After my previous question Why the triangle reference wave is used in PWM for sine modulation I still have some troubles on one particular point of natural sampled PWMs or more precisly SPWM.
My question is: Why the intersection points between the carrier and the reference wave are the "hot spots" where the width of the PWM is calculated?
In all the literature that I read no one mentions why the comparison works and what is the core meaning behind it. In fact every paper and PWM related article states something on those lines:
The output \$V_0\$ of each comparator has a "high" level whenever the instantaneous input reference level exceeds the timing wave level and a "low" level when the reference is exceeded by the timing wave, resulting in a PWM waveform,...[1]
When the reference waveform is greater than the carrier waveform, the phase leg is switched to the upper DC rail. When the reference waveform is less than the carrier waveform, the phase leg is switched to the lower DC rail... [2]
I'm searching meaning behind those types of statements and the only thing that comes to my mind is that:
1) integrating a square (on it's period) produces a half triangle $$ + $$ 2) the technique behind PWM is to reproduce the average value of the reference wave in small \$\Delta t \$'s (over and over) $$\Downarrow$$ intersecting the reference wave with the carrier (that represents the area of a full pulse (1)) produces the point where the width of the pulse has to stop to represent the avg value of the reference wave for that period (\$\Delta t \$ (2)).
$$ $$
[1] "Pulsewidth Modulated Inverter Motor Drives with Improved Modulation" IEEE Transactions on Industry Applications Volume IA-11 issue 6 1975 Zubek Jacob; Abbondanti Alberto; Norby Craig J.
[2] D. Grahame Holmes, Thomas A. Lipo "Pulse Width Modulation for Power Converters Principles and Practice"-Wiley-IEEE Press (2003)