Difficulty: Medium
Correct Answer: vp = (c / sqrt(μr * εr)) / sqrt(1 - (fc / f)^2)
Explanation:
Introduction / Context:
Unlike TEM transmission lines, waveguides support TE/TM modes with dispersive propagation. The phase velocity exceeds the medium wave speed as frequency approaches cutoff, a key concept in microwave engineering.
Given Data / Assumptions:
Concept / Approach:
The phase velocity in a waveguide is vp = ω / β. For TE/TM modes, β = k0 * sqrt(μr * εr) * sqrt(1 - (fc / f)^2), where k0 = ω / c. Therefore vp equals the medium wave speed divided by sqrt(1 - (fc/f)^2). Since the square root in the denominator is less than 1 above cutoff, vp exceeds the medium speed.
Step-by-Step Solution:
Verification / Alternative check:
Near cutoff (f → fc+), the denominator → 0+, so vp → ∞, consistent with dispersion theory. At high f ≫ fc, vp approaches the medium speed.
Why Other Options Are Wrong:
Option B inverts the dispersion; C and D misuse μrεr factors; E is dimensionally incorrect and ignores μr, εr.
Common Pitfalls:
Confusing phase velocity with group velocity; assuming vp cannot exceed c (it can; energy is carried at group velocity, not phase velocity).
Final Answer:
vp = (c / sqrt(μr * εr)) / sqrt(1 - (fc / f)^2)
Discussion & Comments