Difficulty: Easy
Correct Answer: increasing distributed inductance of line
Explanation:
Introduction / Context:
In wireline telephony and low-frequency RF practice, the term “loading” has a precise historical meaning: adding inductance to a line to improve its transmission over distance. Understanding what parameter is changed—and how it is changed—helps interpret classic loading-coil designs and modern distributed implementations.
Given Data / Assumptions:
Concept / Approach:
A transmission line is characterized by per-unit-length R, L, G, and C. “Loading” specifically targets the series inductance L to shape the propagation constant and characteristic impedance. Increasing L (either by coils at spacing d, or continuously with magnetic materials or conductor geometry) flattens the attenuation over the voice band and pushes the line toward distortionless conditions (R/L ≈ G/C). Thus, the correct description is an increase of distributed inductance.
Step-by-Step Solution:
Verification / Alternative check:
Classical Heaviside condition for distortionless transmission is R/L = G/C. If R and G are fixed, increasing L can help meet the condition in the operating band, which corroborates the purpose of loading.
Why Other Options Are Wrong:
“Increasing inductance of line” (generic) omits the crucial notion of per-unit-length distribution and could be misconstrued as a single lump; “decreasing” variants contradict the observed practice; “adding shunt capacitance” increases C and is the opposite of classical inductive loading.
Common Pitfalls:
Confusing lumped one-time inductors with periodic/distributed loading; assuming loading improves high-frequency bandwidth (it typically narrows usable HF response while improving voice-band behavior).
Final Answer:
increasing distributed inductance of line
Discussion & Comments