Electromagnetic Fields and Waves Flashcards
7 cards from real BEE practice questions. Tap to flip, then mark Knew It or Still Learning — missed cards come back until you master them.
Read the first 7 Electromagnetic Fields and Waves flashcards as text
The voltage standing-wave ratio (VSWR) on a transmission line terminated with a short circuit is:
Answer: Infinity (∞)
A short circuit creates a reflection coefficient Γ = -1 (|Γ| = 1), so VSWR = (1+1)/(1-1) → ∞.
Snell's Law of refraction for electromagnetic waves at a planar interface states:
Answer: n₁ sin θ₁ = n₂ sin θ₂
The phase-matching condition at the boundary requires n₁ sin θ₁ = n₂ sin θ₂, identical to optics.
Magnetic vector potential A is defined such that:
Answer: B = ∇ × A
Since ∇ · B = 0, B can always be written as the curl of a vector potential A.
For a lossy transmission line, the propagation constant γ = α + jβ. At very high frequencies in a good conductor, α ≈ β. This means the wave:
Answer: Attenuates by 1/e over exactly one wavelength/2π
When α = β = 1/δ (skin depth formula), the wave decays by e⁻¹ over a distance equal to 1/α = δ ≈ λ/2π inside the conductor.
Image theory in electromagnetics replaces a ground plane conductor with:
Answer: A mirror-image charge of opposite sign at the same depth below the surface
Image theory removes the conductor by placing an opposite charge at the mirror-image position, reproducing the correct boundary conditions above the surface.
The wave equation for E in a source-free, lossless medium is:
Answer: ∇²E - με ∂²E/∂t² = 0
Combining Faraday's and Ampere's laws yields the vector wave equation ∇²E = με ∂²E/∂t² (zero on one side).
The radiation resistance of a half-wave dipole antenna in free space is approximately:
Answer: 73 Ω
The half-wave dipole has a radiation resistance of ≈ 73 Ω, which is why it is commonly fed with 75 Ω coaxial cable.