Difficulty: Easy
Correct Answer: -45°
Explanation:
Introduction / Context: First-order dynamics are ubiquitous in process units (tanks, heat exchangers). Their frequency response is simple yet powerful: knowing the phase shift and attenuation at a given frequency helps in controller tuning and estimating closed-loop behaviour. This question focuses on computing the phase at a specific frequency using the well-known formula for a first-order lag.
Given Data / Assumptions:
Concept / Approach: For G(jω) = K / (1 + jωτ), the phase is φ(ω) = −tan^−1(ωτ). This is independent of K. Substituting τ = 1 and ω = 1 gives φ = −tan^−1(1) = −45°. The negative sign indicates the output lags the input, characteristic of a causal lag element.
Step-by-Step Solution:
Write the phase formula: φ = −tan^−1(ωτ).Insert values: ωτ = 1 * 1 = 1.Compute: tan^−1(1) = 45°.Attach sign: output lags → φ = −45°.Verification / Alternative check: The magnitude at this frequency is |G(j1)| = K / √(1 + 1^2) = K/√2, confirming a −3 dB point when ω = 1/τ. The corner frequency 1/τ = 1 rad/min also typically corresponds to a −45° phase, consistent with the result.
Why Other Options Are Wrong:
45° — sign error; the lag is negative.−90° — would be the asymptotic phase at very high frequency for a first-order lag, not at ω = 1/τ.−180° — never reached by a single first-order lag.0° — only at ω → 0.Common Pitfalls: Forgetting the negative sign (lag), or confusing the break frequency with the high-frequency asymptote.
Final Answer: −45°
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