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Back EMF is an induced electromotive force that opposes the applied voltage in a motor. When a current-carrying coil rotates inside a magnetic field, the changing magnetic flux through the coil induces an EMF according to Faraday's law. By Lenz's law, this induced EMF opposes the current causing the rotation, hence the name back EMF.

Back EMF reduces the current available to drive the motor. The total voltage for supplying current equals the applied voltage minus the back EMF. When a motor starts, back EMF is zero, allowing maximum current through the coil. As the coil rotates faster, back EMF increases, reducing the net voltage and current draw proportionally.

When a motor is first turned on, the induced back EMF is zero because the coil is not yet rotating. Without back EMF to oppose it, the full applied voltage drives through the coil's resistance, producing maximum current. As the motor accelerates and the coil begins rotating, back EMF builds up and reduces the current draw.

When a mechanical load slows the motor, the back EMF decreases because the coil rotates more slowly. With lower back EMF, more current flows through the coil, enabling the motor to produce additional torque and perform more work. However, excessive current from sustained low speed can overheat and damage the motor.

Back EMF increases with motor speed, approaching the applied voltage at maximum speed. When back EMF nearly equals the driving EMF, the motor uses minimal current and energy, overcoming only friction losses. This high-speed, low-current condition represents efficient operation, while low-speed operation draws excessive current and generates heat.

Yes, use the formula: Current = (Applied Voltage − Back EMF) / Resistance. For example, at 100 volts applied with 20 ohm resistance and 50 volts back EMF, the current is (100 − 50) / 20 = 2.5 amperes. This demonstrates how back EMF directly reduces the current available to drive the motor's mechanical output.

A motor acts as a generator because rotating the coil through a magnetic field changes the magnetic flux, inducing an EMF consistent with induced electric fields. This self-generated EMF is the back EMF. Whether the shaft rotates from the motor's own torque or external input like a belt drive, the changing flux produces an induced voltage opposing the applied voltage.