
than would otherwise be the case.
During my testing, my power supply and load became very warm indeed, =
but the=20
MOSFETs (I used IRF540s) remained cool, even though they were mounted on =
a=20
rather small heatsink lying on my workbench. This indicates that =
the=20
heatsinking requirements are easily achievable, but does not mean =
that=20
you can be lax with mounting. My transformer also remained cool, =
with no=20
sign of the core or windings getting even warm. This must be =
considered a
design goal. Even the lead I used to my load became warm, so the =
power=20
output was very real indeed!
You will need an oscilloscope (or at least access to =
one) or=20
the project will be very much harder to build and test. A design =
such as=20
this relies on careful measurements and great care to make certain that =
it will=20
perform as expected. Attempting this without an oscilloscope is =
not=20
recommended.
Please Note:
This project has already created far more questions via e-mail than I =
desired=20
or expected. For everyone who plans on making this supply ... you =
are=20
essentially on your own . I cannot (and will not ) be =
drawn=20
into lengthy e-mail exchanges if you cannot make the supply work.
That it does work if built as described is certain, that you will be =
able to=20
achieve the same results is not. If you do not have (or at least =
have=20
access to) an oscilloscope - don't even think about trying to =
make the=20
supply, as it will not be possible to ensure that the duty cycle of the=20
controller is exactly 50%, or that there is no severe overshoot or =
ringing at=20
the output.
Please do not not send me e-mails asking for =
help. I will=20
simply refer you to this paragraph - I cannot diagnose your problems via =
mail,=20
and will not even try. It is entirely up to the constructor to =
determine=20
his/ her abilities before starting.
The construction of any switching supply is fraught with =
difficulties, risks=20
(including but not limited to elecrocution!) and problems that need to =
be=20
addressed. They are not simple (despite appearances) or easy, and =
there=20
are a great many things that can go wrong. If you are not 100% =
confident=20
that you understand the issues involved, please do yourself a favour and =
build=20
something else instead.
Projects Index Main Index
Copyright Notice. =
This article,=20
including but not limited to all text and diagrams, is the =
intellectual=20
property of Sergio S=E1nchez Moreno and Rod Elliott, and is
Copyright
2002. Reproduction or re-publication by any means whatsoever, =
whether
electronic, mechanical or electro- mechanical, is strictly =
prohibited
under International Copyright laws. The authors (Sergio S=E1nchez =
Moreno
and Rod Elliott) grant the reader the right to use this =
information for=20
personal use only, and further allow that one (1) copy may be made =
for=20
reference while constructing the project. Commercial use is =
prohibited=20
without express written authorisation from Sergio S=E1nchez Moreno =
and Rod
Elliott.
Page =
Created and=20
Copyright
Sergio S=E1nchez Moreno/ Rod Elliott 21 Apr 2002./ Added special=20
note 31 Oct 2002.
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