liveforphysics said:
This is DC getting chopped into square blocks. PF does not apply.
Yes, I figured as much. (Still a bit curious though in what respect it is mentioned in your first paragrapgh, and by Joe90, if not in the sense of PF).
Actually, what I'm fishing for is a mathematical description/model/reasoning concerning advanced timing in a regular 60 degree block commutation scheme. (I admit the connection to the subject of PF is far fetched, but at least both topics share a current lagging an applied voltage). I'm aware the topic of advanced timing has been widely discussed, and I was hoping someone would know of any analytical source of information dealing directly with hard degree, inductance and current values, perhaps with some illustrative equations and diagrams.
I see two different takes on the subject. 1. Advance timing as in field weakening to enable higher top speeds.
2. Advance timing as in making sure the area formed under a current vs. time curve during one commutation period has its total area divided equally around the instance in time when the permanent magnet rotor vector lags the stator magnetic field by exactly 90 degrees, resulting in maximum torque per current.
I'm interested in #2. Block commutation as we know it is set up to commutate 30 degrees before the two magnetic vectors form the sought after 90 degree relationship. It will again commutate 30 degrees past that point. In an ideal situation, the product of current and time from each of the 30 degree periods would be exactly equal. This would be so because the torque contribution of a current will be weighted by how far away it is in time from the 90 degree instance. Moving away from the 90 degree instance in any direction yields diminishing returns.
As has been explained many times by this fantastic forum, for reasons of inductance, duty cycle and BEMF, the current will not rise instantly when applied in the beginning of the 60 degree commutation period. Instead it will "slowly" rise and reach its peak perhaps by the end of the 60 degree period, when time has come to commutate and begin all over again. So, before the 90 degree instance there is very little current*time area, and after the 90 degree instance there is a whole lot more, with diminishing contribution to torque as the motor rotates away from the 90 degree instance. The center of the current*time area is very far away from the 90 degree instance! For large currents, compensating for this by advancing the timing might be of good use.
Still on loose grounds here, but if the above reasoning is correct and relevant, perhaps it has been analysed more in detail somewhere?