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Glossary

Braking Resistor

A resistor used to dissipate kinetic energy returned from a motor during deceleration in variable-frequency drives, servo systems, elevators, cranes and electric vehicles when regeneration to the grid is not possible.

Definition

Definition

When a motor decelerates an inertial load, the kinetic energy ½ J ω² flows back through the inverter and charges the DC bus capacitors. If unchecked, the DC bus voltage rises until the drive trips on over-voltage. The braking resistor absorbs this returned energy: a chopper IGBT (the “brake chopper”) switches the resistor across the bus whenever the voltage exceeds a threshold (typically 780 V on a 400 V AC drive), holding the bus at a safe level.

Sizing is governed by three numbers: peak power = ½ V_bus² / R, average power over the duty cycle, and single-event energy = ½ J × (ω₁² − ω₂²). The peak power must not exceed the resistor's pulse rating; the average must stay within the continuous power rating; the per-event energy must fit the thermal mass before the next deceleration. A 22 kW VFD typically uses a 4 – 8 Ω, 5 – 10 kW (peak), 1 – 2 kW (continuous) aluminum-housed brake resistor.

Applications include hoists, gantry cranes, centrifuges, machine-tool spindles, regenerative braking in EVs and trains. Because the resistor sees chopped DC at 1 – 16 kHz, non-inductive winding is preferred for low EMI. Thermal switches and over-temperature monitoring are standard safety features.

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