Detailed Study Notes on Electromagnetism

Introduction to Electromagnetic Fields

  • Electromagnetic fields cannot exist separately as purely electric or purely magnetic; they generate from one another.
  • The topic to be covered next is the electromagnetic field.

Announcements

  • Homework is due tonight.

Recap from Last Class

Induced Fields
  • Induced fields refer to electric or magnetic fields created as a result of changes in their counterparts.
    • When a charged particle creates a magnetic field, this is called an induced magnetic field.
    • Conversely, a change in the magnetic field induces an electric field, termed the induced electric field.
  • The relationship between electric and magnetic fields:
    • They are perpendicular to each other and generate each other, which is the basis for electromagnetic waves.

AC Generation

Principles of AC Generators
  • AC generation involves changing the magnetic flux linked to a coil which induces an electric field or EMF (Electromotive Force).
    • Magnetic flux can be changed by rotating a coil within a magnetic field, such as in hydroelectric power where water rotates a turbine.
  • The rotation of this coil generates alternating current (AC) because:
    • Every cycle of rotation generates a voltage.
Transformers
  • A transformer is a device that adjusts voltage levels.
    • After generating electricity at 11,000 volts, it is often necessary to step the voltage down for practical use.

Inductance

Understanding Inductance
  • Inductance refers to the property of a coil that results from a change in current.
    • This change can be in the current's direction or in its flow rate.
  • Due to Lenz's Law, the induced EMF will act in opposition to the change causing it.
    • For practical applications, inductance can be used in magnetic braking systems.
  • The energy stored in an inductor is given by: E=12LI2E = \frac{1}{2} L I^2
    • Here, L is the inductance.
Energy Density
  • Energy density in magnetic fields is important when considering LC (inductor-capacitor) circuits, which can exhibit alternating signals.

LR Circuit Analysis

Composition of LR Circuits
  • An LR circuit consists of an inductor (L) and a resistor (R).
    • Kirchhoff's loop law can be applied for circuit analysis:
    • The induced EMF $E = L \frac{dI}{dt}$.
  • Expressing initial conditions: II0=eRLt\frac{I}{I_0} = e^{-\frac{R}{L}t}
    • Integration can help determine current behavior as the switch is turned on or off.
    • The time constant ( \tau ) is given by:
      τ=LR\tau = \frac{L}{R}
Current Decay Calculation
  • To calculate time when current decays to 1% of its initial value:
    • Setting $I = 0.01 I_0$ gives:
      0.01=etτ0.01 = e^{-\frac{t}{\tau}}
    • Taking logarithms leads to:
      ln(0.01)=tτ-\ln(0.01) = \frac{t}{\tau}

Electromagnetics Overview

Electromagnetic Fields and Waves

  • The electric field and magnetic field are interconnected. Changing electric fields generate changing magnetic fields, leading to electromagnetic waves.
Frame of Reference and Field Perception
  • Observations of electric and magnetic fields depend on the observer’s reference frame:
    • Example:
    • Observer A (stationary) perceives a moving charge generating a magnetic field.
    • Observer B (moving with the charge) sees it as stationary; he experiences only electric fields.

Transformations of Fields

Transforming Electric and Magnetic Fields
  • Transformations occur between fields in stationary and moving frames:
    • A charge experiencing motion in a magnetic field will perceive electric fields differently based on the frame of reference.
Galilean Transformations
  • The relationship between electric and magnetic fields as they transform between different reference frames is as follows:
    • Electric field in moving frame:
      E=E+v×BE' = E + v \times B
    • Magnetic field in moving frame:
      B=B1c2(v×E)B' = B - \frac{1}{c^2} (v \times E)
    • Here, ( c ) is the speed of light, and ( v ) is the velocity of the reference frame.

Laws of Electromagnetics

Faraday's Law of Induction

  • States that a change in magnetic flux will induce an EMF:
    E=dΦdtE = -\frac{d\Phi}{dt}
  • Faraday's Law implies that movement through a magnetic field creates induced voltage.

Ampere's Law and Extensions

  • Ampere's Law relates magnetic fields to currents:
    Bdl=μ<em>0I</em>enc\oint B \cdot dl = \mu<em>0 I</em>{enc}
  • Maxwell introduced a modification to Ampere's Law to include displacement current, leading to:
    Bdl=μ<em>0(I+ϵdΦ</em>Edt)\oint B \cdot dl = \mu<em>0 (I + \epsilon \frac{d\Phi</em>E}{dt})
  • Where ( \Phi_E ) is the electric flux.

Maxwell's Equations

  • Maxwell's equations unite electricity and magnetism, composing:
    • Gauss's Law for Electricity
    • Gauss's Law for Magnetism
    • Faraday's Law of Induction
    • Maxwell-Ampère Law
  • These equations describe how electric and magnetic fields propagate and interact, yielding electromagnetic waves.