BLDC
How it works
A permanent-magnet rotor turns inside (inrunner) or outside (outrunner) a wound stator, most often with three phases connected in a wye (Y) or delta configuration. A controller with a transistor bridge (a three-phase inverter) energizes successive winding pairs so that the stator field leads the rotor field and sustains torque. To know which windings to energize, the controller must know the rotor position: it uses Hall-effect sensors or an encoder, or runs sensorless, inferring position from the back-EMF induced in the undriven winding. In trapezoidal control (six-step commutation) two of the three phases are energized at any instant. In sinusoidal control, typically using field-oriented control (FOC), the phase currents are modulated sinusoidally for smoother torque and quieter operation.
Problem solved
A classic brushed DC motor needs a mechanical commutator and brushes that wear down, spark, generate dust and electromagnetic interference and require periodic maintenance. This limits durability, efficiency and maximum speed and prevents operation in sealed or explosive environments. The BLDC motor solves this by moving the commutation function from the brushes to an electronic controller driven by rotor position.
Components
The rotating part carrying permanent magnets (often neodymium). In an inrunner it spins inside the stator, in an outrunner around it.
The stationary core with windings, usually three-phase in a wye (Y) or delta configuration, producing the rotating field.
The electronic controller with a transistor bridge (three-phase inverter) that switches the phase currents — the electronic equivalent of the commutator.
Official
Hall-effect sensors or an encoder that measure rotor position, or sensorless operation based on the back-EMF induced in the undriven winding.
Official
Implementation
At standstill there is no back-EMF, so a sensorless controller does not know the position and startup can be unreliable.
Incorrect phase advance relative to rotor position reduces torque and efficiency and can cause vibration.
Excess heat weakens the permanent magnets and damages winding insulation; power is thermally limited.
Interaction between magnets and stator slots causes torque ripple, troublesome at low speed.
Evolution
The development of solid-state electronics in the 1960s made it possible to replace the brush commutator with transistor switching.
The introduction of neodymium magnets substantially increased the power density and torque-to-weight ratio of brushless motors.
The spread of quasi-direct-drive actuators based on BLDC motors (e.g. in MIT legged robots) established BLDC as a standard in dynamic legged robotics.
Hyperparameters (configurable axes)
Number of rotor magnetic pole pairs; affects the electrical-to-mechanical speed ratio and torque.
RPM per volt (RPM/V) at no load; the inverse of the back-EMF constant Ke.
Torque per ampere of current; key for sizing robotic actuators.
Wye (Y) or delta; affects low-speed torque and top speed.
Trapezoidal (six-step commutation) or sinusoidal (usually FOC); affects torque smoothness and noise.