Iniciar sesión

Generators convert mechanical energy into electrical energy, whereas motors convert electrical energy into mechanical energy. A motor works by sending a current through a loop of wire located in a magnetic field. As a result, the magnetic field exerts a torque on the loop. This rotates a shaft, extracting mechanical work from the electrical current sent in initially. When the coil of a motor is turned, magnetic flux changes through the coil, and an emf (consistent with Faraday's law) is induced. The motor thus acts as a generator whenever its coil rotates. This happens whether the shaft is turned by an external input, like a belt drive, or by the action of the motor itself. When a motor is doing work, and its shaft is turning, an emf is generated. Lenz's law states that the emf opposes any change, so the input emf that powers the motor is opposed by the motor's self-generated emf, called the back emf of the motor.

The generator output of a motor is the difference between the supply voltage and the back emf. The back emf is zero when the motor is first turned on, meaning that the coil receives the full driving voltage, and the motor draws maximum current when it is on but not turning. As the motor spins faster, the back emf grows, always opposing the driving emf. This reduces the voltage across the coil and the amount of current it draws.

When a motor first comes on, it draws more current than when it runs at its normal operating speed. When a mechanical load is placed on the motor, like an electric wheelchair going up a hill, the motor slows, the back emf drops, more current flows, and more work can be done. If the motor runs at too low a speed, the larger current can overheat it, perhaps even burning it out. On the other hand, if there is no mechanical load on the motor, it increases its angular velocity until the back emf is nearly equal to the driving emf. Then the motor uses only enough energy to overcome friction.

Tags
Back EMFGeneratorsMotorsMechanical EnergyElectrical EnergyMagnetic FieldTorqueFaraday s LawInduced EmfLenz s LawSupply VoltageCurrent DrawMechanical LoadAngular VelocityFriction

Del capítulo 30:

article

Now Playing

30.18 : Back EMF

Electromagnetic Induction

2.5K Vistas

article

30.1 : Inducción

Electromagnetic Induction

3.7K Vistas

article

30.2 : Ley de Faraday

Electromagnetic Induction

3.7K Vistas

article

30.3 : Ley de Lenz

Electromagnetic Induction

3.3K Vistas

article

30.4 : Campos electromagnéticos de movimiento

Electromagnetic Induction

3.0K Vistas

article

30.5 : Dínamo de disco de Faraday

Electromagnetic Induction

1.9K Vistas

article

30.6 : Campos eléctricos inducidos

Electromagnetic Induction

3.4K Vistas

article

30.7 : Campos eléctricos inducidos: aplicaciones

Electromagnetic Induction

1.4K Vistas

article

30.8 : Corrientes de Foucault

Electromagnetic Induction

1.4K Vistas

article

30.9 : Corriente de desplazamiento

Electromagnetic Induction

2.7K Vistas

article

30.10 : Importancia de la corriente de desplazamiento

Electromagnetic Induction

4.2K Vistas

article

30.11 : Campos electromagnéticos

Electromagnetic Induction

2.0K Vistas

article

30.12 : La ecuación de Maxwell del electromagnetismo

Electromagnetic Induction

2.9K Vistas

article

30.13 : Simetría en las ecuaciones de Maxwell

Electromagnetic Induction

3.1K Vistas

article

30.14 : Ley de Ampere-Maxwell: Resolución de problemas

Electromagnetic Induction

438 Vistas

See More

JoVE Logo

Privacidad

Condiciones de uso

Políticas

Investigación

Educación

ACERCA DE JoVE

Copyright © 2025 MyJoVE Corporation. Todos los derechos reservados