Electromagnetic Induction Notes

Electromagnetic Induction

11.1 Inducing Currents

  • Learning Objectives:

    • Identify how a changing magnetic field produces an electric current.
    • Define electromotive force.
  • Key Vocabulary:

    • Electric generator
    • Electromagnetic induction
    • Induced electromotive force
Changing Magnetic Fields
  • An electric current can be generated in a wire in a circuit when at least part of the wire moves through, and cuts, magnetic field lines.
  • Field lines can be cut when:
    1. A segment of wire moves through a stationary magnetic field.
    2. A magnetic field moves past a stationary wire.
    3. The strength of a magnetic field changes around a wire.
  • It is the relative motion between a wire and a magnetic field that can produce current.
  • Electromagnetic induction is the process of generating current through a wire in a circuit in a changing magnetic field.
Electromotive Force (EMF)
  • The potential difference given to the charges by a battery or a generator is called the electromotive force (EMF).
  • Electromotive force is not actually a force; instead, it is a potential difference and is measured in volts.
  • When you move a wire through a magnetic field, you exert a force on the charges, and they move in the direction of the force. Work is done on the charges.
  • Their electrical potential energy, and thus their potential, is increased.
  • This difference in potential is called the induced electromotive force (induced EMF).
Factors Affecting Induced EMF
  • The EMF of a wire moving in a magnetic field depends on:
    1. Magnetic field (B)
    2. The length of the wire in the magnetic field (L)
    3. Velocity of the wire in the field that is perpendicular to the field (vsin⁡θ)(v \sin \theta)
  • θ\theta: is the angle between B and v.
  • Remember Ohm's Law: EMF=BLvsin⁡θ\text{EMF} = BLv \sin \theta
Direction of Current
  • To find the force on the charges in the wire, use the fourth right-hand rule:
    • Hold your right hand so that your thumb points in the direction in which the wire is moving, and your fingers point in the direction of the magnetic field.
    • The palm of your hand will point in the direction of the conventional (positive) current.

Induced EMF in a Wire

  • Ohm's Law: I=ΔVRI = \frac{\Delta V}{R}

Example 1: Induced EMF

A straight wire is part of a circuit that has a resistance (R) of 0.50 Ω\Omega. The wire is 0.20 m long and moves at a constant speed of 7.0 m/s perpendicular to a magnetic field of strength 8.0×10−28.0 \times 10^{-2} T.

  • a. What EMF is induced in the wire?
    • EMF=BLv(sin⁡θ)EMF = BLv(\sin \theta)
  • b. What is the current through the wire?
    • I=EMFRI = \frac{EMF}{R}
  • c. If a different metal were used for the wire, increasing the circuit's resistance to 0.78 Ω\Omega, what would the new current be?
    • I=EMFRI = \frac{EMF}{R}

Induced EMF in Microphones

  • A microphone is a simple application that depends on an induced EMF to convert sound waves to electrical signals.
  • The microphone has a diaphragm attached to a coil of wire that is free to move in a magnetic field.
  • Sound waves vibrate the diaphragm, which moves the coil in the magnetic field, inducing an EMF across the ends of the coil.
  • The induced EMF varies as the frequency of the sound varies.
  • In this way, the sound wave is converted to an electrical signal.

Electric Generators

  • An electric generator converts mechanical energy to electrical energy.
  • An electric generator consists of a number of wire loops placed in a strong magnetic field. The wire may be wound around an iron core to increase the strength of the magnetic field (armature).
  • The armature is mounted so that it can rotate freely in the magnetic field.
  • As the armature turns, the wire loops cut through the magnetic field lines and induce an EMF.
  • When a generator is connected in a closed circuit, the induced EMF produces an electric current.
  • The EMF developed by the generator depends on the length of the wire rotating in the field.
  • Increasing the number of loops in the armature increases the wire length, which increases the induced EMF.
  • The direction of the induced current can be found from the third right-hand rule.
  • As the loop rotates, the strength and the direction of the current change.
  • The current is greatest when the loop’s velocity is perpendicular to the magnetic field.
  • As the loop rotates, it moves through the magnetic field lines at an ever-increasing angle. Thus, it cuts through fewer magnetic field lines per unit of time, and the current decreases.
  • When the loop is in the vertical position, the wire segments move parallel to the field, and the current is zero.
  • As the loop continues to turn, the segment that was moving up begins to move down and reverses the direction of the current in the loop.
  • This change in direction occurs each time the loop turns through 180°.
  • The current changes smoothly from zero to some maximum value and back to zero during each half-turn of the loop.
  • Then it reverses direction.
  • Generators and motors are almost identical in construction, but they convert energy in opposite directions.
  • A generator converts mechanical energy to electrical energy, while a motor converts electrical energy to mechanical energy.

Power in AC Circuits

  • The power produced by a generator is the product of the current and the voltage.
  • Because both current and voltage vary, the power associated with an alternating current varies.
  • Note that power is always positive because I and V are either both positive or both negative.
  • Average power, PAC, is half the maximum power:
    • P<em>Avg=P</em>AC=Pmax2P<em>{Avg} = P</em>{AC} = \frac{P_{max}}{2}

Effective Current and Voltage

  • It is common to describe alternating current and voltage in terms of effective current and voltage rather than referring to their maximum values.
  • I<em>eff=I</em>max2I<em>{eff} = \frac{I</em>{max}}{\sqrt{2}}
  • V<em>eff=V</em>max2V<em>{eff} = \frac{V</em>{max}}{\sqrt{2}}
  • Effective voltage is also commonly referred to as RMS (root mean square) voltage.
  • In the United States, Veff=120V_{eff} = 120 V for most wall outlets. The actual voltage oscillates at a rate of 60 Hz.
  • The frequency and effective voltage that are used vary in different countries.