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3D"ESP=20 =20
 Elliott Sound Products Using HEXFETs in High Fidelity=20 Audio 

Using HEXFETs in High Fidelity Audio
Mitch = Hodges
Edited and Updated by Rod Elliott (ESP)
Last = Update:=20 March 2014

=20 =20 =20
Shar= e |
=20
3D"Articles"=20 = Articles=20 Index
3D"Index"Main Index

Contents=20
Introduction=20

When we build linear power amplifiers, we always need to choose some = device=20 for the output stage. This could be any power device including valves, = BJTs,=20 IGBTs, and MOSFETs. Each has its own strengths and weaknesses which = forces us to=20 choose between them. If, perchance, we wanted to build a very simple = and=20 accurate amplifier, we can safely ignore valves, since they all need = heating=20 circuitry and are not simple for a true hi-fi amplifier. That it is = possible to=20 build a valve amp to a high specification is not in doubt, but they tend = to be=20 complex and expensive.

BJTs are often used, but they do not respond well to even momentary=20 overloads. This is because they suffer from second-breakdown - an = instantaneous=20 and catastrophic failure mode. IGBTs (Insulated Gate Bipolar = Transistors) are=20 seldom used, and will be very similar to a BJT, only with an insulated = gate. =20 They still need thermal compensation and a suitable gate drive design, = and can=20 suffer from a 'latch-up' condition in some cases. Lastly there is the = MOSFET,=20 which does not suffer any second-breakdown effects (although this is not = strictly true - see below for = more=20 info). MOSFETs (Metal Oxide Semiconductor Field Effect Transistors) come = in two=20 primary types - vertical and lateral.

These devices are extremely rugged, yet they do have a large = nonlinear gate=20 capacitance to deal with. If driven incorrectly, they show high = distortion=20 levels, especially vertical types - most commonly these days, HEXFETs. = This is=20 why I wrote this article - to show how to use HEXFETs properly in audio=20 applications.

The update=20 below has some important information that I recommend you read = thoroughly and=20 make sure you understand before settling on the use of HEXFETs in your = next amp=20 project. While there appear to be many advantages to their use over = BJTs,=20 HEXFETs may often suffer from exactly the same problems - thermal = runaway and a=20 failure mode that is suspiciously similar to second breakdown. On top of = this,=20 there is a much larger voltage loss ... 2-4V is needed to bias the = HEXFETs to=20 the on condition, vs. 0.65V (nominal) for BJTs. This voltage is usually = taken=20 from the main supplies, so for a given supply voltage, expect a little = less=20 output power.

2 - Description=20

Many people say (including IR) that HEXFETs are not suited for linear = audio=20 circuits and should be avoided. Well, that is the easy route to take = for=20 designing an output stage. Any device can be used for audio and = give=20 great performance if a proper design is found. It is just easier to use = more=20 linear devices. Lateral MOSFETs are usually specified for audio, but = there are=20 relatively few different devices on the market. When found, they tend to = be=20 quite expensive. On the other hand, HEXFETs are very common, reasonably = priced,=20 and only need a good design to do well.

This article is intended for Class-AB designs. HEXFETs will run = Class-A with=20 barely any problems besides driving the gate. If you are designing a = class A=20 amplifier, the first trick (see below) should be used (the second is not = needed=20 since the bias is already quite high).

Alright, now for some explanations. Comparatively, HEXFETs usually = have a=20 low gate capacitance than other vertical MOSFETs, yet have a higher gate = capacitance than their lateral counterparts. There is not only one = capacitance=20 to deal with, but two (one from the gate to source and the other from = the gate=20 to drain). This is the main problem: to find a way to drive the gate=20 capacitance of the HEXFETs. Through a lot of time and molten = breadboards, I=20 found the best two things to design for are the following:

1 Fix: Drive the gates with as much current as possible. This may = include=20 adding a class AB driver stage. =20
Why: HEXFETs have a nonlinear transfer curve up to about an amp or = two,=20 depending on the device(s) used. In a class AB amplifier, this = characteristic is the cause for a majority of the THD. When = driven with=20 enough current, the device will follow the 'new' linear curve, = since it=20 is balancing out the nonlinear gate capacitance. The lower = impedance=20 of the driver stage the better. =20
 =09
2 Fix: HEXFETs like to run hot. This does not mean use an inadequate = heatsink, but the bias between devices should be a bit more than = many=20 are used to. 250mA of idle current is not a bad bias figure for = these=20 devices. =20
Why: To balance out the nonlinear curve, we can simply cut if off = where=20 it seems too bad by using bias. This will increase dissipation, = though.=20

For the design of the amplifier, I will assume a single LTP input = stage. =20 Better performance can be seen by using multiple LTPs, but this will not = be a=20 simple design (in fact it will be quite complex with high frequency = stability=20 issues needing attention).

When choosing the complementary output components, one can obviously = choose=20 the IRFPxxx and its IRFP9xxx complement. If we look at these = complementary=20 device data sheets, we will see very different figures for current = capability,=20 on resistance, and, most importantly, gain (or forward = transconductance). But=20 if we use a matching tool, we will find that the gain varies = considerably from=20 the actual devices vs. the data sheet. That is why we need to buy a few = extra=20 and match them together. Since the gain varies a bit from batch to = batch, it is=20 quite easy to find a IRFPxxx and IRFP9xxx that are very similar, at = least with=20 gain factors.

Also take note that HEXFETs will require a Vbe multiplier for thermal = compensation, since the negative temperature coefficient does not come = into play=20 until the device has about 10 amps through it (at least for the = IRFP240). The=20 exact values around the Vbe multiplier (also known as a bias servo) are = critical=20 to ensure that the thermal performance is matched as closely as = possible.

In every practical design I have tried I had to use a class AB driver = stage. =20 A class-A driver will work fine if you really want an electric heater, = as you=20 will see in the next calculation. Now, in order to size-up the proper = driver for=20 the FETs, we need to do a little maths. I promise it is not hard. An = example=20 would work nicely here ... if we wanted to design a class AB driver = stage with=20 five IRFP240 and five IRFP9240 devices, how much current will we need at = minimum for full functionality up to 50kHz? For a better = understanding,=20 a simplified output stage circuit is shown below.

3D"Figure
Figure 1 - MOSFETs and Driver Circuit

We will do calculations using the gate charge method, which IR = recommends=20 (AN-944). Looking at the data-sheets, we find the IRFP240 has a total = gate=20 charge (Qg) of 70nC and the IRFP9240 has a Qg of 44nC. Don't add these = yet! We=20 will find each device's needs individually. The general formula to = determine=20 gate current is ...

I =3D 100Qgf   where I is = current=20 needed, Qg is the total gate charge in Coulombs, = and=20 f is frequency of operation.

The multiplication factor of 100 gives the headroom needed for = accurately=20 reproducing a square wave (or high frequency sinewave), since the gate = driver=20 needs a lot of current to quickly switch the MOSFET from OFF to ON. = Although the=20 requirement for this is minimal (the CD format is incapable of anything = even=20 approaching a square wave above a couple of kHz), it has become an = expectation=20 that power amps should be able to reproduce perfect square waves at = 10kHz as a=20 minimum.

When we plug our figures in for the IRFP240, we get I =3D 100 *=20 (70E-9 * 50,000) =3D 350mA per device

For the IRFP9240 we get I =3D 100 * (40E-9 * = 50,000) =3D 200mA=20 per device

Multiplying each figure by five (because there are five devices of = each=20 polarity) gives us 1.75 amps for the upper driver and 1 amp for the = lower=20 driver. So a Class-A driver would need bias set to 3.5 amps to get the = job done=20 with a reasonable safety margin.

The value for R7 will depend on the linearity of the driver = transistors. I=20 had to guess and check with my ammeter to get a good value. This can = range=20 anywhere from 100 Ohms up to perhaps 5k. Make sure you check the idle = current=20 before calling the design done! These drivers (Q7 and Q8) may need a = heatsink.=20 Also note the capacitor in parallel with R7. This should be of a high = value=20 (i.e. 100uF or more), and 470uF works fine for my 10 MOSFET stage shown = here. It=20 helps with discharging the MOSFET gates by providing a path for the gate = current.

These current figures seem quite high, but keep in mind this current = will=20 only last a very short time compared to the signal, and virtually no = current is=20 needed to keep the devices either in the OFF or ON state. The current = to=20 reproduce a sinewave will be a bit lower, since it is a smooth curve, = but this=20 much headroom will drastically lower distortion. This is why we cannot=20 practically use a class A driver, unless, of course we use one pair of = output=20 devices.

For some comparison, below is a HEXFET setup driven by a class A = driver at=20 13mA bias:

3D"Figure
Figure 2 - Spectrum of HEXFET with 13mA Class-A = driver

The large notch is at the second harmonic, and the small bump to the = right is=20 the fourth harmonic. Barely any third harmonic is seen. This shows = 0.25%=20 distortion at the second harmonic at =C2=BE power, and 250mA amp bias. = Not very good=20 for a true hi fi, unless we are making a valve-like amplifier. Even = this will=20 not show the same effects as a true valve amp - the nature of the = distortion=20 components will almost certainly be different.

Adjusting the bias to 1 amp removes nearly all distortion, yet now we = are=20 approaching a heater... I mean class A.

After fixing the problem by adding a class AB driver, distortion was = greatly=20 decreased ...

3D"Figure
Figure 3 - Spectrum of HEXFET with Class-AB driver

As the picture shows, the second harmonic was reduced considerably, = while the=20 fourth harmonic is below the noise floor. This shows 0.04% distortion = solely on=20 the second harmonic at =C2=BE power and still with 250mA bias. This = greatly improved=20 the amplifier. At one watt, the distortion is not measurable at all, = unlike=20 with the class A driver. Reducing the gate resistors to 4.7 Ohms to get = more=20 current through does nothing noticeable, so the use of 10 Ohm resistors = is fine.=20 There is no evidence of 'notch' distortion or any other nasty odd = harmonic,=20 only a 'nice' second harmonic added in. Also note that this amp was = built on a=20 breadboard. A compact and nicely wired PCB should decrease distortion = even=20 further.

Below is the final simplified schematic of the entire amplifier = ...

3D"Figure
Figure 4 - Simplified Schematic of Complete HEXFET = Amplifier

It looks very simple, and includes the class AB driving stage to = improve gate=20 driving. It's very simple compared to amps with multiple LTP stages. The = minimum=20 stability network (Zobel) shown is always needed, and a series inductor = (with=20 parallel resistor) may also be required. The values of these components = will be=20 found by experiment.

For some further reductions in distortion, the following work quite = well:

  1. Design a compact PCB layout with feedback taken from as close as = possible=20 to the load terminal. We want to measure what the load is = doing, not=20 what it should be doing.
  2. Don't run any signal wire close to a power supply wire or the = power=20 transformer.
  3. Make big traces on the PCB with decent sized spacing between other = traces.
  4. Make sure your measuring equipment is decently calibrated!
  5. For any output device, use some sort of emitter/source resistors = (as=20 shown) to help balance the load when parallelling.
  6. Use a current mirror with the LTP input to get as much gain as = possible to=20 allow for negative feedback, but do not solely rely on the feedback = to make=20 the amplifier better.
  7. Match the output devices as close as possible, especially for=20 transconductance at low values of VGS.
3 - Conclusion=20

HEXFETs are decent devices once the gates are driven correctly. They = are=20 much more rugged than BJTs as my burned parts pile shows, and sound very = good=20 when a class AB driver is added. I hope this short article with aid = others in=20 using these 'switching' and 'not linear enough for audio' devices to get = distortion figures below many good amplifiers with 'very linear' = devices. And=20 remember one thing - any output device can be precise if a proper = design=20 is found. Finding the correct design parameters becomes more complex = with=20 non-linear devices.

4 - References=20

The following are all PDF files, and are direct links to the = International=20 Rectifier web site ...=20

IRFP240 data sheet
IRFP9240 data sheet
AN-936 application note - The Do's and Don'ts of = Using=20 MOS-Gated Transistors
AN-937 application note - Gate Drive = Characteristics and=20 Requirements for HEXFET=C2=AE power MOSFETs
AN-941 application note - Paralleling = HEXFET=C2=AE power=20 MOSFETs
AN-944 application note - Use Gate Charge to = Design the=20 Gate Drive Circuit for Power MOSFETs and IGBTs
AN-948 application note - Linear Power Amplifier = Using=20 Complementary HEXFET Power MOSFETs

... And many pages from ESP

5 - Footnote=20

The above article is a contribution from Mitch Hodges, and ESP has = not=20 verified all aspects of the design process described. While the circuit = can be=20 (and has been) simulated quite readily with good results, this is no = guarantee=20 that everything will work as expected. I added diodes and zeners to = protect the=20 MOSFET gates from excessive voltage. It may be possible to select the = zeners to=20 achieve basic current limiting, giving the amp some protection from = overload=20 conditions. Because of the high gain of HEXFETs, this simple protection = scheme=20 will not be particularly effective. Also, remember that a series = inductor may=20 also be required.

It will be noted that there are no component values supplied - this = is quite=20 deliberate, and is not an omission. The article is intended to describe = the=20 design process and how to work around the inherent non-linearity of = vertical=20 MOSFETs, and is not intended to be a construction project. Requests for=20 component values will not be fulfilled.

It must be understood that at the suggested current (250mA per MOSFET = pair),=20 the total quiescent current will be in the order of 1.25A - at a typical = supply=20 voltage of perhaps =C2=B150V, this represents a total quiescent = dissipation of 125W!=20 This is a formidable amount of heat to dispose of, and will require very = large=20 heatsinks (and/ or forced air cooling). It is probable that the = constructor will=20 be forced to compromise, using a significantly lower quiescent current = than=20 suggested just to maintain a sensible heatsink size and temperature. = Reducing=20 your expectations of the maximum frequency that needs to be passed at = full power=20 will reduce the loading on the Class-AB drivers, but does nothing for = the MOSFET=20 low current linearity. Compromise will be almost essential (IMHO).

Finally, I'd like to thank Mitch for his contribution, since it = describes the=20 issues and how to solve them in an easy to follow manner, keeping = complexity to=20 the absolute minimum in the final design example.

Rod Elliott
5.1 - Updates (March 2006 & October 2014, ESP) =

I have had occasion to build a HEXFET based power amp as a test for a = client.=20 While it worked well enough, giving the expected power output and with = fairly=20 low distortion, as noted above the required bias current is quite high = to reduce=20 crossover distortion to an acceptable figure. While the circuit I built = was=20 actually quasi-complementary (using only N-Channel MOSFETs), the basic=20 principles apply regardless.=20

As it transpires, the design I was looking at was unsuitable for the = intended=20 purpose, because the quiescent current needed to remove crossover = distortion was=20 too high to be practical. In many cases, the lowest heat output possible = is=20 highly desirable, and HEXFETs are simply unsuited to any application = where very=20 low Iq is desirable or necessary. Lateral MOSFETs would be fine, but are = too=20 expensive for the application (in case anyone was wondering).=20

Bias stability is definitely an issue as discussed above. It is = commonly (and=20 erroneously) stated that MOSFETs are 'safe' because they have a positive = temperature coefficient, so as a device gets hotter, its drain-source=20 (RDS(on)) resistance increases. This much is true, but = this=20 alleged 'benefit' is actually completely useless in a linear circuit. = (It can=20 also cause major problems in switching circuits, but that's another = topic=20 altogether and will not be covered here.)

What is not commonly noted is that all MOSFET devices have a = fairly=20 high negative temperature coefficient for the gate-source = threshold=20 voltage (Vth). At the gate-source voltages needed to = obtain=20 typical bias currents, even a small temperature increase causes a large=20 drain-source current increase, so the use of a carefully designed bias = servo=20 (Q5, R5 and R6 in the Figure 4 schematic) is absolutely = essential. This=20 point is made above, but is sufficiently important that repetition will = not go=20 astray.

To illustrate this, Figure 5 shows the graph from the IRF540 data = sheet, and=20 although it does not continue down to the levels we are interested in, = the trend=20 is clearly visible. At a VGS of 4.5V, we see = ID of=20 around 12A at Tj =3D 25=C2=B0C, rising to a little over = 20A at=20 Tj =3D 175=C2=B0C. While the graph might seem to indicate = that the=20 effect will be greatly exaggerated at lower gate voltages and = drain-source=20 current, the initial tests that I did indicate that the effect is = roughly=20 similar. The graph was taken from the IRF540 data sheet, but has been = colour=20 coded to make identification of each graph easier. The use of source = resistors=20 to help force current sharing is essential, and these should be as high = as=20 practicable. While 0.1 ohms is common for BJT amplifiers, I would = recommend=20 values not less than 0.47 ohms for HEXFETs. Higher values provide more = stable=20 quiescent current with temperature variations. For example, with 1 ohm = source=20 resistors, the current can increase at a maximum of 1mA/mV or 1A/V. = Should=20 Vth fall by 100mV, Iq can only increase by 100mA. This eases = the=20 design of the bias servo.

3D"Figure
Figure 5 - Temperature Coefficient, VGS = (IRF540)

The test I ran was very simple. Apply a suitable voltage to the = drain, then=20 carefully adjust the gate voltage until a suitable measurement current = was=20 drawn. The current started at a relatively low value (around 1A in my = test), and=20 as the device heated up this was seen to rise. It stabilised fairly = quickly=20 because the heatsink prevented further (possibly damaging) heat levels, = but with=20 two MOSFETs in parallel, the current between them was different, and = (more=20 importantly) it remained different, even as they became hotter. The = claims for=20 better (and 'automatic') current sharing apply only to devices operated = as=20 switches, or where the two curves shown in Figure 5 cross over each = other. Only=20 lateral MOSFETs provide a crossover point on their transfer = characteristics that=20 is low enough for linear operation.

Something that is missing from nearly all MOSFET data sheets I have = looked at=20 is gate threshold voltage vs. temperature, although it is shown = in the=20 data I have for the IRF840. This will show that the threshold voltage = falls as=20 Tj increases - a negative temperature coefficient. = The=20 positive coefficient of RDS(on) is insignificant at the = current=20 levels needed for setting quiescent current accurately. Note that the = two curves=20 cross over, but the point where the temperature curves cross is when=20 VGS is at a current of over 40A and the gate-source = voltage is=20 5.5V - this is not useful. Lateral MOSFETs (as used in P101) have = exactly the=20 same issue, but the curve changes from negative to positive at a much = lower=20 current (around 100mA), and this is visible on the transfer = characteristic graph=20 (but you will need to look for it carefully - it is not specified in a = useful=20 manner IMO).

In an application note [=20 1 ], OnSemi describe this transition as the 'inflection' point, and = it is=20 determined by VGS, although it appears to be related more = to the=20 drain current than gate voltage. However, the two are directly related, = so the=20 point is moot. Lateral MOSFETs are usually quite safe here, because the=20 inflection point is at such a low voltage and current, but vertical = MOSFETs=20 (HEXFETs and similar) are prone to thermal runaway. There is also the=20 possibility of a failure mode very similar to second breakdown when = HEXFETs used=20 in linear circuits, where VGS is usually (well) below the = inflection point. This must remain a very good reason to stay clear of = these=20 devices for audio, unless you are fully aware of the potential risks, = and how to=20 avoid them. Note that the article above does not address this potential = failure=20 mode, (nor do many others), and your only choice is to find MOSFETs = where the=20 thermal 'changeover' occurs at the lowest possible drain current. = Lateral=20 devices are almost unbeatable in this respect.

A careful examination shows that the 'inflection' point is actually = the=20 region where the negative temperature coefficient of VGS = exactly=20 compensates for the positive temperature coefficient of = RDS(on).=20 That's the reason it's at such a high current for HEXFETs (because of = the=20 usually low RDS(on) value), and it is known that the = inflection=20 point is inversely proportional to RDS(on). Note = that this=20 only applies if the device is used in linear mode. When switching,=20 Vth and its temperature coefficient is not relevant = because the=20 gate voltage is invariably selected to provide 'hard' switching to = minimise=20 losses.

In contrast, a typical lateral MOSFET (such as the 2SK1058) has an=20 RDS(on) of around 1.5 to 1.7 ohms at ~10A, compared to an = IRF540N=20 with 0.044 ohms at 16A. When choosing HEXFETs for use in linear = circuits, I=20 suggest that you use devices with the highest value of=20 RDS(on) that you can find. This is entirely = counter-intuitive,=20 and is almost certainly the exact opposite of what you would expect.=20 RDS(on) is actually meaningless in a linear application = until the=20 amp starts to clip, and even then only reduces the maximum output power=20 slightly. As a figure of merit, it only has meaning for switching=20 applications.

3D"Figure
Figure 6 - Normalised Vth Vs. Junction = Temperature

From Advanced Power Devices, their application note [=20 2 ] provides the graph shown in Figure 6. Normalising simply means = that=20 everything is taken back to a reference of unity, so simply multiply the = claimed=20 Vth by the figure shown along the left side, for the = temperature=20 at which your device will operate. If your MOSFET will undergo a = temperature=20 change from 25=C2=B0 to 100=C2=B0, then Vth will fall to = 0.83 of the=20 ambient temperature value at 100=C2=B0C. This application note also = mentions the=20 possibility of a failure mode similar to second breakdown when operating = switching MOSFETs as linear amplifiers. The App. Note refers to this = failure=20 mode as 'hot-spotting' or 'current tunnelling', but it's very similar to = traditional second breakdown. Indeed, two of the articles listed below = refer to=20 the fact that using a HEXFET much bigger than needed (to provide a = safety=20 margin) has exactly the opposite effect. Rather than increasing = the=20 safety margin, the larger device is more likely to fail if it is = working=20 well below the 'inflection' current in a linear circuit.

Do not be mislead by claims that MOSFETs are immune from thermal = runaway,=20 although lateral MOSFETs are much better in this respect than vertical = MOSFETs=20 (HEXFETs and similar high-gain switching devices). Based on the above, = it is=20 quite apparent that vertical MOSFETs can easily get into thermal runaway = if the=20 bias servo is not set up correctly. Using just a pot (as shown in P101) = is=20 absolutely forbidden with vertical FETs - a matched bias servo thermally = coupled=20 to the MOSFET heatsink is essential to prevent both thermal runaway and=20 crossover distortion.

Further searching revealed a document from Solid State Optronics [=20 3 ], where the temperature coefficient for VGS is = said to be=20 -1.5mV/=C2=B0C (the above chart shows it as 1mV/=C2=B0C for = VGS of 4.5V at=20 25=C2=B0C). It is claimed to be 'insignificant', and for switching = applications this=20 is true. It is definitely not insignificant for a linear circuit (as = shown in=20 Figure 4), and especially so because of the relatively high = transconductance of=20 vertical MOSFETs. A few (tens of) millivolts of gate voltage is the = difference=20 between acceptable quiescent current and overheating.

What of the second breakdown effect that the manufacturers deny even = happens=20 other than in the (very) fine print? HEXFETs, and indeed most other = MOSFET=20 devices, are made using a multiplicity of individual small MOSFETs = called cells.=20 If the device as a whole exhibits a negative temperature coefficient for = VGS, so must each internal cell. If one cell has a = slightly lower=20 VGS than the others (perhaps due to microscopic = variations in the=20 silicon) it will take more of the total current. This will cause it to = get=20 hotter, so the threshold voltage will fall further and it will then draw = more=20 current, causing it to get still hotter. This process continues until = the cell=20 fails due to over temperature, at which point the MOSFET suffers = catastrophic=20 failure.

While this scenario is not common in switching application, if the = MOSFET is=20 used linearly it is very real, and has caused problems in the past. It = will=20 continue to cause problems if designers are unaware that this failure = mode even=20 exists - after all, most comments seen describe MOSFETs as almost=20 indestructible. While this is true to an extent, it is obvious that it = is not a=20 general rule upon which one should rely in all circumstances. HEXFETs = operated=20 in linear mode need to be derated from the claimed maximum dissipation, = and my=20 suggestion is that a maximum of half the rated power dissipation = is=20 reasonable. Likewise, the peak current should also be much lower than = the rated=20 maximum.

Now you know why International Rectifier and other vertical = MOSFET=20 manufacturers don't recommend HEXFETs or their equivalent for linear=20 applications - they are simply not designed for the purpose. Yes, they = most=20 certainly will work, but you must be aware of the limitations. I suggest = that=20 high voltage, relatively low current devices are preferable to the = reverse, as=20 they will have an inherently higher RDS(on), and = therefore a=20 lower inflection point. Alternatively, you can look for 'vertical' = MOSFETs that=20 are specifically designed for linear operation. They exist, but are = probably=20 considered 'exotic' by most suppliers. An example is the IXYS = IXTK22N100l (with=20 'extended' FBSOA), but=20 at over AU$70 each (one off price) when I looked most people will think = that's a=20 bit rich.

Toshiba used to make vertical MOSFETs that were designated as being = suitable=20 for audio amplifiers. The 2SK1530 and 2SJ201 were basically switching = devices,=20 but with a comparatively high (but unspecified) RDS(on) = of=20 between 0.3 and 0.6 ohms. I've tested an amplifier that used them, and = they=20 perform well enough, but it's doubtful that there was really any = advantage over=20 using bipolar output transistors (other than cost). These devices are = now=20 obsolete, but they were classified for VGS(off), with '0' = classed=20 devices having a threshold voltage of 0.8-1.6V, and 'Y' class with = 1.4-2.8V.=20 This was unique amongst MOSFETs, and I don't know of any other MOSFET = type that=20 has provided a degree of 'pre-matching' when you buy them.=20

If you intend to use vertical MOSFETs for any linear application, you = need to=20 be aware that the published SOA curves do not apply to linear = operation.=20 Feel free to read that again to make sure that you understand the = ramifications.=20 =20

There's little or nothing in the datasheets to warn you, and many = data sheets=20 even show the SOA for DC. A few careful calculations will show that = there is no=20 way that the MOSFET can be operated at full rated power while keeping = the die=20 temperature below the absolute maximum (typically 175=C2=B0C). The only = way that you=20 can be assured of safety is to keep the peak dissipation well below the = claimed=20 maximum, thus minimising the die temperature. This is a minefield, and I = suggest=20 that you tread very carefully. See the IR application note for more = detailed=20 information [ 4=20 ]. =20

Interestingly, some of the earliest MOSFET fabrication processes are = less=20 likely to fail if used in linear mode, because they have a comparatively = high=20 RDS(on). However, most of the early types are obsolete, = and their=20 nominal replacements are 'better' in that RDS(on) is = lower then=20 the previous version(s). While this is good for switching (reduced = losses), it=20 also ensures that they are less suited to linear operation. =20

It's worth looking at RDS(on) for lateral MOSFETs as a = point=20 of comparison. The figure isn't quoted, but it can be calculated using = the=20 Drain-Source saturation voltage figure provided. VDS(sat) = will=20 normally be in the order of around 12V (gate shorted to drain) at a = current of=20 7-8 amps, so RDS(on) is in the order of 1.5-1.7 ohms! = Compare=20 that with the figures you see for HEXFETs - the IRFP240 has an=20 RDS(on) of 0.18 ohm, but it's also important to = understand that=20 completely different test methods are used so a direct comparison isn't = as easy=20 as it seems.=20

One thing that is a dead giveaway as to whether a MOSFET is lateral = or=20 vertical is to compare the pinouts. Lateral MOSFETs have the = source pin=20 in the centre, while vertical types invariably have the centre pin as = the=20 drain.

3D"Figure
Figure 7 - Vertical Vs. Lateral MOSFET Pinouts

As far as I'm aware, there are no exceptions to the above. There are = very few=20 lateral MOSFETs in the TO-220 case, and all true lateral high-power = MOSFETs use=20 the TO-247 case or a small variation thereof. It's worth noting that the = TO-220=20 package is useless (regardless of what's inside) for getting rid of any = more=20 than about 20W worth of heat, unless extraordinary care is taken with = mounting.=20

As should now be quite obvious, it's very hard to recommend using = HEXFETs in=20 an audio amplifier. Mitch has made a compelling case, but much has = changed since=20 the article was written, and there is also more information available. = This=20 won't stop people from trying, because HEXFETs are cheap compared to = lateral=20 MOSFETs and high power bipolar transistors, and seem to offer = many=20 advantages. As is now clear (I hope), most of the 'benefits' are an = illusion,=20 and can easily lead to tears if the warnings here aren't heeded.

References

1   On Semiconductor - AND8199
2   Advanced Power Technology - = AN0002 - no longer found at the source, but now = available=20 from the ESP site
3   Solid State Optronics - Application Note 50
4   International = Rectifier -=20 AN1155=20
  =20
3D"Index"Main Index
Articles Index

Copyright Notice. = This=20 article, including but not limited to all text and diagrams, is = the=20 intellectual property of Rod Elliott and Mitch Hodges, and is = Copyright =C2=A9=20 2006. Reproduction or re-publication by any means whatsoever, = whether=20 electronic, mechanical or electro- mechanical, is strictly = prohibited=20 under International Copyright laws. The author (Mitch Hodges) and = editor=20 (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. Commercial use is prohibited without express written=20 authorisation from Mitch Hodges and Rod = Elliott.
Page created and copyright =C2=A9 15 Jan 2006./ = Updated 13 March=20 2006 - Added update with thermal characteristic data and additional = caveats./=20 Mar & Oct 2014 - further updates on HEXFETs used in linear=20 mode.

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