Electromagnetism - Lesson 2 – Applications of Induced Currents Part 2

Self-Inductance

  • EMF induced by changing magnetic field (external or from the wire itself).
  • Changing current in a coil induces an EMF opposing the change, reducing potential difference and net current.
  • Self-inductance: Property of a wire to create an induced EMF opposing the change in potential difference.
  • Self-inductance is the property of the current- carrying coil that resists or opposes the change of current flowing through it.

Transformers

  • Devices that increase or decrease potential differences (AC only).
  • Two coils (primary and secondary) electrically insulated but wound around the same iron core.
  • Changing current in primary coil creates a changing magnetic field, inducing a varying EMF in the secondary coil.
  • Mutual inductance: EMF and current in one coil due to changing current in another.
  • Step-up transformer: Secondary voltage > primary voltage.
  • Step-down transformer: Secondary voltage < primary voltage.
  • Isolation transformers: Primary and secondary coils have the same number of turns, with identical input and output potential differences, used for safety reasons.
  • Ideal transformer: P<em>p=P</em>sP<em>p = P</em>s
  • Transformer equation relates number of turns, currents, and potential differences: V<em>sV</em>p=N<em>sN</em>p\frac{V<em>s}{V</em>p} = \frac{N<em>s}{N</em>p}
  • In real transformers, some electrical energy is converted to thermal energy, reducing efficiency.
  • Efficiency is the ration of the output power to the input power.

Practical Applications of Transformers

  • Long-distance transmission uses high potential differences to reduce current and energy loss.
  • Step-up transformers increase voltage at power sources (e.g., up to 480,000 V).
  • Step-down transformers reduce voltage for consumer use (e.g., 120 V in homes).

Transmission of Electrical Energy

  • High voltage, low current minimizes power loss during long-distance transmission.

Transformer Problems

  • Step-up transformer example: Primary coil (200 turns, 90.0 V), secondary coil (3000 turns).
    • Secondary voltage: V<em>s=N</em>sN<em>pV</em>p=(3000)(90.0V)200=1350VV<em>s = \frac{N</em>s}{N<em>p}V</em>p = \frac{(3000)(90.0 V)}{200} = 1350 V
    • Secondary current is 2.0 A, primary current: I<em>p=V</em>sI<em>sV</em>p=(1350V)(2.0A)90.0V=3.0×101AI<em>p = \frac{V</em>sI<em>s}{V</em>p} = \frac{(1350 V)(2.0 A)}{90.0 V} = 3.0 \times 10^1 A