electromagnetic effects

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ELECTROMAGNETIC EFFECTS

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ELECTROMAGNETIC EFFECTS. THE MOTOR EFFECT. Current-carrying wires in an external magnetic field experience a force, dependent on B, I, l and the angle between wire and B field. F = Bilsin θ This is the basis of electric motors and analogue electric meters. CATHODE RAY TUBES. - PowerPoint PPT Presentation

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Page 1: ELECTROMAGNETIC EFFECTS

ELECTROMAGNETIC EFFECTS

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1. Current-carrying wires in an external magnetic field experience a force, dependent on B, I, l and the angle between wire and B field.

F = Bilsinθ

This is the basis of electric motors and analogue electric meters.

THE MOTOR EFFECT

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CATHODE RAY TUBES

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This is the basis of the old cathode ray tube TV’s and computer monitors (and oscilloscopes). F = qvBsinθ

Free charges also experience a force in a magnetic field.

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Moving a wire in a magnetic field can produce a voltage in the wire, and thus a current. Moving a magnet around a wire does the same thing.

Key concept: if the flux (amount of magnetic flow or amount of magnetic field lines) changes around a conductor, then a voltage is produced across the ends of the conductor.

Φ = B A cosθ

Electromagnetic induction

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The faster the flux changes, the higher the voltage.

There will be opposition to flux change. As we change flux, a voltage (emf) is generated in the wire, that opposes the change we are making. (Lenz’ Law).

Every loop of wire exposed to a changing flux experiences its own emf across its ends. If the loops are in series, we add the emfs.

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All together,

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These concepts of changing flux associated with a wire are used in electric generators.

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The voltage produced (and so also the current) will be an alternating current (AC).

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Generators must supply power to distant places. How is this done? To reduce heat losses, it is better to send the electric current with a low I and high V, rather than high I and low V. To do this a transformer is needed.

Vp/Vs = Np/Ns

VpIp = VsIs

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A last look at electric motors:When a motor starts up, lights often dim.

Why is this? When the motor starts, there is a maximum

current flow due to the high emf across the motor. As the motor speeds up, a back emf is induced (coils rotating in a magnetic field) in the coils, that opposes the forward emf. The back emf reaches a maximum when the motor is turning at full speed. This reduces the overall emf across the motor. The current is also reduced, and the lights elsewhere get more current again.