Can square waves cause a DC voltage

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Discussion Overview

The discussion revolves around the concept of whether square waves can induce a DC voltage across a coupling capacitor in electronic circuits, particularly in the context of audio amplifiers and preamp tubes. Participants explore the implications of non-symmetrical square waves, the behavior of coupling capacitors, and the definitions of DC in relation to these signals.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants assert that a non-symmetrical square wave can cause a temporary DC voltage to appear across a coupling capacitor, affecting the operation of subsequent components in the circuit.
  • Others argue that while the effect may resemble DC, it is not technically DC if the capacitor is functioning properly, as it averages out the signal over time.
  • A participant suggests that any time-varying signal with a non-zero average can be considered to have a DC component, which aligns with the idea of a "DC-like effect."
  • One contributor discusses the mathematical interpretation of square waves and their DC components, emphasizing that the DC level depends on the phase at which the wave is initiated.
  • Another participant raises questions about the definition of DC, suggesting that a frequency of zero is a requirement for a signal to be classified as DC.
  • There is a mention of using diodes in parallel with coupling capacitors to mitigate voltage excursions caused by spikes.

Areas of Agreement / Disagreement

Participants express differing views on the definition and implications of DC in the context of square waves. While some agree that a square wave can produce a DC-like effect, others contest whether this constitutes true DC. The discussion remains unresolved regarding the precise definitions and interpretations of these concepts.

Contextual Notes

Participants highlight the complexity of defining DC and its relationship to time-varying signals, indicating that assumptions about ideal components and real-world behavior may influence their conclusions. The discussion also touches on the mathematical aspects of signal analysis, such as Fourier transforms.

Planobilly
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I read this statement from Lenard Audio.

"When a large signal spike is created by un-plugging or plugging in signal leads, or when a pre-amp valve is driven hard into distortion (guitar amps), a large non-symmetrical square wave may cause a temporary DC Voltage to appear across a coupling capacitor, to the Grid of the following valve. This short DC pulse will cause the following valve to be shut off, or go into full conduction, for approx 1mS to 1 second, until the following Grid resistor discharges the coupling capicator."

First, is this statement correct. Second, if yes, how does this work?

Thanks,

Billy
 
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It isn't "technically" DC if you have a good quality capacitor, but a non-symmetrical square wave can easily change the effective DC level after the coupling cap due to bandwidth limitations on the following circuits. Since you probably have reasonably low bandwidth after the coupling capacitor, the circuit will average the spike and the level will rise and slowly fall as the pulse goes away.

The easiest way to visualize this is:

1. The coupling capacitor passes any spikes with little attenuation (the impedance is low at high frequency, and spikes have a lot of high frequency energy).
2. The signal path has limited bandwidth (for noise reasons, among others)
3. The high frequency spikes is then low-pass filtered.
4. A low-pass filtered square wave is just its average value (you can use a low-pass filter to measure duty cycle, for instance)
5. This appears as an effective DC shift across the coupling capacitor.

You can see this exactly thing by plugging in a scope probe on an oscilloscope. Do you see how the level jumps up and slides back down to baseline? This is the effect. Make sense?

To fight this kind of thing, you can put diodes in parallel with the coupling capacitor to limit the voltage excursion. This is sometimes done but it often is not due to cost/component count/space considerations.
 
Thanks Analogdesign

As I am learning something new every day and I am far from knowledgeable about electronics, I hesitate to just say "that's not correct". So, when I read that statement I just did not think that this was DC. I had even less idea how it could be possible to create DC on a grid through a good capacitor by driving a preamp tube into distortion.

DC like effect, yes I can buy into that idea. I am pretty sure the guy writing the statement knew what he meant. Perhaps sometimes I read things in a "too literal"

Thanks for clearing this up for me.

LOL...every question answered brings up another question...lol Now I need to go investigate diode in parallel idea!

Cheers,

Billy
 
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Planobilly said:
Thanks Analogdesign

As I am learning something new every day and I am far from knowledgeable about electronics, I hesitate to just say "that's not correct". So, when I read that statement I just did not think that this was DC. I had even less idea how it could be possible to create DC on a grid through a good capacitor by driving a preamp tube into distortion.

DC like effect, yes I can buy into that idea. I am pretty sure the guy writing the statement knew what he meant. Perhaps sometimes I read things in a "too literal"

Thanks for clearing this up for me.

LOL...every question answered brings up another question...lol Now I need to go investigate diode in parallel idea!

Cheers,

Billy
DC can also arise if the amplifier is driven hard because the grid/cathode circuit acts as a diode rectifier.
 
Planobilly said:
So, when I read that statement I just did not think that this was DC. I had even less idea how it could be possible to create DC on a grid through a good capacitor by driving a preamp tube into distortion.

DC like effect, yes I can buy into that idea. I am pretty sure the guy writing the statement knew what he meant. Perhaps sometimes I read things in a "too literal"

Perhaps you are too literal. Any time varying signal whose average is not zero has a DC component. I think that is what they are describing.
 
yes it's correct

here's a shot at how it works
it's a quirk of math that the circuit guys quashed for us.

It doesn't even have to be asymmetrical, a symmetrical square wave can have a DC component
but the coupling capacitors in your signal path soon force it to zero

If all is quiet,
then you switch on a nice square wave (or sine wave for that matter)
its DC component depends on where in the cycle you start it. Man oh man is that counterintuitive, though..

Thought experiment time

Let's think of DC as just the long term average, over several cycles

and also consider short term average, most recent half cycle

for the red square wave ,
gray is short term average note it builds from zero in first half cycle then heads back toward zero next half cycle, barely makes it there and turns right around again
brown is long term average which builds to average of gray wave, slower than i showed it though.

squarewaveDC_planoB.jpg

so that nice looking square wave has a DC component shown by the brown line,
and how much DC depends on when in its cycle it got switched on.

Same is true for a sinewave
and that's why power transformers have such huge inrush if you close on them at sinewave's zero crossing.
We had a thread on that last year...So,
the coupling capacitors in your signal path not only separate the high plate DC from the low grid DC,
they block any DC that's got your signal because of the random time somebody threw a switch.
More accurately they bleed it down to zero,
and thus spake Lenard .

old jim
 
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Hi Jim,

I get where you are going with your post.

I guess this whole discussion should go back and define DC. I took this definition from a website and it looks as good as any.

"DC (direct current) is the unidirectional flow or movement of electric charge carriers (which are usually electrons). The intensity of the current can vary with time, but the general direction of movement stays the same at all times. As an adjective, the term DC is used in reference to voltage whose polarity never reverses.

I ASSUME the following. Correctly?

DC has a frequency of zero. If it does not have a frequency of zero it is not DC. A frequency of zero imply infinite impedance
A "ideal" capacitor will not pass DC
Pulsed DC, while everyone knows in general what that means...that is it alternates from from zero to some value over some period of time, it none the less alternates. It does not have a frequency of zero.

For a "spike" or call it a "pulse" a Fourier transform will clearly show frequencies other than zero for a pulse or spike.

I am saying this jokingly but I am beginning to wonder if at some level DC even exist...lol

I assume even a battery could have less than a perfect rate of discharge however small.

Cheers,

Billy
 
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Ahhh now we're getting there

to get by in today's world we need to be able to think like a pure mathematician
and still get by as a practical technician.

If you redraw that square wave i drew up above
but instead of starting it at zero you start it at 1/4 cycle
go ahead, copy it into paint and do it
draw the short term average this time in say green not gray
squarewaveDC_planoB2.jpg


observe the short term average now is centered about zero
so this symmetrical square wave has no DC component, but the only difference between the two is where in the first cycle they started

Your scope has FFT which breaks any waveform down into its component frequencies
one of them is 0 hz, the DC component ,,, often calleda0
first wave's 0 hz component is nonzero second one's is zero
 

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