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 Elliott Sound Products MOSFET = Relays 

MOSFET Solid State Relays
Rod Elliott - = =A9 2012

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Shar= e |
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3D"Articles"Articles Index
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Contents=20
Introduction=20

Solid-State relays (SSRs) for AC have been around for as long as the = first=20 SCRs and TRIACs became available. However, none of these early devices = was=20 suitable for use with audio signals, because of gross distortion around = the=20 zero-crossing point of the waveform. MOSFET based SSRs have existed from = around=20 1984, when a patent was taken out by International Rectifier Corporation = for a=20 MOSFET circuit that could handle AC with very low distortion. [1]. = It is not known if this is the earliest example, but it's probably = close.=20

There are any number of SSRs available that are suitable for DC, but=20 comparatively few low-distortion types that can handle the high = AC=20 voltages and currents that are typical of high power amplifiers. Those=20 commercial devices that might be electrically suitable will most likely = do some=20 serious damage to your bank account. There are a many that can handle up = to=20 around 2.5A at voltages as high as 600V, but comparatively few that can = handle=20 the 30-40A or so that is needed for a high power amplifier driving low = impedance=20 loads.=20

While conventional relays can be used, they have a small problem ... = when a=20 high power amplifier fails and the output goes DC, there could be 100V = or more=20 with a load impedance of perhaps 4 ohms or less. Breaking 100V at 25A DC = is a=20 very difficult job for a relay, because the DC allows a substantial arc = to be=20 created across the contacts.=20

This arc is very difficult to stop, and the only way to actually = protect the=20 speaker is to earth the normally closed contact so that the arc is = connected to=20 the power supply common rail (earth/ ground). The relay will be = destroyed, but=20 the speakers will (probably) survive. Most mains rated = electro-mechanical relays=20 are limited to around 30V DC, but even with this seemingly low voltage = it is=20 still likely that the relay will be damaged if it ever has to protect = the=20 speakers.


Figure 1 - Conventional Relay Wiring

The above shows the wiring scheme that must be used to protect = the=20 loudspeaker. The earth connection is often neglected in 'protection' = circuits=20 shown on the Net, and the end result is that while it may happily pass = your=20 basic tests, it will likely fail when you really need it due to the DC = arc.=20

Perhaps due to the known problems with electro-mechanical relays, = there seems=20 to be some interest in solid state relays on audio forum sites, but = while some=20 of the information is actually quite good, there are many misconceptions = and=20 often a failure to understand the things that can go wrong.

Note that the DC detector and control circuit (not shown - see = Project=20 33 for an example) must be connected directly to the=20 amplifier's output. If it's connected after the relay, fault = induced DC=20 will only be present when the relay is closed, so your speakers = will be=20 subjected to repeated pulses as the relay closes, DC is sensed, = and the=20 relay opens again. This process will continue until you switch the = amp=20 off.

When the detector is connected to the amp output, the = relay=20 will never close because the fault condition is detected before = the=20 detector attempts to connect the speaker.
1   MOSFET Relay Principle Of Operation=20

The general idea of an AC SSR is shown in Figure 2. Two N-Channel = switching=20 MOSFETs are used, with their sources and gates joined. The signal and = load are=20 connected to each of the drain terminals - it doesn't matter which is = which,=20 because the 'switch' is symmetrical. =20

With no voltage between the gate and source terminals, the MOSFETs = are off,=20 so no current flows. Depending on the MOSFETs used, they will conduct = fully when=20 the gate-source voltage exceeds around 7 Volts. It is always a good idea = to=20 provide 10-12V gate drive to ensure that they always turn on fully. The = zener=20 diode you see is to protect the delicate insulation between the gate and = MOSFET=20 channel.=20

The gate insulation is typically rated for a maximum of around = =B120V. Even a=20 little bit of stray capacitance or resistance (moisture on the PCB for = example)=20 can easily allow the voltage to rise to destructive levels because of = the very=20 high impedance, and the zener is mandatory.=20

While the concept is very simple, in practice there may be quite a = lot of=20 additional circuitry needed because the control circuit must generally = be=20 completely isolated from the switching MOSFETs. Two complete circuits = are needed=20 for stereo, even if they are driven by the same detector. This is = because the=20 two pairs of MOSFETs cannot be connected together in any way, other than = sharing=20 a common control drive circuit such as a dual optocoupler or miniature = double=20 pole relay.=20

In addition, the MOSFETs used need to have a very low RDS = (on), or=20 multiple smaller units used. The lower the value of drain-source = resistance, the=20 lower he distortion contributed by the circuit. Note that each MOSFET's = voltage=20 should be rated for at least 25% more than the supply rails of the = amplifier=20 with no load. This is due to the way the circuit works, and because of = the=20 possibility of instantaneous back-EMF from the speaker coil when the DC = fault=20 current is suddenly interrupted. It may be useful to include a MOV = (metal oxide=20 varistor) across the SSR switch terminals, or use a capacitor 'snubber' = to=20 prevent the likelihood of any destructive voltage spike. The latter is = shown in=20 Figure 2, along with a pair of 'catch' diodes (D2 and D3) that connect = to the=20 amp's supply rails. (Note that the diodes are also included in other = drawings,=20 as it is very important that they be included.)=20

When MOSFETs fail, they almost invariably fail short-circuit (like = most=20 semiconductors), and it is conceivable that a failure could go entirely=20 unnoticed until your speaker catches on fire. It is essential to make = sure that=20 failure is rendered highly unlikely, or that some kind of test process = be=20 incorporated (which adds further complexity of course). Quite obviously, = a=20 conventional relay can fail too, but they are generally extremely = reliable and=20 have no sensitive electronic bits in them.


Figure 2 - Basic MOSFET Relay

What we need to activate the MOSFET relay is a floating DC source. It = must be=20 electrically isolated from the amplifier's speaker output (and with high = impedance) or it will either be damaged by the amp, or will damage the = amp. For=20 simplicity, the DC source is shown as a 9V battery (discussed further = below).=20 Then the DC is connected and disconnected as needed to switch the relay = on and=20 off (shown above by a switch). There are any number of different ways to = implement the switching function, ranging from miniature relays, = opto-isolators=20 (either LED + LDR or LED + photo transistor) or by remotely turning the = gate=20 supply on and off by some means. The zener is used to ensure that the = voltage is=20 kept below that which may damage the gate's sensitive insulation. =20

As noted above, the MOSFET voltage rating needs to be at least 20% = more than=20 the supply voltage. If you have =B1100V supplies, the MOSFETs should be = rated for=20 at least 120V, as this provides a comfortable safety margin. You can add = resistors in parallel with each MOSFET, which reduces the effects of = stray=20 capacitance and ensures that your safety margin is maintained. 100k is a = good=20 place to start, but this isn't strictly necessary (especially with the = relay=20 circuit shown in Figures 7 and 8). The likelihood of excessive voltage = is most=20 likely with the 'charge coupled' circuit in Figure 6.=20

Capacitance from the speaker output to earth must also be minimised, = or there=20 is a risk that the amp may oscillate. Ideally the floating supply should = be=20 isolated from any stray capacitance by series resistors. These damp the = effect=20 of the capacitance and render it harmless. Where an output coil is = fitted to=20 isolate the amp from speaker cables and other stray capacitance, the SSR = should=20 be between the coil and speaker terminal - never between the amp and = coil.=20

Note that the MOSFET switch is completely bidirectional, and although = it may=20 seem that it must introduce considerable distortion, this is actually = not the=20 case. When the switch is closed and the MOSFETs are biased on, the only = voltage=20 that appears across the pair is due to their on resistance (RDS=20 (on)). With suitable devices, this resistance is very low and = reasonably=20 linear. Linearity is not as good when the 'switch' is off, but that's of = little=20 consequence. Bear in mind that any series resistance reduces damping = factor, so=20 if you happen to think that very high values are essential, you may be=20 disinclined to add a circuit that adds resistance. =20

The choice of suitable MOSFETs is huge - so much so that I'll only = attempt a=20 couple of types for consideration. A popular and inexpensive part is the = IRF540N. It's rated at 33A with a voltage rating of 100V, so it can be = used with=20 supply voltages up to about =B170V. Another worth considering is the = IRFP240, 200V=20 and 20A. RDS (on) is higher than desirable, but 2 or more can = be=20 paralleled to reduce that. There are many others, and I leave it to the = reader=20 to find a device that suits the purpose and the budget. =20

I've shown IRF540N devices in the circuits, but that's only a = suggestion.=20 RDS (on) is quoted as 44mΩ for these MOSFETs, so the = total series=20 resistance will be 88mΩ, or 0.088 ohm. With an amp current of (say) = 20A peak,=20 there will be a loss of 1.76V peak (1.25V RMS) across the relay, and a = total=20 power dissipation of less than 150mW.=20

Note that while it would be very convenient (and easy) to use a = battery as=20 shown in Figure 2, that would be a really bad idea. Even though the = MOSFET gates=20 require minimal current, the battery will eventually discharge to the = point=20 where a significant voltage will appear across the MOSFETs because they = are not=20 switched on hard enough, and this will cause severe overheating and = gross=20 distortion. As an example, the circuit shown above has a distortion of = 0.013%=20 with 28V AC applied (a 100W/ 8 ohm amp at full power). =20

Should the MOSFET gate bias voltage be reduced to 5V, the maximum = output is=20 dramatically reduced, and distortion becomes excessive at any level = above around=20 50-60W. In addition, the MOSFETs will overheat badly, because normally = they only=20 need a very modest heatsink (if any at all). Once there is a significant = voltage=20 across them and they are passing current, they will dissipate power. =20

Having ruled out using a couple of 9V batteries (at least from a = purely=20 practical perspective), we have to find an alternative solution to = provide the=20 necessary voltage needed to switch the MOSFETs on. Switching them off is = easy -=20 just take away the voltage. Some of the options are as follows in the = next=20 sections.=20

Note that if you use a cap across the relay terminals as shown, there = will be=20 a small signal current that will be audible with high sensitivity = speakers.=20 Provided the 'clamp' diodes are used, the cap can be omitted, or you can = use a=20 MOV for protection. If used, the MOV must have an RMS voltage rating = that is=20 less than the rated breakdown voltage of the MOSFETs, but = greater=20 than the amplifier's RMS output voltage. Given that MOV devices have a = rather=20 broad tolerance and are only available with a limited range of voltages, = this=20 makes selection rather difficult.

2   Photo-Voltaic Opto-Couplers=20

Several manufacturers make photo-voltaic MOSFET drivers that seem = ideal (they=20 use an infra-red LED and a bank of photovoltaic-diodes or tiny "solar = cells" to=20 generate the gate voltage) [2]. = While they can be obtained fairly cheaply (less than $10 if you find a=20 supplier), a few problems exist. They are ...=20

The final issue is the one that is likely to cause some grief, = because most=20 have an output current that's less than 100uA, with some below 10uA. = This means=20 that the MOSFETs cannot be switched quickly (on or off), so peak power=20 dissipation may be unacceptably high during switching. Remember that all = MOSFETs=20 have a gate-source capacitance that must be charged and discharged when = the=20 MOSFET is switched on and off. Although this must be considered, it is = still=20 possible to get switching times in the order of a few milliseconds, and = this=20 will generally be considered acceptable.=20


Figure 3 - Photo-Voltaic MOSFET Driver

The arrangement shown above is fairly typical of the general scheme, = and will=20 work very well provided the optimum photovoltaic optocoupler can be = found at a=20 sensible price. Ideally, you will need a photovoltaic opto that can = provide at=20 least 50uA or switching times become embarrassingly slow. In some data = sheets=20 (and included above) you will see a JFET used to speed up the MOSFET's = gate=20 discharge and turn-off time. As shown, turn-off is almost instantaneous. =

This arrangement can also be seen if you have a look at the Vishay = VO1263AB=20 data sheet, but they use a P-Channel JFET. It is pretty much mandatory = to=20 include the JFET if you choose to use the photovoltaic isolator circuit, = unless=20 you use the circuit shown in Figure=20 9. In other circuits you might come across, a high value resistor = (~10MΩ) is=20 placed across the isolator's output, but this has a much longer = turn-off=20 time (perhaps 100ms or even more, depending on MOSFET gate-source = capacitance).=20 This will almost certainly cause excessive peak dissipation in the = MOSFETs and=20 lead to failure.=20

The opto's LED typically needs to be driven with around 10-50mA to = work,=20 depending on the device used. This current is easily supplied by the = speaker DC=20 detector circuit. Project=20 33 can do the job easily.=20

In case you are wondering, the JFET circuit shorts the MOSFET gate to = source=20 when there is no current from the opto. When the opto is active = (supplying=20 current), a voltage is developed across R2 that biases the JFET off, so = it does=20 not draw any current. With 50uA and a 2.2M resistor, the JFET is biased = fully=20 off. Because of the wide parameter spread of JFETs and photovoltaic = isolators,=20 you may need to experiment with the value of R2 to ensure reliable = switching.=20

It is important to understand that there will be some voltage drop = across R2,=20 sufficient to bias the JFET off. This voltage is unavailable to the = gates of the=20 MOSFETs, so the already limited voltage from the coupler is reduced a = little=20 more. This may be enough to not allow the MOSFETs to conduct fully, a = highly=20 undesirable outcome. The extra resistance also means that the MOSFETs = turn on=20 slower than they otherwise would. The difference is not great, but is = easily=20 measured.

3   Transformer Drive=20

Using a small transformer is a good solution, and it only requires a = simple=20 rectifier and minimal filtering to drive the MOSFET gate. Since the = transformer=20 can easily supply 10mA or more, switching times are dramatically = reduced.=20 Unfortunately, a transformer coupled circuit also needs a driver circuit = to=20 provide a signal at the secondary (or secondaries). This should operate = at 50kHz=20 or more to minimise the size of the transformer(s). Not really a = problem, but=20 there's more circuitry needed which takes up potentially valuable = space.


Figure 4 - Transformer Based MOSFET Driver

An example is shown above (just one of a great many possibilities), = based in=20 part on the original patent [1], = but somewhat simplified. While it's not overly complex, there are = nuisance=20 issues like finding a suitable transformer that have to be solved. It = will=20 generally be easier to find single secondary winding transformers, so = two will=20 have to be used for a stereo system. If a single transformer with dual=20 secondaries is used for a stereo amp, the insulation between the primary = and=20 also between both secondaries has to be able to withstand the full = amplifier=20 supply voltage. This means that if the amp uses =B160V supplies, the = insulation=20 has to be rated for at least 120V. It would be wise to ensure that all=20 inter-winding insulation is rated for a minimum of 500V.=20

The drive signal typically needs to be a squarewave of no less than = 15V=20 peak-peak. The advantage of using a voltage doubler is that there is a = small=20 parts saving - the caps that form part of the doubler also smooth the = DC.=20 Without the doubler, either the drive voltage has to be increased or the = transformers have to be step-up types to obtain enough gate voltage.=20

Note that the diodes (D1 and D2) must be high speed types, preferably = Schottky or at least 'ultra-fast' types. Normal diodes are far too slow = and will=20 cause very high losses in the rectifier - so much so that it may not = even work.=20

The drive oscillator can be almost anything you like, but as noted on = the=20 circuit diagram above, you need at least 15V P-P drive voltage, at a = frequency=20 of around 50kHz. Current is fairly low at 45mA RMS for a transformer = with 500uH=20 primary inductance. Depending on the transformer you use, the current = may be=20 somewhat higher. There is no point trying to specify particular cores = and=20 formers, as their availability is highly variable - parts I can get here = may be=20 unavailable elsewhere and vice-versa.=20


Figure 5 - Typical Oscillator

The oscillator shown above is the simplest possible arrangement using = a 555=20 timer, but is perfect for this application. The output signal is close = to a=20 squarewave, and any small variation in duty cycle is handled by the = capacitor=20 feeding the transformer. This prevents any DC magnetic flux build-up = that may=20 cause the transformer to saturate. There are countless other oscillator = designs=20 that will also work, but few that are quite as simple as the one shown.=20

When the CTRL line is open circuit or high, the oscillator runs, and = gate=20 voltage is available to the MOSFET relay which turns on. When the CTRL = line is=20 pulled low, the oscillator stops and the MOSFETs also turn off once the = gate=20 caps discharge. It is possible to incorporate additional circuitry to = ensure the=20 relay turns off very quickly, but in reality anything up to a few = milliseconds=20 will be alright in most cases. A simulation tells me that as shown, it = will=20 switch off in under 1ms.=20

You may also be able to use small 'output' transformers intended for = low=20 power transistor amplifiers (portable radios for example). These provide = another=20 option - just use the core and bobbin. Remove the existing primary and=20 secondary, and wind new ones by hand. The inter-winding insulation = layers can=20 easily be improved to suit the new requirements. We are not overly = concerned=20 with efficiency, because the power needed is negligible. Unless you have = access=20 to small ferrite cores, this is likely to be the cheapest option.=20

As an alternative to using discrete circuits, it is also possible to = use=20 miniature DC-DC converters to provide both isolation and gate drive. = This is a=20 more expensive option though, since most of these small converters are = at least=20 $15 each, even in quantity. You will have to use transistor output = optoisolators=20 if you use any kind of power supply module, or it will take far too long = for the=20 voltage to fall to the point where the MOSFETs turn off.

4   Capacitive Drive=20

There is the option of doing away with the transformer(s), and simply = using=20 low value capacitors to couple a high frequency AC signal to a rectifier = circuit=20 that then drives the MOSFET gates [3]. = This arrangement is also known as a 'charge-coupled' circuit, and can = use the=20 same oscillator as shown above. Although the data sheet says that a 555 = timer=20 can operate at a maximum frequency of around 500kHz, I wouldn't be happy = with it=20 running that fast. Up to 250kHz should be fairly safe though.=20


Figure 6 - Capacitive-Coupled MOSFET Driver

Like the transformer solution, an oscillator at 50kHz or more is = needed, and=20 the coupling caps are so small that they will pass very little signal in = the=20 audio range. At the high switching frequency, the caps are almost a=20 short-circuit, and can fully charge the gate driver within a couple of=20 milliseconds. Current is quite low though, depending on the switching = speed and=20 capacitor value. High speed Schottky diodes are essential, as I would = normally=20 expect that switching frequencies well in excess of 100kHz be used. In = the=20 circuit shown above, the circuit can supply around 300uA, but can still = switch=20 MOSFETs on or off in a few milliseconds. The capacitors used should be = rated for=20 at least 600V DC.=20

The primary disadvantage of using capacitive drive is that the amp's = output=20 must be limited to no more than perhaps 25kHz or so. Should the amp = decide to=20 oscillate, there is a real chance that the capacitive driver circuits = will be=20 damaged. This will happen if any amplifier output frequency (intended or = accidental) is high enough to pass a signal back from the speaker line = to the=20 driver circuit.=20

In addition, the voltage across C2 increases with increased amp = output=20 frequency, because the caps (especially C1) pass some of the signal and = this=20 assists the charging process. The only way to avoid this is to use a = higher=20 oscillator frequency and a smaller value for C1 and C3. For example, = with an=20 oscillator frequency of 500kHz and C1 and C3 reduced to 470pF, an = amplifier=20 signal of 25kHz at full power causes no increase in the normal voltage = developed=20 across C2. Also note that although the RMS drive current is only around = 5mA, the=20 peak value is over 30mA with the values shown.=20

Switching times are passable. While turn-on is quite fast at about = 1ms,=20 turn-off is rather lethargic - it takes just over 3ms for the MOSFETs to = turn=20 off with the values shown, so dissipation under fault conditions will be = rather=20 high. Although turn-off time can be improved by reducing the value of = R3, this=20 demands a higher drive signal (either higher voltage or frequency).=20

For the reasons described above, I do not consider this a usable = approach for=20 an audio amplifier. There are too many factors that make it unsuitable. = It can=20 be used for switching mains (50/60Hz) without any problems though.

5   Stand-Alone Floating Power Supplies=20

The final option is to use conventional small power supplies that can = have=20 their outputs fully floating. A small transformer with dual secondaries = is one=20 possibility, but there is a real risk that the insulation between = windings will=20 be unable to withstand the output voltage swing from powerful stereo = amplifiers.=20 When doing some initial tests, I used a 12V DC switchmode plug-pack (aka = 'wall-wart') as the voltage source (it's actually built-in as part of my = workbench system, but that's irrelevant).=20

A small 50/60Hz transformer with dual windings can be used, having a=20 conventional rectifier and filter cap on each output. As with the = transformer=20 drive approach, inter-secondary insulation has to be up to the task. = This is=20 actually rather unlikely, so it's hard to recommend this approach - it's = much=20 safer to use two transformers, but that gets bulky and rather costly. = The DC to=20 the MOSFET gates is simply switched using optocouplers with transistor = outputs=20 as demonstrated in Figure 7. =20

This kind of approach certainly works, but the cost and space is such = that=20 you'd be a lot better off financially by using miniature DC-DC = converters. It's=20 hard to recommend the use of separate mains powered supplies as it is = somewhat=20 clumsy, physically large and comparatively expensive. However, it does = offer a=20 simple and easily implemented solution, with the minimum number of = electronic=20 bits to fail.

6   Power Rail Supply=20

This arrangement perhaps doesn't really look like it could work, but = that's=20 an illusion. By taking a diode blocked resistive feed from the positive = supply,=20 the DC is stored in C1 and because of the high impedances will hold up = well even=20 at low frequencies. C1 can't discharge back through the resistor when = the=20 amplifier's output voltage swings fully positive because the diode = prevents=20 this. Note that there is some modulation of the supply, but this = is=20 smoothed by the zener as it simultaneously protects the MOSFET gates. = The zener=20 is absolutely essential in this arrangement (but should always be used = anyway),=20 because without it the voltage can rise to the full DC supply - gate = destruction=20 is a certainty. R4 is optional but recommended. The cap will charge = whether it's=20 there or not, as long as the amplifier or speaker remains connected (the = MOSFETs' internal diodes provide the current path).=20


Figure 7 - Supply Rail Gate Bias

As shown, the supply resistor (R2) does provide a small DC offset = current to=20 the speaker when the SSR is turned off, but at less than 2mA with 60 = volt=20 supplies it can be ignored. This is by far the simplest way to obtain = the=20 necessary DC to keep the MOSFETs turned on. To switch them off, you may = use an=20 opto-coupler as shown, or even a small relay can be used. Note that R2 = and R4=20 are suitable for supply voltages up to around =B150V. Higher values will = be needed=20 if the amp uses higher voltage supply rails. R4 can be connected to the = -ve=20 supply instead of earth if desired, but there's little point - the = circuit won't=20 work any better by doing so.=20

This circuit has the advantage of great simplicity compared to the = other=20 methods described. There is no need for an oscillator or transformers, = no=20 rectifiers or high speed diodes, and no side issues with high = frequencies.=20 Because of the continuous supply and use of an optocoupler, the turn-off = time is=20 also very fast. Turn-on speed is determined by the value of R3 and the = MOSFET=20 gate-source capacitance. We don't need sub microsecond switching, and in = most=20 cases the values shown will be more than acceptable.=20

It's also worth noting that the circuit doesn't actually have to be = powered=20 from the amp's supply rail. Any positive voltage source of 15V or = greater is=20 enough to allow the relay to turn on and remain on until the = optoisolator turns=20 it off again. It may be helpful if R2 is reduced to suit the lower = voltage -=20 about 22k is fine, but you might need to experiment a little. The second = 'feed'=20 resistor (R4) should be the same value. You may need to use 1W resistors = with=20 high power amps.

Note, however, that there are contra-indications to this = technique.=20 When used as shown and in the 'off' state, there is a small = charging=20 current that is rectified by the diode D1 and the MOSFET's = intrinsic=20 internal diode. When the cap is used in parallel, this tends to = swamp the=20 very small but highly distorted leakage current that flows each = time the=20 diodes conduct. While R2 (the bias feed resistor) does reduce the = noise,=20 you will hear a low-level distorted signal across the speaker - = especially=20 if the circuit is connected as shown in Figure 8. The capacitor = (C2) tends=20 to swamp this to a degree, but that allows even more signal to = pass.=20

None of the above affects the relay's ability to disconnect the = speaker=20 if DC is detected, but is something you need to be aware of. The=20 distortion component of the muted signal is especially audible if = you=20 choose to use a feed voltage that's less than the full amplifier = supply=20 voltage, and you have very sensitive speakers such as horn = compression=20 drivers. For this reason, the MOSFET relay is not really suitable = as a=20 signal mute - this should be done at the amp's input or from the = mixing=20 desk.

BEWARE! - the relay's default state is ON! The external circuitry = turns the=20 relay off, but if the supply to the detection circuit is not present=20 before the amplifier supply rails start to rise, DC can be fed to = the=20 speaker until such time as the detection circuits function and = disconnect the=20 load. This is easily circumvented by some additional circuitry or by = leaving the=20 detector permanently powered ... with the proviso that the amp = cannot be=20 turned on at all if the relay supply is not present!=20

For example, you could use P39 (soft start circuit), and use its power supply = to power=20 the detector (such as P33=20 which powers the optocoupler), as well as the soft start. While this = adds some=20 complication, a high power amp needs soft start anyway, so it's not = necessarily=20 a big deal.

7   MOSFET Relay In Speaker Return=20

It is possible to design the overall circuit so that the power supply = constraints are reduced. Instead of placing the MOSFET relay in series = with the=20 amp's speaker output, simply connect it between the speaker common = terminal=20 (normally PSU earth/ ground) and the actual PSU earth bus. Now the = entire=20 circuit has one terminal that is earth referenced, which reduces the = isolation=20 requirements between the separate power supplies. However, when switched = off,=20 the centre-tap between the two MOSFETs can easily reach a voltage that = still=20 demands good insulation of any floating supply (roughly 1/2 the +ve = supply=20 voltage). The diode shown in Figure 7 (in series with R2) is not needed = in the=20 earth-referenced circuit shown below, because C1 cannot discharge when = the amp's=20 output swings positive - the junction between MOSFETs is at (close to) = zero=20 volts when the MOSFET relay is on.


Figure 8 - MOSFET Relay Circuit In Earth Line

Needless to say, this method cannot be used with BTL (bridge tied = load) amps=20 regardless of bias supply type, because each side of the speaker is = driven by a=20 separate amplifier driven 180=B0 out-of-phase with the other. Both = speaker=20 terminals are therefore 'live' with the amplified signal, so a fully = floating=20 system is definitely required. Even if you do decide to connect your = MOSFET=20 relay in the earth end of the speaker (i.e. the speaker return), I still = recommend that the power supplies are properly isolated or you may have=20 unforeseen problems (assuming that you use one of the other methods = shown, not=20 the one in Figure 8). I don't know what they might be, because they = are=20 unforeseen =20

Another potential issue is the added resistance in the speaker line, = and that=20 will reduce 'damping factor' (assuming that you consider it to be = important) and=20 output power. Any voltage and current combination that appears across/ = through=20 the MOSFETs also causes heating. For these reasons, using MOSFETs with a = very=20 low RDS (on) is essential. The lower this resistance, the = less=20 distortion the circuit contributes as well.=20

It is possible to use a conventional relay in parallel with the = MOSFET relay,=20 so that there is no added series resistance. In the case of a fault, the = relay=20 must open first, followed by the MOSFET relay. This process will add an=20 inevitable delay, because you must allow sufficient time to allow the=20 electromechanical relay to be fully open before the MOSFET relay opens. = The=20 control system will also be far more complex, with more things to go = wrong.=20

It is also very important to ensure that the capacitance of the power = supply=20 (when connected in the 'live' speaker line) does not impose enough = capacitance=20 to cause the amplifier to oscillate. Most amps get very upset if the = output sees=20 around 10-100nF directly to earth, so consider including 100 ohm = resistors in=20 series with the power supply as shown in Figure 4.=20

Based on simulations and some tests, distortion can be expected to be = well=20 below 0.1% unless you don't have enough gate voltage or RDS = (on) is=20 too high. Remember that there are two sets of RDS (on) in = series with=20 the speaker, so maintaining a very low figure for each MOSFET is = essential. It=20 may be necessary to use two or more MOSFETs in parallel on each side of = the=20 switch to keep the insertion loss as low as possible. For a high power = amp, even=20 0.1 ohm represents a significant power loss, and that power is turned = into heat=20 in the MOSFETs. Any increase in temperature further increases RDS=20 (on), causing higher losses and more heat. Thermal runaway is = possible if=20 the MOSFETs are not sized correctly.

8   Final Approach=20

The solution that you eventually use will be determined by a number = of=20 factors, including space, cost and switching speed. As always, there are = trade-offs that must be made in any design to get a final circuit that = does=20 what's required, but doesn't compromise the internal layout or add = excessive=20 cost and complexity.=20

Photovoltaic optoisolators are a good solution, but the JFET (or the = scheme=20 shown in Figure 9) is mandatory to ensure fast turn-off times. The = greatest=20 obstacles you will face with this technique are cost and availability of = suitable photovoltaic devices. There's a wide range available, but some = will=20 struggle to provide enough voltage to ensure the lowest possible = RDS=20 (on). Others have very limited current - perhaps 20uA or less. = These will=20 have rather long turn-on times, but that's not a major limitation - = simply mute=20 the amp's input until the MOSFET relay is turned on.=20

A transformer coupled system that uses squarewave drive needs very = little=20 capacitance after the rectifier to get a clean DC switching waveform. = This means=20 that turn-on/ off times can be quite respectable, without having to = resort to=20 using opto-couplers. Once the oscillator is stopped, the relay will = switch off=20 within a millisecond or so.=20

The high frequency transformer drive arrangement is also fairly=20 straightforward, and will probably work out cheaper than using = photovoltaic=20 isolators. You can almost certainly make your own transformer quite = easily - at=20 50kHz or so you don't need many turns, so it can be wound by hand. = Naturally,=20 the secondaries must be insulated to a standard that suits the amp's = output=20 voltage - both from the primary and each other. Another possible source = of=20 suitable small transformers is to use those tiny transistor output = transformers=20 that most electronics suppliers sell. Although they are extremely basic, = some=20 suppliers ask rather silly prices for them (up to $5-6 each). While they = are=20 basically rubbish in terms of audio quality, that's the least of your = concerns=20 when they are driven with a 50kHz squarewave .=20 Their insulation may not be appropriate for a high power amp though, and = this=20 would need to be tested.=20

As noted earlier, I cannot recommend the charge coupled driver for = use in an=20 audio amp. It may be suitable for switching mains ... in which case the = coupling=20 caps (C1 and C3) must be Y-Class intrinsically safe. All = circuitry must=20 have the required creepage and clearance distances for separation of = hazardous=20 voltage from your control electronics.=20

Using separate DC supplies (whether via a mains transformer or = miniature=20 DC-DC converters) is expensive and rather clumsy. It's hard to recommend = this=20 approach, but it may be required for some less pedestrian uses for a = MOSFET=20 relay. Since isolated switchmode DC-DC converters are available with = over 1kV=20 isolation, the technique is suitable for switching mains, provided = transistor=20 output optoisolators are used for MOSFET control.=20

If you do use floating fixed supplies, you need to decide whether to = switch=20 the supply on and off to control your relay, or leave the supply running = and use=20 an optocoupler to control the gate voltage. The opto approach has a = definite=20 advantage in speed - it's easy to achieve sub-millisecond switching = times, but=20 at the expense of additional components. Switching the power supply on = and off=20 can result in MOSFET switch-off times of 10s or even 100s of = milliseconds!=20

In terms of ultimate simplicity, the supply rail bias scheme wins = hands down=20 for power amplifiers. No oscillators or transformers, and very few = parts, so=20 there's not much to go wrong. Standard transistor output optocouplers = are cheap=20 and readily available, and the most expensive part of the system is the = MOSFETs.=20 This is the scheme that I would probably use, provided that the speaker = relay=20 isn't used for muting. It's unlikely that any alternative scheme can = come close=20 for overall cost and lack of complexity.=20

It is important to understand that it does cause a distorted signal = to be=20 produced across the speaker when turned off (especially when connected = in the=20 earth lead of the speaker oddly enough). This is of no consequence if = the only=20 goal is speaker protection, and it is by far the easiest to implement. = If full=20 muting is needed, you will need to use one of the other schemes. The = circuit=20 must also introduce a small amount of distortion when turned on, because = the=20 diodes still go into and out of conduction as the signal voltage varies. = However, the amount of distortion is very low indeed, and is unlikely to = be=20 audible at any level. While I have attempted to test for this, I was = unable to=20 measure the distortion, but of course that doesn't mean it's not there.=20

It used to be quite common for power amplifiers to have meters on the = front=20 panel to show the power level. These also used diodes driven from the = amp's=20 output, and therefore introduced some non-linearity. As far as I'm = aware, no-one=20 ever heard the distortion created, and I expect much the same with the = circuits=20 shown.=20

The circuit shown below has none of the limitations of the other = schemes, but=20 is comparatively expensive because of the two optocouplers. This is = really a=20 'cost-no-object' approach, having only one limitation - the MOSFET = turn-on time.=20 This can only be made faster by having a low impedance supply for the = gates,=20 something you can't get with photovoltaic isolators.

=20


Figure 9 - Composite MOSFET Relay Using Dual = Optocouplers

The arrangement shown above has many things to recommend it. Unlike = the=20 circuit shown in Figure 3, there is no series resistance and no JFET = that must=20 draw a tiny amount of current, thus reducing the available gate voltage = and the=20 resistor further limits the gate charge current. When the photovoltaic=20 optocoupler is active, the transistor output opto is turned off, and all = the=20 available voltage from U2 is presented to the gates of the MOSFETs. When = the=20 input signal switches from 5V (MOSFETs on) to 0V (MOSFETs off), U1's = output=20 transistor shorts the MOSFET gates to the sources, ensuring fast = turn-off.=20

The drive system is shown using 5V, but it can really be any voltage = you have=20 handy. It's just a matter of scaling R1 and R2 to get the right current = into the=20 opto's LEDs from the supply you have available. You may need to use = higher=20 voltage transistors if you want to use a voltage of over 25V or so.=20

Of course, disconnecting the speaker is not the only option. You can = also use=20 MOSFETs to switch off the amplifier's power rails when a fault is = detected [4], = however=20 the circuit must latch so that the protection system doesn't = cycle. This=20 approach also has the limitation that you can't detect the fault before = the=20 speakers are connected, since the amplifier(s) need power to trip the = protection=20 circuits, so speakers will thump loudly when the amp is turned on.

9   MOSFET Relays In Other Applications=20

Although I have shown the various circuits here as speaker relays, = needless=20 to say this is only one of many applications. When switching DC loads, = the=20 schemes described here are not needed because the polarity will be known = (so=20 only a single MOSFET is needed), and for mains AC it's generally easier = to use a=20 TRIAC or a conventional relay.=20

There are applications for the MOSFET relay in AC mains circuits = though -=20 trailing-edge light dimmers being one. In addition, if used with AC it = is=20 possible to use the relay to limit inrush current by turning on the = MOSFETs=20 relatively slowly. This may be hard to recommend though, because = dissipation=20 will be high and even a small asymmetry can cause an effective DC = component that=20 will cause serious problems for motors and transformers.=20

The number of applications is almost unlimited, but I confess that I = can't=20 think of many that haven't been covered already. Low current SSRs can be = used=20 for audio signal switching, and they are not particularly expensive. = While this=20 method of switching would satisfy most consumer audio requirements, it = is=20 probable that most people who love to build hi-fi equipment would frown = upon the=20 idea of active switches. CMOS active analogue switches already exist, = but it's=20 rare to find them in the audio path of any hi-fi equipment.=20

Even when switching high power circuits, there is usually no good = reason to=20 add the extra complexity. In general it's far easier to use a more = conventional=20 approach - traditional relays, TRIAC solid state relays, etc. However, = it's also=20 important to know about other techniques that might just prove to be the = perfect=20 answer to a problem that appeared to be insoluble.

Conclusion=20

While the MOSFET relay has some significant advantages over and above = a=20 traditional electro-mechanical relay, these advantages come at a cost. = The=20 MOSFET relay will be physically larger than a conventional relay, and = the=20 overall circuitry is more complex and costly. Where a relay can be glued = into=20 place on the rear panel of an amp, the MOSFET version requires at least = one=20 printed circuit board, as well as more wiring. While it will survive a = DC fault=20 in the amp (possibly many times over), DC faults are uncommon in well = designed=20 amps, used properly, and with good heatsinks.=20

To obtain complete isolation (full muting), you have to forego the = parallel=20 capacitor, and use a MOV and/or 'catch' diodes on the speaker side of = the relay.=20 With the cap shown in the above examples, there is a small 'leakage' = current via=20 the cap, and if the relay is used to mute the speaker output, a = low-level signal=20 is audible with sensitive speakers. Also, note the comments for my = simplified=20 'supply rail powered' version - ignore this at your peril.=20

Yes, a conventional relay will be a real mess after the DC arc has = been=20 shorted to earth, and the relay should always be replaced if the amp has = failed=20 DC. However, the relay is cheap, easily replaced and you never have to = worry too=20 much about a multiplicity of electronic parts that can also fail, = rendering the=20 amp unserviceable even if there's no other fault. Contact resistance is=20 sufficiently low as to ensure minimal power loss (if any), and = distortion should=20 be somewhere between zero and negligible if you have good contact = materials and=20 no oxidation. Once driven to power, any oxidation will be burnt away = anyway - it=20 is extremely uncommon for anyone to suffer from audible distortion = caused by=20 relays.=20

The MOSFET relay will survive countless DC faults, but this should = never=20 happen. All the additional complexity and cost is essentially wasted, = with the=20 exception of very high power amplifiers. It is extremely hard to find = any relays=20 that can break 100V DC at 25A or more - they exist, but are large and = expensive.=20 In such cases, it is worth considering the use of a final level of = protection -=20 a high power TRIAC that acts as a 'crowbar'. It protects the speaker by = simply=20 shorting the amp's output to earth. The amp has already failed, so = additional=20 damage is of little consequence because it will be limited when the fuse = blows -=20 which it will do spectacularly.=20

The important thing is to ensure that an amplifier failure only means = that=20 you have to repair the amp - not the speakers to which it's connected. = In many=20 cases, the loudspeaker drivers can cost more than the amplifier.=20

Naturally though, the idea of building your own MOSFET relay should = have some=20 appeal, just for the knowledge gained and the experience you'll get, not = to=20 mention the fun factor. I leave it to the reader to decide which method = to=20 explore and how much fun they should have doing so.

References=20
  1. Solid State Relay Employing MOSFET Power Switching Devices, US = Patent=20 4,438,356 - 20 March 1984 =20
  2. Dionics DIG-1115-SM Photovoltaic MOSFET / IGBT Driver =20
  3. Charge-Coupled MOSFET Relay - David Johnson and Associates =20
  4. A=20 DC Fault Protection Circuit for Audio Amplifiers

I also looked at a great many suggestions, websites and application = notes -=20 some good, some decidedly otherwise. The references shown above are = intended as=20 representative, and the same or similar information can be found = elsewhere. A=20 search is always a good place to start, but you need to know just what = to look=20 for in any circuit you may find. While some ideas seem ok on the = surface, that's=20 because the potential shortfalls haven't been mentioned (or = addressed).

  =20
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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 =A9 2012.=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 allow=20 that one (1) copy may be made for reference. Commercial use is = prohibited=20 without express written authorisation from Rod=20 Elliott.
Published 09 June 2012
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