There are two major causes of hybrid stepper motor heating: copper losses and iron
losses. Copper losses are the easiest to understand; this is the heat generated
by current passing through a resistance, as in the current passing through the
motor’s winding resistance. Often this is referred to as “I2R” dissipation.
This cause of motor heating is at a maximum
when the motor is stopped and rapidly diminishes as the motor speeds up since
the inductive current is inversely proportional to speed.
Eddy current and hysteresis heating are
collectively called iron losses. The former induces currents in the iron of the
motor while the latter is caused by the re-alignment of the magnetic domains in
the iron. You can think of this as “friction heating” as the magnetic dipoles
in the iron switch back and forth. Either way, both cause the bulk heating of
the motor. Iron losses are a function of AC current and therefore the power
supply voltage.
As shown earlier, motor output power is
proportional to power supply voltage, doubling the voltage doubles the output
power. However, iron losses outpace motor power by increasing non-linearly with
increasing power supply voltage. Eventually the point is reached where the iron
losses are so great that the motor cannot dissipate the heat generated. In a
way this is nature’s way of keeping someone from getting 500HP from a NEMA 23
motor by using a 10kV power supply.
At this point it is important to introduce
the concept of overdrive ration. This is the ration between the power supply
voltage and the motor’s rated voltage. An empirically derived maximum is 25:1,
meaning the power supply voltage should never exceed 25 times the motor’s rated
voltage or 32 times the square root of motor inductance.
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