Bob Lee (QSC)
In case you missed it, I work for QSC Audio!
- Jul 3, 2001
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- Disclosures
- Former Technical Communications Developer, QSC Audio
By definition, a square wave has components of a DC signal.
The flatted peaks on both sides of the null-point are at a voltage that are held for x/moments and that effectively is a partial square wave.
One can see that any repeating, non-sinusoidal waveform can be equated to a combination of DC voltage, sine waves, and/or cosine waves (sine waves with a 90 degree phase shift) at various amplitudes and frequencies. This is true no matter how strange or convoluted the waveform in question may be. So long as it repeats itself regularly over time, it is reducible to this series of sinusoidal waves. In particular, it has been found that square waves are mathematically equivalent to the sum of a sine wave at that same frequency, plus an infinite series of odd-multiple frequency sine waves at diminishing amplitude:
Then ::: As noted step by step from here - it's rather obvious what it is we're creating in musical wave form.
In this first plot, one can see the fundamental-frequency sine-wave of 50 Hz (an slightly sharp-tuned G1) by itself. It is nothing but a pure sine shape, with no additional harmonic content. This is the kind of waveform produced by an ideal and perfect musical note, although for purposes of argument, the 50 Hz is not normally a tuned note :![]()
Pure 50 Hz sinewave.
Next, we see what happens when this clean and simple waveform is combined with the third harmonic (three times 50 Hz, or 150 Hz - all very common in a stringed instrument). Suddenly, it doesn't look like a clean sine wave any more:![]()
The sum of the 1st (50 Hz) and 3rd (150 Hz) harmonics approximates a 50 Hz square wave.
The rise and fall times between positive and negative cycles are much steeper now, and the crests of the wave are closer to becoming flat like a squarewave. Notice what happens as we add the next odd sinusoidal harmonic frequency:![]()
The most noticeable change here is how the crests of the wave have flattened even more. There are several more dips and crests at each end of the wave, but those dips and crests are smaller in amplitude than they were before. Watch again as we add the next odd harmonic waveform to the mix:![]()
The sum of 1st, 3rd, 5th, and 7th harmonics more aptly approximate a square wave.
Here we can see the wave becoming flatter at each peak. Finally, adding the 9th harmonic, the fifth sine wave voltage source in our circuit, we obtain this result:![]()
The sum of 1st, 3rd, 5th, 7th and 9th harmonics approximates a true square wave.
We can get into the Squarewave for SPICE/Fourier analysis, but you can see that at almost any time a note is struck on a string, it generates a certain quality that approximates a square wave with all the primary, secondary, tertiary harmonics, etc.
You are almost always attacking the speaker(s) with these semi-square wave or their equivalent in form by mass acceleration/magnetic hysteresis/field collapse, subtrahention and reversal and REMF anyway.
I too once agonized over the causative damage (via distortion boxes and stomp pedals) to the speaker cones and voice coil windings, but with ample heat radiation/conduction/convection and the resulting damage induced into the delicate micro windings in the coil and the fact that paper burns at Fahrenheit 451, I can see that there might be some concern about square waves.
Just don't hold a note for more than 1.4 seconds and you'll be alright! <sarcastic smiley>
A square wave still isn't DC and shouldn't be confused with DC.
