From: "Saved by Internet Explorer 11" Subject: Project 101 - High Power, High Fidelity Lateral MOSFET power amplifier Date: Tue, 19 Jan 2016 09:04:16 -0800 MIME-Version: 1.0 Content-Type: multipart/related; type="text/html"; boundary="----=_NextPart_000_0000_01D15298.5FEE1480" X-MimeOLE: Produced By Microsoft MimeOLE V6.1.7601.17609 This is a multi-part message in MIME format. ------=_NextPart_000_0000_01D15298.5FEE1480 Content-Type: text/html; charset="utf-8" Content-Transfer-Encoding: quoted-printable Content-Location: http://sound.westhost.com/project101.htm =EF=BB=BF =20 =20 = =20 Project 101 - High Power, High Fidelity Lateral MOSFET power=20 amplifier =20 =20 =20
3D"ESP=20 =20
 Elliott Sound Products Project = 101 

High Power, High Fidelity Lateral MOSFET Power=20 Amplifier
Rod Elliott (ESP), Updated 21 Apr = 2012

=20 =20 =20
Shar= e |
=20
=20   Please Note:  PCBs are available for this project. = Click the=20 image for details.
Introduction=20

In various parts of The Audio Pages, I have said that I am not a fan = of=20 MOSFET power amplifiers. Well, this amp changed my views, and I consider = this to=20 be a "reference" system in all respects. It uses lateral MOSFETs - not = switching=20 types! The latter cannot be used in this circuit - they will self = destruct! The performance is extremely good, with vanishingly low = distortion=20 levels, plenty of power, very wide full power bandwidth, and the "self=20 protecting" nature of the lateral MOSFETs themselves.

This is not to suggest that the amp is indestructible (no amplifier = can make=20 that claim successfully), but it is much more tolerant of faults than a = bipolar=20 transistor amp, and requires nothing more than a pair of zener diodes to = limit=20 the current. Having said that, I would still recommend that you avoid = shorted=20 output leads and the like - i.e. Don't push your luck =20 )

One thing that emerged during the design is that PCB layout is = absolutely=20 critical. The layout of this new amplifier is similar to that used for = the P68=20 Subwoofer amplifier, and this has some major benefits. P68 has no right = to sound=20 as good as it does, and although designed for subwoofer use, it has = proven=20 during listening and testing to be a very low distortion design - = despite the=20 Class-B output stages. All PCB tracks in the input and driver section = are as=20 short as possible, minimising the chance of noise pickup from other = sections of=20 the circuit - especially noise/distortion generated by the half-wave = signal=20 current handled by each output device.

This MOSFET amplifier is designed to be as flexible as possible, with = no bad=20 habits. Indeed, it will operate stably with supply voltages as low as = +/-5V=20 (completely pointless, but interesting), all the way to the maximum = supply=20 voltage of +/-70V. The only change that is needed is to trim the MOSFET = bias=20 pot!

With the full supply voltage of +/-70V (which must not be exceeded!), = continuous ('RMS') power is around 180W into 8 ohms, or 250W into 4ohms. = Short=20 term (or "music") power is typically about 240W into 8 ohms and 380W = into 4=20 ohms. Note that depends to a very great degree on the power supply, and = a robust=20 supply is a requirement for the maximum output. The recommended supply = voltage=20 is =C2=B156V.=20

As noted, unless you really need the maximum possible power, I = suggest=20 that you use a supply voltage of =C2=B156V obtained from a 40+40V = transformer. You=20 will get around 150W into 8 ohms from this supply voltage, but you also = relax=20 the demands placed on the MOSFETs and heatsinks. The difference between = using=20 =C2=B156V and =C2=B165V is less than 1dB - for the extra peace of mind = and relaxed=20 heatsink requirements that's a very small price to pay.

Since this amp probably has more power than you will normally need, = even if=20 you do skimp a little on the transformer, the loss will be very small. I = must=20 make one thing perfectly clear - this is a hi-fi amplifier. It is not = designed=20 for professional PA use, although this is possible if the supply voltage = is=20 reduced so that both peak and long term dissipation are maintained = regardless of=20 how hard the amp is driven. Although it is quite ok to use with a sub, = P68 is a better proposition in that role. =20

It is worth noting that a MOSFET amp will always produce less power = than a=20 bipolar transistor version using the same supply voltage. Even using an=20 auxiliary supply will make only a small difference (one reason I elected = not to=20 add the extra complexity). A bipolar design using a =C2=B170V supply = can be expected=20 to produce something in the order of 270W into 8 ohms, and well over = 500W into 4=20 ohms. The specified MOSFETs have a rated Vds (saturated voltage, Drain = to=20 Source) of 12V at full current, and that is simply subtracted from the = DC value=20 of the supply voltage. Using a =C2=B156V supply with a lateral MOSFET = amp will always=20 give less power than can be obtained from a bipolar design (see below = for=20 measured figures).

3D"Photo"=20
Photograph of = Completed=20 Amplifier Board (Early Version)

The photo shows the simplicity of the PCB. The MOSFETs are mounted = below the=20 board, and are bolted down in the same way as with the P3A and P68 = boards. No=20 other mounting is needed. PCB pins or tinned copper wire pins are used = as anchor=20 points for the power ground link (the green wire along the front edge), = so that=20 the main current carrying tracks were not compromised by running a = separate=20 track (which would have required a reduction in size of the positive = supply=20 rail).

The entire front-end section is between the electrolytic caps, and is = deliberately as compact as possible. This improves performance, by = ensuring that=20 there are no long tracks for the input stage, which will pick up noise = and can=20 seriously degrade the sound of the amplifier.

Performance Figures=20

The performance of this amp is such that many measurements are very=20 difficult. Some of the more basic measurements are as shown below, based = on my=20 custom made transformers which provide =C2=B165V unloaded. Other than = output power=20 (which will be ~150W into 8 ohms), the figures are virtually identical = with =C2=B156V=20 supplies ...

Parameter Measurement Conditions
Output Power > 180W < 1% THD, 8=CE=A9
> 275W < 1% THD, 4=CE=A9
DC Offset < 20mV Typical
Noise < 2mV RMS Unweighted (-54dBV)
THD 0.015% No load, 30V RMS output, 1kHz
0.017% 8 Ohms, 30V RMS output, 1kHz
0.02% 4 Ohms, 30V RMS output, 1kHz
Output Impedance < 10 m=CE=A9 1kHz, 4=CE=A9 load
< 25 m=CE=A9 10kHz, 4=CE=A9 load
Frequency Response 10Hz to 50kHz At 1W, -1.5dB
Basic = Performance=20 Figures

In particular, the distortion figures show that amp loading causes = only very=20 small variations, with any harmonics being predominantly from my audio=20 oscillator. There are no visible or audible high order components to the = distortion waveform. Output impedance was measured on a fully built = amplifier,=20 including the internal wiring. This entails around 200mm of wire in all = (per=20 channel), so the output impedance of the amplifier itself is obviously = lower=20 than quoted. For an 8 ohm load, the damping factor at 1kHz is around = 800 (8 /=20 10 milliohms) - completely pointless of course, since any speaker lead = will ruin=20 that very quickly.

Noise was measured with inputs open-circuited, and at -54dBV may not = look too=20 wonderful, however this figure is very pessimistic. Remember that this = is the=20 unweighted measurement, with bandwidth extending to well in excess of = 100kHz.=20 Even so, signal to noise ratio (referred to full power) is 86dB = unweighted, and=20 the amp is completely silent into typical speakers. Indeed, even = connecting a=20 pair of headphones directly to the amp outputs revealed that no noise = was=20 audible. Naturally, your methods of construction will differ from mine, = and you=20 may not be able to get the same performance.

Intermodulation distortion cannot be measured with the equipment I = have=20 available, but I have included a screen capture of the three = measurements I=20 took. Most of the harmonic content visible (not that there is a great = deal=20 anyway) is present in the two generators I used, and the amplifier = contributes=20 virtually nothing.

3D"IMD"
1kHz + 2kHz at +30dBV Output (8=CE=A9)

3D"IMD"
1kHz + 2kHz at -25dBV Output (8=CE=A9)

3D"IMD"
10kHz + 12kHz at +20dBV Output (8=CE=A9)

Click on any of the images above for a full resolution version.

Description=20

The very first thing you will notice is that I have broken with = tradition=20 with this amp, and there are no component values shown. Given the = performance of=20 the circuit, and the fact that I have already sold a couple as = completed,=20 finished amplifiers, I am not about to give away all my secrets for the = design.=20 If you want the component values, you must purchase the PCB. There are=20 no exceptions, so don't ask.=20

The schematic of the amp is shown in Fig. 1, and it is about as = simple as a=20 high power MOSFET amplifier can get - it is considerably simpler than = most, but=20 lacks nothing in performance. The circuit diagram belies the ability of = the=20 amplifier though, so do not be tempted to think that it cannot perform = as well=20 as more complex designs - it does, and exceeds the performance of many = (if not=20 most) of them. It will be seen that I elected to use a bootstrap current = source=20 rather than an active version - there is negligible cost difference, but = I was=20 unwilling to make such a radical change after testing the prototype and = being so=20 impressed with the results. (If it ain't broke, don't fix it!)

The front end is a conventional long-tailed pair (LTP) using a = current mirror=20 load and an active current sink in the "tail". Interestingly, adding the = current=20 mirror made no difference to distortion, but reduced the DC offset to = less than=20 25mV. The improvement was such that I elected to retain the mirror.=20

In tests thus far (both measurement and listening), I have been = unable to=20 detect even a hint of what is commonly referred to as the "MOSFET = sound". The=20 relatively high levels of low order distortion and susceptibility to = crossover=20 (or "notch" distortion that plague many MOSFET designs are completely = missing -=20 indeed, even with zero bias on the MOSFETs, crossover distortion = below=20 10kHz is barely measurable, let alone audible!

Note Carefully:
The most critical aspect of the design is = the PCB=20 layout, and it is very doubtful that if you make your own board, that = you will=20 get performance even approaching mine. Power output is essentially = unchanged,=20 but distortion and stability are achieved by a compact and carefully = designed=20 layout for the front end and driver circuits, which minimises any = adverse PCB=20 track coupling that causes much higher distortion levels, and may cause=20 oscillation.

This is not a ploy on my part to get people to purchase my PCBs - = that has=20 already been taken care of by leaving out the component values. The = simple fact=20 is that unless the PCB layout is done with the utmost care, any = amplifier can be=20 made to have far greater distortion levels and reduced stability margins = than=20 the published figures suggest.

Low Power Version
As shown in the schematics below (figures = 1 and=20 2), the amplifier can be made in high or low power version, and although = there=20 is a bit of vacant PCB real estate in the low power design, it is = significantly=20 cheaper to make and will be more than sufficient for most constructors. = If this=20 version is built (using only 1 pair of MOSFETs), IMO it is essential to = limit=20 the supply voltage to =C2=B142V so that it can drive both 4 and 8 ohm = loads without=20 excess dissipation. With this voltage, expect about 100W continuous into = 8 ohms,=20 and around 150W into 4 ohms. Naturally, dual MOSFET pairs may be used at = this=20 voltage as well, providing much better thermal performance (and = therefore cooler=20 operation), far greater peak current capability and slightly higher = power. This=20 version may be used at any voltage from =C2=B125V to =C2=B142V.

3D"Fig
Figure 1 - Standard (Low Power) Version

The MOSFETs used are Hitachi lateral devices, 2SK1058 (N-Channel) and = 2SJ162=20 (P-Channel). These are designed specifically for audio, and are far more = linear=20 than the (currently) more common switching devices that many MOSFET amps = use.=20 Unfortunately, they are not especially cheap, but their performance in = an audio=20 circuit is so much better than vertical MOSFETs, HEXFETs, etc., that = there is no=20 comparison. Note that using HEXFETs or any other vertical MOSFET type is = not an=20 option. They will fail in this circuit, as it was not designed to use = them.

An alternative (and possibly marginally better than the 2SK/2SJ = series) is=20 the Exicon ECX10N20 and ECX10P20 (available from Profusion PLC in the = UK). These=20 have been used in most of the amps I have built, and they work very = well. So=20 potential constructors can verify that the semiconductors are available = before=20 purchasing a PCB, this information has now been included. All other = parts are=20 quite standard. You may also use BUZ901P/BUZ905P devices.

High Power Version
The same PCB is used, but has an extra = pair of=20 MOSFETs. Since the devices are running in parallel, source resistors are = used to=20 force current sharing. Although these may be replaced by wire links, I = do not=20 recommend this. This version may be operated at a maximum supply voltage = of =C2=B170V=20 (=C2=B156V is recommended), and will give up to 180W RMS into 8 ohms, = and 250W into 4=20 ohms. Short term (peak) power is around 240W into 8 ohms and 380W into 4 = ohms.=20 These figures are very much dependent on your power supply regulation,=20 determined by the VA rating of the transformer, size of filter caps, = etc.

3D"Fig
Figure 2 - High Power Version

Although not shown, the transistors and MOSFETs are the same in this = version=20 as for the low power variant. The additional capacitors (C11 and C12) = shown are=20 to balance the gate capacitance. The P-Channel MOSFETs have = significantly higher=20 gate capacitance than their N-Channel counterparts, and the caps ensure = that the=20 two sides of the amp are roughly equal. Without these caps, the amp will = almost=20 always be unstable.

As noted above, the PCB is the same for both versions, but for Fig. 2 = it is=20 fully populated with 2 pairs of power MOSFETs. The high power version = may also=20 be used at lower supply voltages, with a slight increase in power, but=20 considerably lower operating temperatures even at maximum output, and=20 potentially greater reliability.

With both versions, the constructors' page gives additional = information, and=20 the schematics there include an enhanced Zobel network at the output for = greater=20 stability even with the most difficult load. This is provided for on the = PCB,=20 and allows the amp to remain stable under almost any conditions.

The entire circuit has been optimised for minimum current in the = Class-A=20 driver, while still providing sufficient drive to ensure full power = capability=20 up to 25kHz. The slew rate is double that required for full power at = 20kHz, at=20 15V/us, and while it is quite easy to increase it further, this amp = already=20 outperforms a great many other amps in this respect, and faster = operation is=20 neither required nor desirable.

Note - There are actually two caps marked C5, and two = marked C6. This is what is on the PCB overlay, and naturally was not = found=20 until it was too late. Since these caps cannot be mixed up, it will = not cause=20 a problem.

In both versions of the amp, R7 and R8 are selected to provide 5mA = current=20 through the voltage amplifier stage. You will need to change the value = to use a=20 different supply voltage ...=20

R7 =3D R8 =3D Vs / 10 (k)   (Where Vs is one = supply=20 voltage only)
For example, to set the correct = current for=20 =C2=B142V supplies ...=20
R7 =3D R8 =3D 42 / 10 =3D 4.2k (use the next lower = standard=20 value - 3.9k)
Construction=20

As suggested above, I strongly recommend that you purchase the PCB = for this=20 amplifier, or you will almost certainly get results that are nowhere = near the=20 amp's real ability. The PCB also makes construction a breeze, with = everything=20 except the power supply mounted on the board itself. Like many other ESP = power=20 amps, the MOSFETs are mounted underneath the board, requiring only two = (or four)=20 screws to attach the PCB and output devices. As always, full = construction=20 details will be available in the ESP secure site when you purchase the = board(s).=20

Heatsinks for an amp like this are always going to be an issue. Since = the amp=20 is intended for hi-fi use, fans are undesirable, so the heatsink needs = to be=20 substantial. I suggest that you aim for a heatsink with a thermal = resistance of=20 around 0.4=C2=B0C/W for the high power version. It can be somewhat = smaller for the=20 low power version of course, but I recommend that it be no smaller than = ~1=C2=B0C/W.=20

The heatsinks used must have a perfectly flat back, without = any=20 protrusions or anything else that prevents the MOSFETs from making = perfect=20 contact with the heatsinks. The MOSFETs must be electrically isolated = from the=20 heatsink, and you can use thin mica, Kapton (25um) or aluminium = oxide=20 insulators. Do not attempt to use silicone pads - they have far too much = thermal=20 resistance and will result in MOSFET failure.

The suggested power supply is completely conventional. Although a = small=20 amount of additional power can be obtained by using an auxiliary supply = (to=20 boost the rail voltage for the MOSFET drive stage), this is at the = expense of=20 greater complexity and more things to go wrong. The transformer for the = supply=20 should be matched to the expected power you wish to obtain from the amp. = The=20 following table shows the recommended transformer voltage and VA rating = for a=20 single channel - either use two transformers or a single unit with twice = the VA=20 rating shown for stereo.

AC Volts DC Volts VA Power (8=CE=A9)
20-0-20 +/-28V 100 40
25-0-25 +/-35V 100 50
30-0-30 +/-42 160 80
40-0-40 +/-56V 200 150 (Recommended Supply Voltage)
50-0-50 +/-70V 300 240 (Can be used, but not really = recommended)

Note that all powers shown are "short term" or peak - continuous = power will=20 always be less as the supply collapses under load. Peak power levels are = usually=20 achieved (or approached) with most music because its transients are = generally=20 between 6dB and 10dB greater than the average power output. Transformer = VA=20 ratings shown are a guide only - larger or smaller units may be used, = with a=20 marginal increase or reduction of peak power. Always use at least the = size shown=20 for subwoofer use! Values in bold are preferred, and will give enough = power for=20 most systems along with optimum reliability and low operating = temperature.

3D"Fig
Figure 3 - Power Supply Circuit Diagram

Figure 3 shows the power supply circuit diagram for a =C2=B156V = supply, and there=20 is nothing new about it. As I always recommend, the bridge rectifier = should be a=20 400V/35A chassis mount type, and should be properly chassis mounted = using=20 heatsink compound.

Filter capacitors must be rated to at least the nominal supply = voltage, and preferably higher. If possible, use 105=C2=B0C rated caps, = and join the=20 earthed terminals very solidly to form the star earthing point.

Note - The fuse should be selected according to the = size of=20 the power transformer. For any toroidal transformer over 300VA, a = soft start=20 circuit is highly recommended. Use the transformer manufacturer's = suggested=20 fuse - if this information is not available, ask the supplier - = not=20 me!

The DC supply must be taken from the capacitor terminals - never from = the=20 bridge rectifier. Using several small capacitors will give better = performance=20 than a single large one, and is usually cheaper as well. For example, = the=20 performance of 10 x 1,000uF capacitors is a great deal better (in all = respects)=20 than a single 10,000uF cap, at between 50% to 70% of the cost of the = large unit.=20 This lunch is not free, but it is heavily discounted

When you purchase the PCB, you will not only get all component = values, but=20 will also have access to information for a power supply that is = optimised for=20 the best possible performance for a conventional supply. There is = nothing=20 especially innovative about the "advanced" supply schematic, but the = overall=20 results will surprise you.

Testing=20

Connect to a suitable power supply - remember that the supply earth = (ground)=20 must be connected! When powering up for the first time, use 10 ohm to 22 = ohm=20 "safety" resistors in series with each supply to limit the current if = you have=20 made a mistake in the wiring.

For a much more detailed description of the general test processes = (as well=20 as troubleshooting information if the amp does not work), please see the = Troubleshooting = &=20 Repair Guide. That article has much more detailed information than I = can=20 include in each project page.

  =20
3D"Index"Projects=20 Index
3D"ESPMain Index

Copyright = Notice.This=20 article, including but not limited to all text and diagrams, is = the=20 intellectual property of Rod Elliott, and is Copyright =C2=A9 = 2004.=20 Reproduction or re-publication by any means whatsoever, whether=20 electronic, mechanical or electro-mechanical, is strictly = prohibited under=20 International Copyright laws. The author (Rod Elliott) grants the = reader=20 the right to use this information for personal use only, and = further=20 allows that one (1) copy may be made for reference while = constructing the=20 project. Commercial use is prohibited without express written=20 authorisation from Rod Elliott.
Page Created and Copyright =C2=A9 Rod Elliott 07 = Jan 2004./=20 Updated 01 Feb 2004 - added measured results./ 21 Apr 12 - minor page = reformat=20 and added heatsink info.
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