Chapter 25: Electromagnetic Induction
Focus on Section 1: Inducing Currents
Oersted's Discovery: Demonstrated that an electric current produces a magnetic field.
Faraday's Hypothesis: Proposed that a magnetic field could induce an electric current.
Important Result: In 1822, Faraday determined that moving a wire through a magnetic field could induce electric current.
Joseph Henry's Contributions: Independently discovered that changing magnetic fields could also induce current but did not publish his findings.
The direction of current induced in a wire depends on the wire's motion relative to the magnetic field.
Key Conditions for Current Induction:
Wire must be stationary or moved parallel to the field—no current induced.
Current is induced if the wire moves perpendicular to the field.
Current direction reverses when the wire moves in the opposite direction.
Wire moves through stationary magnetic field.
Magnetic field moves past a stationary wire.
Change in strength of a magnetic field around a stationary wire.
Electromotive Force (EMF): Not an actual force but the potential difference that drives current flow, measured in volts.
EMF is generated when a wire moves through a magnetic field, creating an electric field due to the movement of charges within the wire.
Formula: EMF = BLv(sin A)
Induced Current: I = EMF / R
Use Right-Hand Rule:
Thumb: Direction of wire movement
Fingers: Direction of magnetic field
Palm: Direction of force (current flow on positive charges).
A straight wire part of a circuit moves at speed 7.0 m/s in a magnetic field (0.08 T).
a. Induced EMF: 0.112 V
b. Current: 0.224 A
c. Current with increased resistance (0.78 Ω): 0.144 A
Microphones convert sound to electrical energy via electromagnetic induction.
Components: Diaphragm, coil, magnetic field.
Sound waves cause diaphragm movement, inducing EMF in the coil.
Variations in induced current correspond to sound frequency.
Function: Converts mechanical energy to electrical energy.
Components: Wire loops, magnetic field, iron core (armature).
Wire loops cut through magnetic field lines, inducing EMF.
More loops increase the induced EMF.
Current varies as the generator's loop rotates.
Peak current occurs when wire moves perpendicular to the magnetic field.
Current decreases as wire moves parallel, becoming zero before reversing direction.
Formulas highlighted include EMF = vLBsinθ and I = EMF/R.
Angle (θ) significantly affects EMF values at different positions of rotation.
Common mechanical sources: wind, water, turbines.
Conventional power generation methods include steam, fossil fuels, and uranium fission.
Generators and motors have similar construction but function oppositely (energy conversion direction).
DC Generators: Direct current flows in one direction.
AC Generators: Use slip rings, producing alternating current, inducing current in a sinusoidal manner.
Effective current and voltage expressed as RMS (Root Mean Square).
Edison's DC distribution system vs. Tesla's AC system leading to the "war of the currents".
Edison's direct current system challenged by Tesla and Westinghouse’s alternating current system.
AC became prevalent due to its efficiency and delivery advantages.
Various questions provided to apply understanding of induced EMF and current generation.
Induced EMF calculation in different setups and resistances.
Clarification on misconceptions regarding AC and power dissipation in electrical devices.
Additional problems and application scenarios relating to generators, EMF calculations, and AC/DC systems.
Overview illustrations reflect varieties of electrical devices: microphones, generators, and motors.
Exploration of the relationship between electricity and magnetism, and the technology derived from these principles.