Difficulty: Easy
Correct Answer: Correct
Explanation:
Introduction / Context:First-order RC low-pass filters are fundamental in smoothing, anti-aliasing, and bandwidth limiting. The hallmark of a low-pass is that it passes low frequencies with little attenuation and attenuates high frequencies. This question verifies that intuition for the common configuration with output across the capacitor.
Given Data / Assumptions:
Concept / Approach:The transfer function is H(jω) = 1 / (1 + jωRC). Its magnitude |H(jω)| = 1 / sqrt(1 + (ωRC)^2). As frequency increases, the denominator grows, so the magnitude decreases. Therefore, the output amplitude drops with higher input frequency, which is exactly what a low-pass filter is designed to do.
Step-by-Step Solution:
Write H(jω) = 1 / (1 + jωRC). Compute magnitude: |H| = 1 / sqrt(1 + (ωRC)^2). Observe monotonic decrease with increasing ω. Conclude the statement is correct for this configuration.Verification / Alternative check:At ω = 0, |H| = 1 (no attenuation). At ω = ω_c, |H| = 1/√2 (−3 dB). As ω → ∞, |H| → 0. Scope measurements on a simple RC confirm the roll-off behavior.
Why Other Options Are Wrong:Incorrect: contradicts the low-pass definition. Inductive loads / frequency constraint options do not alter the basic monotonic trend for the ideal RC low-pass with output across C.
Common Pitfalls:Confusing the low-pass with the high-pass (output taken across R); forgetting that loading by the next stage can shift the effective corner frequency.
Final Answer:Correct
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