I'm making this post mostly to check things for another post I'll make (if I don't find any error up to this point).
I'm trying to calculate the efficiency for an ideal DC series motor as a function of the speed, without any load attached to it.
Once I'm considering it's ideal (in classical mechanics), then there's no friction and it will accelerate indefinitely for any given input voltage U. The mechanical output is going to be entirely converted into rotational kinetic energy at any moment.
The expressions I developed for the series motor are:
T = KtI²
Torque is proportional to the square of the current with a constant Kt
I = (U-Eb)/R
The current is equal to the resulting voltage (applied voltage minus back emf) divided by the total series resistance
Eb = KeNI
The back emf is proportional to the speed and the current (once it's the same for the field winding) with a constant Ke
Solving this the current and the torque will be:
I = U/(R+KeN)
T=KtU²/(R+KeN)²
The mechanical power (Pm), electrical power (Pe) and Efficiency (E) will be:
Pm=NKtU²/(R+KeN)²
Pe = U²/(R+KeN)
E=NKt/(R+KeN)
The efficiency varies only with the speed, and as N tends to infinity, the expression tends to E=Kt/Ke
I'm unsure of the meaning of this result.
I know that at least until the expression for efficiency the dimensional analysis checks, both sides of the fraction have the unit Ohm (N·m·s/C²), so the result is dimensionless as efficiency should be.
This also shows that the efficiency is independent of the applied voltage or the torque its exerting, the only variable in there is the speed.
Is this true for a situation with load?
I mean, if I find the equilibrium speed for a given load and applied voltage, then I can find the efficiency directly through that expression?