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Point to Point Versus PCB Amps - What's the = difference?

Copyright 2000 R.G. Keen. All = rights reserved. No permission for local copies or serving from web sites other than http://www.geofex.com/.

[Point=20 to Point] [Stripboard] [Pros=20 and Cons] [Capacitances] [PCB=20 Right] [PCB=20 Wrong] [Good Stripboard] [Bad=20 Stripboard] [Myths]

Ever hear this one?

"Get a point-to-point wired amp - those PCB amps are no good. They = just don't=20 have the tone they did in the old days." 

The deeper you dig into this issue, the more repair techs you'll find = that=20 say that PCB amps are no good. They'll give explanations involving = things like=20 tiny traces run too close together, and the capacitance leaking signal = from=20 place to place and then make the leap that this somehow spoils the tone = of the=20 amp. Is this bit of folk wisdom right? 

Yes and no. The short version of the answer is this:
There is no = technical=20 reason that PCB amps *can't* be every bit as good as point-to-point = wired amps -=20 or stripboard wired amps, which is what the grizzled techs usually refer = to.=20 However, there are some serious reliability (not tone!) shortcomings in = most of=20 the PCB based amps that have been put on the market; this is the origin = of this=20 folk myth. 

At the bottom of both sides of this question is self-interest. On the = side of the amp makers, most of the time the PCB conversion is done as part of = a cost saving measure; the same motive to change to PCB's also drives changing = to cheaper practices and parts all around. This most often gives worse = tone. They're doing less than the best they could, for money.

On the amp tech side,  PCB amps that have been done poorly have = frequent breakdowns. They are not as easy to repair as hand-soldered terminal = wiring.=20 They require some delicacy in fixing, and they can be a true pain to get = the=20 boards in and out. So to the techs, they break more often, and are = fiddlier to=20 repair. The techs usually can't charge more for PCB amps, so - no = surprise -=20 they don't like them much.

So - PCB based amps, from what we've seen so far, have poorer = reliability and techs don't like to repair them; but that is because they were poorly = designed from a reliability standpoint in the first place. The tone is not = necessarily poorer. Here are some comparisons

PROS and CONS

  Advantages Disadvantages
True Point to Point Approaches "ideal" in electronic terms; lowest = parasitic=20 coupling and crosstalk if done well. =20

Sturdy.

Withstands repair surgery well.

 Very expensive to design well =20

Very expensive to produce in today's market

Usually heavy.

Stripboard Less expensive to make than PTP. =20

Parasitics and crosstalk OK for most applications.

Parasitics and crosstalk are variable depending on lead = dress.

Withstands repair surgery well.

 Higher parasitics than PTP. =20

Variable parasitics.

Moderately expensive to produce in today's market

PCB Inexpensive to downright cheap to produce

Absolutely fixed, known parasitics - whether good or = bad

Extremely reproducible.

 Needs special planning and design to avoid = mechanical =20 problems. =20

Repairs must be done delicately if it needs=20 repaired.

Most PCB amps that have been produced *have* been poorer than tube = amps, for reasons having nothing to do with the PCB's. Like plastic bobbins in transformers, this does nothing to change the tone. The *other* poor = practices that go with a cost-cutting attitude that were introduced at the same = time may, but PCB's are unfairly indicted.

 

If you're interested, here's some more information about the = differences in point to point, stripboard, and PCB construction practices that DO make = a difference.

Point to Point (PTP) - What is it and = what's good about it?

This is one version of real "point to point" construction.

The view is from underneath the chassis surface, looking at the = bottom of a 9 pin miniature tube socket and two terminal strips that the circuit is = built on. Good point to point layout makes the actual component bodies bridge = most of the distance from the socket lugs to any other connections. Really, really = good PTP construction will have the components arranged in almost a star = pattern, all of them leading radially away from the socket. 

What's important there is that (a) all the component leads are pretty = close to being as short as they can be (b) the component to component wiring = lengths are as short as possible (c) neither the components nor the wires = criss-cross one another (d) the lengths of paralleled wires are about as small as = they can be.

The reason that all these are important is that there is an = unavoidable bit of capacitance between any two electrical conductors that are at = different voltages. You can think of this as a little "ghost" capacitor between = every=20 combination of two points on the schematic - ugly! These ghost = capacitors are=20 often referred to as parasitic capacitors.

This capacitance is proportional to the facing areas of the two = conductors,=20 and inversely proportional to the distance between them. For maximum = coupling=20 between two conductors. they need to be as close together as possible, = and have=20 the maximum area exposed to one another. 

For two wires, the closest they can get is with their insulation = touching. For the maximum area, they'd have long parallel runs; for minimum area, = they'd=20 cross at right angles. In true PTP, the components and wires are as far = from one=20 another as it's practical to get, and where crossovers are needed, they = can be=20 at almost right angles. Also, the wiring between amplifier sections can = be=20 minimized by laying out the tube sockets in a manner that the signal = flows=20 directly from one tube circuit to the next with no long runs of parallel = wires.=20 Also, the terminals themselves space the wires a goodly distance away = from the=20 presumably grounded metallic chassis.

The worst case for cross coupling in wiring of any kind is where the = wires=20 run parallel and with their insulation touching. I spend part of a = Saturday=20 morning digging through my collection of electronics and physics texts = to come=20 up with some rules of thumb for how big the capacitive coupling is. Of = course,=20 this varies all over the map depending on the layout and wire sizes. = However,=20 for two 22 gauge hookup wires with kind of nominal insulation = thicknesses, the=20 capacitance between the two wires is about 0.381pF per inch. Ten inches = of=20 parallel run, the capacitance is 3.81pF. With the wires crossing, = there's only=20 about 0.025" of wire "parallel", so the capacitance is on the order of=20 0.008pF.

Oddly enough, the capacitance of two PCB traces under similar = conditions is actually less. For two 0.025" wide traces spaced a conservative 0.075" = apart,=20 the capacitance is 0.317pF per inch. Finer traces even closer together = do have a=20 higher capacitance per unit length, but much less than you'd expect - it = goes up=20 much less than linearly with smaller, finer traces. We have the curious = result=20 that wires and PCB traces have very similar parasitic capacitances, and = PCB=20 traces have a slight edge over wires. That kind of means that it's how = you use=20 them, not which you use, huh?

Note that a poor PTP layout can be a nightmare of = criss-crossing parts and wires that can loose a herd of electronic demons. What makes a PTP = wired circuit good is (a) careful planning and (b) very skilled labor doing = the=20 wiring neatly and carefully. For reason (b), true PTP is very expensive, = and has=20 been even as far back as the late 50's.

True PTP construction is good for frequencies up to UHF (several = hundred MHz!!) if properly done. This is the reason all that old tube radio = equipment was laid out that way. Good PTP layout has wires that almost never come = close=20 to one another, and when they do, the cross instead of running parallel. = That's=20 good, but it's a long way from audio to UHF, so maybe there's something = else=20 that can fill the bill. 

Stripboard = Construction

The kind of construction in amps that is most often referred to as = "point to point" is not really point to point at all. Most amps use some kind of insulating board with either eyelets (notably Fender) or turrets set = into the board, and the components strung in neat little rows on the = board. 

All the connections to tube sockets are made with wires from the = stripboard to the tube sockets and controls. Note that unlike true PTP, the wiring = lengths=20 from the components to the tube sockets are no longer as short as they = were.=20 Also, the wires are often stranded wire, and free to move around, where = the=20 component leads in PTP were solid, and pretty much held in place by = being short=20 and stiff. To get easier wiring, we have sacrificed the very short interconnections that are a characteristic of good PTP wiring.

The freer, stranded wires can now move around relative to one = another. This means that they have variable capacitances among them! = The coupling of signal from place to place by accident (if it was on = purpose, we'd use a wire or capacitor) is now a variable that depends on how you push = the wires around after they're installed. The placement of wires in this = kind of construction is referred to as lead dress. Not too = surprisingly, poor lead dress can cause the wrong signal to get picked up and = amplified. This can cause hum if the wires get too close or too parallel to those = green/black filament heater wires, or oscillation if an output signal wire gets too = near a sensitive input.

Good stripboard construction can approach the performance of true = PTP. However, stripboard construction abandons the electronic elegance of = true PTP for easier, faster manufacturing by less-skilled (and cheaper!) = workers. With=20 stripboard, assuming a minimum of good workmanship on putting the parts = on the=20 stripboard, the differences in quality will depend primarily on the = wires that=20 lead away from the stripboard to the outboard controls and other = components.

This is an illustration of a = good style=20 of stripboard layout. The input and power transformers are at opposite = ends of=20 the chassis. The tube sockets, stripboard, and controls are laid out so = that the=20 wires from the stripboard to the sockets and controls are as short and = direct as=20 possible - no long runs of parallel wires.

Doing this is not all that easy. It takes a good deal of foresight = and skill at the processes of wiring and building things in this style to get the = wires=20 as short and direct as possible. 

There is also a built-in service problem with this style. Notice that = the stripboard is "tied down" by the wires coming off both sides of the = stripboard=20 to tube sockets on one side and controls on the other. To lift the = stripboard=20 itself requires unsoldering all the wires from one or the other side. Fortunately, most of the parts are easy to get to and replace from the = top side if the board has NO components or wires running under the board. Sadly, = this is not always true. Poor layout is not limited to PCB's.

Stripboard has a dark side, too. = Consider the=20 following picture.

In an attempt to be neat and tidy, the wires have been = gathered into=20 neat, tidy bundles where the wires from some mechanical area are = gathered into a=20 paralleled bunch, often tied into the parallel bundles by lacing ties = (beeswax=20 impregnated cotton is the old standard!) or nylon cable ties. The = advantage here=20 is that you can drive nails into a dummy amp baseboard at the corners of = the=20 wiring, to pre-cut and lace in place all the wires before ever putting = them in=20 an amp. What's wrong with this picture?

That ugly word - parallel. This is how you maximize coupling, = remember. Putting the wrong components side by side can cause performance = problems in=20 high impedance circuits. Putting the wrong wire in the wrong bundle can = make=20 this construction oscillate uncontrollably, or can introduce treble = loss.=20 Conversely, not every signal wire coupling makes a difference to every = other=20 wire, so there's usually some bundling arrangement that can make this=20 arrangement work OK. Sometimes a signal wire must be shielded to run in = a bundle=20 without unwanted coupling.

Which brings up an interesting point - shielding. Shielding a signal = wire is most commonly taken to mean running a coaxial wire with the signal on = the central conductor and the shield connected to ground. The shield does = in fact keep any other signals out side the shield from touching the central = conductor by shunting those signals to ground. However, it does it by completely=20 enclosing the signal wire in an enveloping parallel (ack! there's that = word=20 again!) sheath. As you might expect from the earlier comments on = parallel wires,=20 a wire with a shield completely surrounding it has a lot of capacitance = to the=20 shield. Indeed, coaxial cable often has specifications on the = capacitance per=20 length of cable. Good cables can be down in the range of 10-15pF per = foot. Bad=20 cables can be significantly more. Put a couple of feet of bad shielding = cable on=20 a grid signal, and you're losing treble. Better than oscillating, but = not=20 perfect by any means. 

Wiring capacitances - how much = matters?

It's easy to calculate how much is too much for audio purposes. There = are two important cases - a capacitor in parallel with a resistor and a = capacitor in series with a resistor. We don't consider inductors and capacitors=20 because 

Fortunately, we can calculate the frequency where the capacitor and = resistor interact the most very easily. This is the frequency where the = capacitor's impedance equals the resistance, or F =3D 1/ (2*pi*RC). To a first = approximation we can consider every frequency below this to be unaffected by the = resistor,=20 and above it to be unaffected by the resistor. 

Guitar amps are a special case of audio amplifiers. Hifi amps have to = handle 20kHz, and some purists would insist that 40kHz is a minimum. However, = the best wound guitar pickups pretty much cut off above 7kHz and our speakers = don't put out much above 4kHz. Even for fuzz-box generated hash, there's not much happening above 10kHz. To make some sense of the huge numbers of=20 variables, we'll have to make some assumptions. The capacitances we = calculate=20 may be wrong by a factor of two either way, but then calculating = capacitances between free-swinging wires is prone to some error anyway. We'll at = least be close enough to know where to dig deeper if we need to.

For a resistor, the "significant capacitance" is C =3D 1/ (2*pi*Rf), = or at=20 10kHz, C=3D (15.9/R) uF. If the resistor in question is a 1M resistor, = the=20 capacitance will be C =3D 15.9pF. So a resistor between 8 and 32pF makes = a=20 "significant difference" to a 1M resistance. We can see then that the = higher the impedances involved, the smaller the capacitance that makes a = difference to tone. Likewise, the lower the resistance, the bigger the capacitance = must be to make a difference.

One "resistance" we don't see listed on schematics also has a big = effect -=20 the equivalent plate resistance. Since we already know that the higher = the=20 resistance, the smaller the capacitance that has an effect, we'll = consider two=20 high-end examples - the 12AX7 plate and a small-signal pentode plate = resistance.=20 The 12AX7 has a plate resistance of about 60K under the conditions it's = most=20 often used in preamps. This resistance is effectively in parallel with = the plate=20 resistor, so the parallel combination makes for a resistance of about = 37.5K in=20 the very common instance of a 100K plate resistor. 

We can quickly see then that the wire coming from a 12AX7 plate may have  a 37.5K source resistance - that is, it can = supply current exactly like a perfect voltage source with a 37.5K resistor in = series with it. This wire couples the signal it carries to every conductor = anywhere near it - and is loaded by every conductor near it through the = parasitic capacitances. If the wire is run right along the chassis, insulation = actually touching, this is just like a capacitor to ground connected to the = wire. If=20 that capacitance is more than 424pF, then we lose treble above 10kHz, = and the=20 amp starts to sound a little dull. We've lost some high-end tone.

If there are 10Vac of signal on that plate wire (not at all = unusual),  and it runs near a wire connected to an input tube's grid, Then to = couple in a feedback signal equal to a typical guitar signal of 100mv, we only need = a capacitor of  C=3D15.9/100M uF  =3D 0.159pF - YIKES!! A SIXTH = OF A PICOFARAD!!!! We suddenly see how oscillations start - a grid wire too = close to a plate wire and a bit of bad luck on the phasing and the amps starts = screaming at 100kHz.

OK. So now we know what we're playing with. A fraction of a pF can = give us oscillations, but we need something between 8 and 400pF to start = cutting treble off, depending on the circuit. 

Here's some detailed considerations on the = implications:

The picture shows a somewhat representative tube amplifier voltage = gain circuit. The "real" circuit is shown in black, and the parasitic = capacitances=20 are shown in red. The excess capacitors may come from wires or PCB = traces,=20 doesn't matter which. 

Cp1 shunts signal away from the grid when its impedance is less than = Rsrc. Cp3 shunts amplified signal around the plate resistor Rp, and Cp2 leaks = inverted and amplified signal from the plate to the grid. Every single = one of=20 these results in treble loss. Cp2 is the worst because its real value is "amplified" by the voltage gain of the stage. It can be modeled by = another=20 capacitor in parallel with Cp1 of Cp2*voltage gain. 

So how much capacitance matters? 

Cp1 and Cp2: for a representative Rsrc of 35K (typical of a 12AX7 = plate with a 100K plate resistor), when the sum of Cp1 and Cp2 times the voltage = gain is Cep=3D1/(2*pi*35K*20kHz) =3D 227pF, this "dulling capacitor" is eating = half the=20 signal. If we assume that all of this is from Cp2, and a voltage gain of = 30 for=20 the stage, then the max capacitance we can stand for Cp2 is 7.5pf.  = As we=20 know from the calculations above, either PCB land or #22 wires are both = about .3=20 to 0.4pF/inch, so we can stand a maximum of about 18 inches of = absolutely=20 parallel run wires before we start getting treble loss even at 20kHz. = That's a=20 lot! Even when we correct for our assumption that Cp1 and Cp3 didn't = matter,=20 allowing for a fifth of the capacitance to be in them, we would be safe = with=20 12-15 inches of parallel, side by side signal run. While the = laced-and-bundled=20 stripboard techniques might do this, it's unlikely to be a real problem. = Good=20 stripboard and good PCB construction will not even come close.

On Rp, Cp3 could be C=3D 1/(2*pi*100K*20kHz) or C=3D79.5pF before = we'd get treble loss at 20kHz. That's 227 inches of paralleled wire.

For Rk, there can be no effect if Ck is part of the circuit. Cp4 is completely swamped by Ck.  If there is no Ck, the gain of = this stage=20 will start rising at the frequency F=3D1/(2*pi*Rk*Cp4), or for ballpark = values,=20 F=3D1/ (2*pi*1500*7pF) =3D 15.1MHz!! The tube itself will be = cutting off at=20 that frequency. So wiring capacitance from this source has no effect on = the=20 frequency response of this tube.

Between two stages the picture changes a bit. This = illustration shows=20 two stages, one following the other, but connected with a feedback = capacitor=20 that we'll assume was caused by bad wiring. The signal at the second = plate is in=20 phase with the signal at the first grid, and considerably larger. If = each stage=20 has a gain of 30, the second signal is 30*30=3D 900 times as big as the = input=20 signal. For a 0.1V signal, we'd see 90Vac of signal on the second plate = if it=20 was not otherwise limited.

The feedback through the parasitic Cfb is limited by the plate = resistance of the second triode, maybe the 37.5K of a 12AX7, and is divided down by = the other capacitances at the grid of the first triode, Cgeq, and by any loading = at the input other than the grid leak resistor. Let's take worst case, the = input=20 open.

Unless we've done something special to make Cgeq smaller, it's = probably on the order of 2-3pF. Let's see what Cfb makes the loop gain one, so this = thing oscillates. We'd have to have a feedback loss of 900 to make this true, = so the impedance of the parallel combination of Rgrid and Cgeq have to equal = 1/900th=20 of Cfb's impedance. At frequencies below F=3D1/(2*pi*1M*3pf) =3D 53kHz, = the=20 impedance is dominated by Rg, and decreases above that. Phase shift also = accumulates above that, so let's take the resistance as the limiting = resistance.=20 To get oscillation, the impedance of Cfb has to be no more than 900 = times Rg, so=20 Cfb=3D1/(2*pi*900M*10kHz) =3D 0.018pF. ACK!! 18 FEMTO-FARADS???? HOW = DOES THIS THING=20 EVER WORK AT ALL??

It works at all because that picture does not show the whole story, = of course; it's too simplistic. There are other parasitics that are not = shown in this picture that actually raise the needed coupling well above the 18 = fF=20 level. The phase shifts and leakages we've blithely ignored, as well as = the=20 parasitics from the first tube itself enter into it as well. However, = the math=20 complexity goes right through the roof, so it gets to being a poor = illustration,=20 lost in the complexity.

It makes a great morality play for keeping your input and output = wires well separated though, doesn't it?  

This is actually one of the places that PCB construction would be a = big help. The Cfb path would likely be much nearer other signal traces and = especially ground traces, which would eat a lot of the feedback signal.

Parasitic capacitance effects on the tone stack

--- coming ---

 

 

 

 

 

 

 

 

 

 

 

 

How to do PCB construction wrong

This is easy. Just use the technology in ways that ignore the mix of = strong points and failings that every technology has. Some examples of WRONG techniques:

Unfortunately, PCB technologies are most cost efficient when = everything is connected to the PCB, which encompasses all the things you can do = wrong. So you get a clear conflict between cost efficiency (that is, the manufacturer = making money) and long term reliability.

How to do PCB construction right

Don't let the boards flex

Don't let the boards get too hot

Don't use solder as a mounting glue

Don't treat high impedance analog signals the same way you do = low-impedance digital signals.

 

PTP Wire Amp Myths You'll Hear

PCB's use traces to connect components that add a small degree of=20 capacitance between the parts which changes the = tone/sound
It is=20 correct that PCB's use thin copper traces to connect parts and that = there is=20 capacitance between all the traces. However, the implication that point = to point=20 wiring does NOT have such parasitic elements is =20 completely false. Point to point wiring uses "wires" to connect = components;=20 these "wires" also add a small degree of = capacitance=20 between the parts. In fact, for some instances, hookup wire can have = MORE=20 wire-to-wire capacitance per unit length than PCB traces. There are no = wires=20 that *don't* have self inductance, capacitance, =20 resistance and all the other ills that every electronic part is heir to. = Which=20 has more? It depends... you have to know the = mechanical=20 specification of exactly where every part is in relation to every wire = and the=20 chassis to compute the capacitance for either = traces or=20 wires. A well designed PCB with attention paid to where the traces go = may have=20 bigger or smaller capacitances to other traces = and=20 parts. 

As to this necessarily degrading tone - almost = always no.=20 The capacitances may or may not have any audible effect, and if there is = an=20 effect on the tone, it may or may not be = positive, or=20 may or may not be swamped out by the actual parts instead of the=20 wires/traces. The only way to tell is to figure out what the = capacitances=20 actually are and see if it makes a difference - what's the capacitance = of a=20 signal wire lying against the chassis for 6"? Is it more or less than = the =20 capacitance of a PCB trace for 6"? Hmmm... can't tell = without=20 measuring and seeing what this capacitance couples together in the=20 amp.

Companies used to use carbon comp resistors which yield = a=20 richer, more complex tone.
Ah, yes. The old "They don't make them = like=20 they used to". They really don't make them the same any more - thank = God.=20 Resistors used to be 20% tolerance, drifted another 5-10%, and had a = "hole in=20 the middle" where all the ones that did by accident get within 5% and = 10% of the=20 nominal value had been selected out. A 20% resistor was = guaranteed=20 to not be any closer that 11% to the nominal value because all the 10% = and=20 better ones had been selected out by the manufacturer. Old carbon comp = processes=20 had build in distortions, rectification effects, and so on. Process = control is=20 much better than it used to be. The differences in carbon comp and = modern film=20 resistors are real, but that whole thing is a topic for another article. = Suffice=20 it to say that just because it's carbon comp, it's not tone magic. = Carbon comps=20 were the cheapest available resistors in the "golden age", and were used = for=20 that reason. Leo Fender was a businessman, not a guitarist.

The quality of the parts has been reduced = / Companies used to use better quality caps. 
Another one. = This one=20 is pure nonsense. Modern capacitors are more stable, more consistent, = have=20 closer tolerances, lower drift with time and soldering, and so = on. 

Ah, but the old paper capacitors were tone magic/mojo=20 magnets/whatever.
Nonsense. Old paper capacitors had higher ESR = and ESL=20 than some modern capacitors, lower than others. It's entirely possible = to get=20 *better* modern caps and then add resistors to "ugly them down" to what = the=20 older caps did. You do have to know what you're doing, though.

Modern parts that cost next to nothing when bought bulk quantities = are=20 loaded by computers. 
Leo Fender would have jumped on that!! = He'd=20 have loved it. As it was, he used the cheapest parts and labor that = would=20 produce his amps reliably enough to sell well. Leo was a businessman, = not a=20 guitarist.

Cheaper parts and pcb's lead to an amp or effect = =20 that sounds stiff, lifeless or one dimensional compared to the earlier=20 ones
Huh? Why? What parts affect the tone? This is a form of = creeping=20 superstition. Most audio research indicates that the terms "stiff", = "lifeless",=20 "tiring", and so on are associated with low levels of intermodulation=20 distortion. This is a circuits thing, not a wiring thing, no matter how = it's=20 done.

Handwired, point to point will always sound better than any stock = PCB=20 amp.
Lets face it, in the 50's and early 60's amps were wired=20 point-to-point, because it was cheap...the skilled labor required to = solder=20 wires to the turrets was cheaper than buying PCB making equipment, which = was=20 still experimental at the time. But there's no real evidence that you = can't do=20 as well or better with a PCB. And the PCB's will come out the same way, = every=20 time. No little lead dress problems making some of your amplifiers = oscillate=20 when the rest of them are OK.

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