Study Notes on Fundamentals of Applied Electromagnetics

1. Pedagogical Overview and Resources
  • Authors: Fawwaz T. Ulaby and Umberto Ravaioli (8th Edition).

  • Core Objective: Bridging the gap between circuit analysis and electromagnetic field theory.

  • Interactive Learning: Inclusion of 52 web-based simulation modules (em8e.eecs.umich.edu) for visualizing wave propagation, transmission lines, and Smith charts.

  • Prerequisites: Proficiency in circuit analysis (Ohm’s Law, KCL, KVL) and multivariable calculus is required.

2. Historical Milestones in Electromagnetics
  • 1800: Alessandro Volta invents the first electric battery.

  • 1820: Hans Christian Ørsted discovers that electric current affects a magnetic compass needle.

  • 1830s: Michael Faraday demonstrates electromagnetic induction (V=NdΦdtV = -N \frac{d\Phi}{dt}).

  • 1873: James Clerk Maxwell publishes "A Treatise on Electricity and Magnetism," unifying the field.

  • 1888: Heinrich Hertz experimentally verifies the existence of electromagnetic waves.

3. Standards, Units, and Notation
  • SI Units (International System of Units):

    • Length: meter (mm)

    • Mass: kilogram (kgkg)

    • Time: second (ss)

    • Electric Current: ampere (AA)

    • Note: Charge is measured in Coulombs (CC), where 1C=1As1 C = 1 A \cdot s.

  • Notation Conventions:

    • Scalars: Written in italics (e.g., V,I,qV, I, q).

    • Vectors: Written in boldface (e.g., E,B,D,H\mathbf{E}, \mathbf{B}, \mathbf{D}, \mathbf{H}).

    • Phasors: Indicated by a tilde (e.g., V~,E~\tilde{V}, \tilde{\mathbf{E}}).

4. The Nature of Electromagnetism and Fundamental Forces
  • Lorentz Force Law: Describes the total force acting on a charge qq moving with velocity u\mathbf{u} in the presence of electric (E\mathbf{E}) and magnetic (B\mathbf{B}) fields:
    F=q(E+u×B)\mathbf{F} = q(\mathbf{E} + \mathbf{u} \times \mathbf{B})

  • Coulomb’s Law: The electrical force between two point charges q<em>1q<em>1 and q</em>2q</em>2: F=14πϵ<em>0q</em>1q2R2F = \frac{1}{4\pi\epsilon<em>0} \frac{q</em>1 q_2}{R^2}

    • Where Permittivity of free space ϵ08.854×1012 F/m\epsilon_0 \approx 8.854 \times 10^{-12} \text{ F/m}.

  • Field Categories:

    • Electrostatics: Fields produced by stationary charges (constant over time).

    • Magnetostatics: Fields produced by steady currents (dcdc).

    • Electrodynamics: Time-varying fields that produce electromagnetic waves.

5. Traveling Waves
  • General Wave Equation: A wave traveling in the +z+z direction is expressed as:
    y(z,t)=Acos(2πtT2<br>πzλ+ϕ0)y(z, t) = A \cos\left(\frac{2\pi t}{T} - \frac{2<br>π z}{\lambda} + \phi_0\right)

  • Key Parameters:

    • Amplitude (AA): Maximum value of the wave.

    • Phase Velocity (u<em>pu<em>p): The speed of wave propagation: u</em>p=fλ=ωku</em>p = f\lambda = \frac{\omega}{k}.

    • Angular Frequency (ω\omega): ω=2πf=2<br>πT\omega = 2\pi f = \frac{2<br>π}{T}.

    • Wavenumber (kk): k=2<br>πλk = \frac{2<br>π}{\lambda}.

    • Phase (ϕ\phi): The argument of the cosine function: (ωtkz+ϕ0)(\omega t - kz + \phi_0).

6. The Electromagnetic Spectrum
  • Speed of Light (cc): In vacuum, c3×108 m/sc \approx 3 \times 10^8 \text{ m/s}.

  • Frequency-Wavelength Relationship: c=fλc = f \lambda.

  • Spectrum Segments: Ranges from Gamma rays (high frequency, short wavelength) to Radio waves (low frequency, long wavelength).

7. Complex Number Review and Phasor Analysis
  • Representations:

    • Rectangular: z=x+jyz = x + jy

    • Polar: z=zejθ=z(cosθ+jsinθ)z = |z|e^{j\theta} = |z|(\cos \theta + j \sin \theta)

    • Identity: j=1,j2=1,1j=jj = \sqrt{-1}, j^2 = -1, \frac{1}{j} = -j

  • Phasor Transformation:

    • To solve time-harmonic problems, time-domain functions are converted to phasors:
      v(t)=V<em>mcos(ωt+ϕ)V~=V</em>mejϕv(t) = V<em>m \cos(\omega t + \phi) \leftrightarrow \tilde{V} = V</em>m e^{j\phi}

    • Linearity: Phasor analysis allows differential equations describing the system to be converted into much simpler linear algebraic equations.