Electromagnetic Induction, AC Circuits, and Electrical Technologies

46 Induced Emf and Magnetic Flux

Learning Objectives

  • Calculate the magnetic flux of a uniform magnetic field through a loop with any orientation.
  • Describe how changing magnetic fields can produce an electromotive force (emf) in a loop of wire.

In the previous chapter, we learned that electric currents produce magnetic fields. Michael Faraday showed that the reverse process is also possible: a changing magnetic field can produce an electromotive force (emf) and, when a closed conducting path is available, an electric current.

Faraday’s original apparatus is shown in Figure 46.1. A battery and switch are connected to the upper coil wrapped around an iron ring. When the switch is closed, current begins to flow through the upper coil and creates a magnetic field in the iron ring. The changing magnetic field passes through the lower coil, which is connected to a galvanometer that detects electric current.

Each time the switch is closed, the galvanometer briefly indicates a current in one direction. When the switch is opened, it briefly indicates a current in the opposite direction. However, if the switch remains either open or closed, the galvanometer returns to zero. A steady magnetic field does not continue to induce an emf. It is the change in the magnetic field that produces the emf.

Faraday's apparatus consists of two coils wrapped around an iron ring. The upper coil is connected to a battery and switch. The lower coil is connected to a galvanometer. Opening or closing the switch changes the magnetic field in the ring and briefly induces current in the lower coil.
Figure 46.1: Faraday’s apparatus for demonstrating electromagnetic induction. Opening or closing the switch changes the magnetic field produced by the upper coil. This changing field induces an emf and a temporary current in the lower coil. No current is induced while the magnetic field remains constant.

A simpler experiment is shown in Figure 46.2. When a bar magnet is moved into or out of a coil, an emf is induced in the wire. Moving the magnet in opposite directions produces emfs with opposite signs. Reversing the magnet’s poles also reverses the direction of the induced emf.

The result is the same if the coil moves while the magnet remains still. What matters is the relative motion between the magnet and the coil. Moving the magnet or coil more quickly produces a larger emf because the magnetic conditions change more rapidly. When the magnet and coil are stationary relative to each other, no emf is induced.

Five diagrams show a bar magnet moving relative to a coil connected to a galvanometer. Moving the north pole toward the coil induces current in one direction, while moving it away reverses the current. Repeating the motion with the south pole reverses the current directions. Holding the magnet stationary produces no galvanometer deflection.
Figure 46.2: Relative motion between a magnet and a coil induces an emf. Reversing the direction of motion or reversing the magnet’s poles reverses the induced current. Faster motion produces a larger emf, while no emf is produced when the magnet and coil remain stationary relative to one another.

Most electric generators use a related method, illustrated in Figure 46.3. A coil rotates inside a magnetic field. As the coil turns, its orientation relative to the field continually changes, producing an alternating emf. Mechanical work used to rotate the coil is therefore converted into electrical energy.

A generator is similar in construction to an electric motor, but the direction of energy conversion is reversed. A motor converts electrical energy into mechanical motion, whereas a generator converts mechanical motion into electrical energy.

A rectangular coil rotates between the north and south poles of a magnet. The coil is attached to an axle and connected through rings and brushes to a galvanometer. Rotation changes the orientation of the coil in the magnetic field and induces an electric current.
Figure 46.3: Rotation of a coil in a magnetic field produces an emf. This is the basic operating principle of an electric generator, in which mechanical energy is converted into electrical energy.

Magnetic Flux

The previous experiments show that an emf is produced whenever the magnetic conditions through a loop change. To describe this quantitatively, we use a quantity called magnetic flux, represented by the Greek letter [latex]\Phi[/latex].

For a uniform magnetic field passing through a flat area, magnetic flux is defined as

[latex]\Phi=BA\cos\theta,[/latex]

where

  • [latex]B[/latex] is the magnetic field strength,
  • [latex]A[/latex] is the area of the loop or surface, and
  • [latex]\theta[/latex] is the angle between the magnetic field and the line perpendicular to the surface.

The angle is measured from the magnetic field to the normal, an imaginary line perpendicular to the surface. This is important because magnetic flux depends only on the component of the magnetic field that passes directly through the surface.

A uniform magnetic field B passes through a flat surface of area A. The field makes an angle theta with the normal, a line perpendicular to the surface. The perpendicular component of the magnetic field is B cosine theta.
Figure 46.4: Magnetic flux depends on the magnetic field strength, the area of the surface, and the angle between the magnetic field and the normal to the surface. Only the perpendicular component, [latex]B\cos\theta[/latex], contributes to the flux.

The perpendicular component of the magnetic field is

[latex]B_{\perp}=B\cos\theta.[/latex]

Therefore, magnetic flux can also be written as

[latex]\Phi=B_{\perp}A.[/latex]

The SI unit of magnetic flux is the tesla–meter squared,

[latex]\text{T}\cdot\text{m}^{2},[/latex]

which is also called the weber (Wb).

Magnetic flux is greatest when the magnetic field is perpendicular to the surface. In that case, the field is parallel to the normal, so [latex]\theta=0^\circ[/latex] and [latex]\cos\theta=1[/latex]. The flux is then

[latex]\Phi=BA.[/latex]

If the magnetic field lies parallel to the surface, it is perpendicular to the normal. Then [latex]\theta=90^\circ[/latex], [latex]\cos\theta=0[/latex], and the magnetic flux is zero even though the magnetic field itself is not zero.

A change in magnetic flux can be produced in several ways:

  • changing the magnetic field strength [latex]B[/latex],
  • changing the area [latex]A[/latex] through which the field passes, or
  • changing the angle [latex]\theta[/latex] between the field and the surface normal.

Any change in magnetic flux can induce an emf. This process is called electromagnetic induction.

In Faraday’s apparatus, opening and closing the switch changes the magnetic field strength. Moving a magnet relative to a coil changes the field passing through the coil. Rotating a generator coil changes the angle between the coil and the magnetic field. Although these situations appear different, they all produce an emf by changing the magnetic flux.

Electromagnetic induction is also important in healthcare technology. Changing magnetic fields induce signals in the receiver coils of MRI systems, allow wireless charging of some implanted and portable medical devices, and are used in sensors that monitor motion, position, and physiological activity.

Section Summary

  • Magnetic flux, represented by [latex]\Phi[/latex], is defined as
    [latex]\Phi=BA\cos\theta,[/latex]

    where [latex]B[/latex] is the magnetic field strength, [latex]A[/latex] is the area of the surface, and [latex]\theta[/latex] is the angle between the magnetic field and the line perpendicular (normal) to the surface.

  • The SI unit of magnetic flux is the tesla–meter squared,
    [latex]\mathrm{T}\cdot\mathrm{m}^2[/latex], also known as the weber (Wb).
  • Electromagnetic induction occurs whenever the magnetic flux through a conducting loop changes. A change in magnetic field strength, loop area, or orientation can all induce an electromotive force (emf).

Conceptual Questions

  1. How do the multiple-loop coils and iron ring in Faraday’s apparatus shown in Figure 46.1 enhance the observation of the induced emf?
  2. When a magnet is thrust into a coil as shown in Figure 46.2(a), what is the direction of the force exerted by the coil on the magnet? Draw a diagram showing the direction of the induced current and the magnetic field produced by the coil to justify your response. How does the magnitude of the force depend on the resistance of the galvanometer?
  3. Explain how magnetic flux can be zero even when the magnetic field is not zero.
  4. Is an emf induced in the coil shown in Figure 46.5 when it is stretched? If so, explain why and determine the direction of the induced current.
    A circular wire loop is stretched by two hands while it remains in a uniform magnetic field directed into the page. Stretching the loop changes the area enclosed by the wire.
    Figure 46.5: A circular coil of wire is stretched while it remains in a magnetic field directed into the page.

Problems & Exercises

  1. What is the value of the magnetic flux through coil 2 in Figure 46.6(a) due to the magnetic field produced by coil 1?
    Figure (a) shows two single-loop coils whose planes are perpendicular to one another. Coil 1 is vertical and carries a counterclockwise current, while coil 2 is horizontal. Figure (b) shows a vertical straight wire carrying current upward next to a horizontal single-loop coil.
    Figure 46.6: (a) The planes of the two coils are perpendicular. (b) The straight wire is perpendicular to the plane of the coil.
  2. What is the value of the magnetic flux through the coil in Figure 46.6(b) due to the magnetic field produced by the straight wire?

Glossary

magnetic flux
A measure of the magnetic field passing through a surface. For a uniform magnetic field, the magnetic flux is given by
[latex]\Phi=BA\cos\theta[/latex],
where [latex]B[/latex] is the magnetic field strength,
[latex]A[/latex] is the area of the surface, and
[latex]\theta[/latex] is the angle between the magnetic field and the line perpendicular (normal) to the surface.
electromagnetic induction
The process of producing an electromotive force (emf) by changing the magnetic flux through a conductor or conducting loop.
definition

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Introductory Physics for the Health and Life Sciences II Copyright © 2012 by OSCRiceUniversity is licensed under a Creative Commons Attribution 4.0 International License, except where otherwise noted.