Dashboard Deep Learning Electrical Machines Special machines Brushless DC (BLDC) motors

Brushless DC (BLDC) motors

Inverted DC: stator 3-φ windings + rotor PM. Trapezoidal back-EMF (vs PMSM sinusoidal), 6-step commutation via 3 Hall sensors, T = k_t·I torque law. Drones, EVs, HDDs, power tools.

Junior ~11 min

Step 1 — BLDC = inverted DC motor: electronic commutation replaces brushes

0.55×
sector T Halls

Reference notes

A brushless DC (BLDC) motor is an "inverted" brushed DC machine — windings move to the stator, magnets to the rotor, and the mechanical commutator is replaced by an electronic inverter. Use Next → to walk through construction, the trapezoidal back-EMF that defines a BLDC (vs sinusoidal PMSM), six-step commutation via Hall sensors, the torque equation, and where BLDC fits among neighboring machine types.

BLDC = inverted brushed DC

Construction

Trapezoidal back-EMF — the defining waveform

The fingerprint of a BLDC is its trapezoidal back-EMF: each stator phase sees a back-EMF e(θ) that is flat-topped for ~120 electrical degrees per half-cycle. This is engineered via magnet pole-arc shaping and concentrated stator winding placement. Compare to a PMSM (permanent-magnet synchronous motor), physically very similar but designed with distributed windings and shaped magnets to produce a perfectly sinusoidal back-EMF.

The trapezoidal shape is what permits simple six-step (square-wave) commutation while keeping torque ripple manageable.

Six-step commutation

Sector boundaries occur every 60 electrical degrees; current always flows through 2 phases series-connected by the inverter

Torque equation

Because trapezoidal e(θ) × square i(θ) ≈ constant instantaneous power during the flat region, BLDC torque follows the same simple linear law as a brushed DC motor:

T = kt · I, E = ke · ω

In SI units, kt and ke are numerically equal (consequence of energy conservation). Steady-state speed at terminal voltage V:

ω ≈ (V − I · R) / ke

Speed control is therefore voltage control, same as brushed DC, but without the brushes-and-commutator maintenance penalty.

BLDC vs neighbors

Field weakening

Above base speed, advancing the commutation angle relative to the rotor position effectively weakens the air-gap flux — same principle as separately-excited DC motor field weakening. Allows constant-power operation above base speed at reduced torque. Used in EV traction inverters and high-speed spindle drives.

Sensorless BLDC

The 3 Hall sensors can be eliminated for cost-sensitive applications. The inverter monitors the back-EMF in the currently-floating phase and uses zero-crossings of e(θ) to infer rotor position. Works well above ~10 % rated speed; below that, special starting algorithms are needed (open-loop ramping, high-frequency injection, or short-pulse inductance sensing). Used in nearly all hard drives and many drone ESCs.

Take-away. BLDC moves the windings to the stator and the magnets to the rotor, replacing brushes with an electronic inverter. Trapezoidal back-EMF lets simple 6-step commutation (driven by 3 Hall sensors) produce constant torque using square-wave 2-phase-on currents. Torque law is the same as brushed DC (T = kt·I). Result: high efficiency, sealed operation, dominant from fractional HP up to ~100 kW. PMSM is the smoother-torque cousin; induction is the rare-earth-free alternative for large drives.

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