We can view this region 3 phenomenon in a different way by analyzing the torque equation and the inverter response.
Let's briefly review the way an induction motor works. The electrical power is supplied via 3 phases to the stator, which is fixed and does not rotate. However, the sinusoidal AC waveform applied to the 3 stator phases causes a rotating magnetic field to appear inside the stator. The speed of rotation is given by:
where N=the speed of the magnetic field rotation in RPM, f = the applied AC waveform frequency in Hz, and P = the number of poles (pairs of windings) per phase in the stator of the motor.
This speed is referred to as the "synchronous speed". Take a normal AC motor in an industrial application, such as a pump. With 2 poles and a 60 Hz line frequency, the synchronous speed is 3600 RPM.
The rotor of the induction motor lies within this rotating magnetic field, and contains shorted windings. Like a transformer, the rotating magnetic field from the stator
induces a current to flow in the rotor windings (hence the name
induction motor). The current flow in the rotor causes the rotor to create its own magnetic field. The interaction between the stator's rotating magnetic field and the rotor's magnetic field now creates a torque that causes the rotor to rotate.
The important thing to realize is that the rotor
cannot turn at synchronous speed. If it does, the net difference in speed between the stator's rotating magnetic field and the rotor will be zero, and
no current can be induced in the rotor. This causes the magnetic field of the rotor to fall to nothing, and therefore no torque can be produced.
Thus to produce torque, the rotor always must rotate slower than synchronous speed. The difference between the two speeds is referred to as
slip and is given by the equation:
s is the slip (near 0 when the motor is unloaded, 1 when the motor is at standstill), Ns is the synchronous speed, and Nr is the rotor speed.
A running induction motor developing torque must always have some slip. Torque is directly proportional to slip, and the more slip, the more torque.
Now, let's explain why the Model S hits region 3, where the power begins to decrease. Let's start with the torque equation for an induction motor:
T is total torque
ns is the synchronous speed of the stator's rotating magnetic field
s is the slip
E2 is the rotor's induced voltage. This is proportional to the stator's voltage E1 which is applied by the inverter.
R2 is the rotor winding's resistance (fixed).
X2 is the rotor winding's inductive reactance (fixed).
Now remember that the inverter can vary both the applied frequency (and therefore the synchronous speed, Ns, and thus also the slip, s) and the applied voltage E1 (which then directly affects E2).
Let's assume a Model S is accelerating at maximum capability through region 2, where the inverter is keeping power limited to the maximum that the inverter elements can handle. Let's hold the inverter parameters constant, and observe what happens in the torque equation if the car speeds up a small amount:
As the car speed up, rotor speed goes up, which reduces the slip, s. The net result is that torque would go down. The inverter has to react to this to maintain torque. The inverter can do two things: Increase applied frequency and/or increase applied voltage. At first, it might seem that we can completely counteract the increase in rotor speed by just increasing applied frequency. This will bring the slip back up. Unfortunately, there is another effect in that increasing frequency also increases synchronous speed, and the Ns parameter in the denominator means that it will bring torque down:
Thus, the inverter can't completely counteract the torque decrease by only raising frequency. It will have to increase applied voltage as well:
Now the torque can be brought back up along with the current, and our power can remain constant.
Note that the inverter is taking battery voltage and dividing it. Some of that voltage is dropped across the IGBT's in the inverter, the rest is delivered to the motor (E1). With what just happened above, the division of the voltage has changed: Less of the battery's voltage is being dropped across the IGBT's, and more is being delivered to the motor. This process continues throughout region 2.
Eventually, we hit a point where nearly all of the battery's voltage is being delivered to the motor, and virtually none of it is being dropped across the IGBT's. At this point, E1 (and therefore E2) can no longer be increased by the inverter. We enter region 3.
Now, the only thing the inverter can do is increase frequency. We result in the same equations as above:
The vehicle speeds up, the slip decreases, and therefore the torque decreases. The inverter will try to compensate by increasing applied frequency, but that can't fully stem the torque decrease.
With lower torque, current drops. With constant voltage and less current, we have less power.
You might ask, well, can't we just increase slip even further by raising applied frequency and get more torque? At this point, no you can't. There is a balancing act for increasing the applied frequency. At low values of slip, increasing the applied frequency will indeed increase the torque, but past a certain amount, the ns term in the torque equation becomes dominant, and increasing applied frequency past that point will result in a torque decrease, not an increase. The inverter will keep the applied frequency at the exact point throughout region 3 such that the torque is maximal.