From: "Saved by Internet Explorer 11" Subject: Switchmode Power Supply For Car Audio Date: Fri, 12 Feb 2016 11:48:01 -0800 MIME-Version: 1.0 Content-Type: multipart/related; type="text/html"; boundary="----=_NextPart_000_0000_01D1658B.3A0CC530" X-MimeOLE: Produced By Microsoft MimeOLE V6.1.7601.17609 This is a multi-part message in MIME format. ------=_NextPart_000_0000_01D1658B.3A0CC530 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Content-Location: file://C:\Users\R&D 1\Documents\Research\Power Supplies\CAR SMPS Design.htm =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 4.62 / 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:

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: =

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


=20
My system's input choke, obtained from an old = PC power=20 supply.

=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. =

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:


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 totalpower = 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!

3D"Figure
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.


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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.
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