Introduction / Context:
Fourier analysis of inverter waveforms is central to designing filters and estimating fundamental RMS values. In a half-bridge, the output toggles between +V/2 and −V/2, producing a square wave whose fundamental must be extracted for RMS calculations.
Given Data / Assumptions:
- Ideal half-bridge with amplitude levels ±V/2.
- Pure square wave, 50% duty, no dead-time or device drop.
- We seek RMS of the fundamental component only (not total RMS).
Concept / Approach:A symmetrical square wave of peak amplitude A has a fundamental (sine) component with peak value V1_peak = 4A/π. The RMS of the fundamental is V1_rms = V1_peak/√2 = (4A/π)/√2 = (2√2/π) * A.
Step-by-Step Solution:1) Here A = V/2.2) V1_peak = 4*(V/2)/π = 2V/π.3) V1_rms = (2V/π)/√2 = (√2/π)V ≈ 0.450V.Verification / Alternative check:Compare with full-bridge where amplitude is ±V, yielding fundamental RMS (2√2/π) * (V/2) * 2? For half-bridge, halving the level halves the fundamental magnitude relative to a ±V square wave, so 0.450V is consistent.
Why Other Options Are Wrong:- 2V: Dimensionally incorrect for RMS of a component.
- V/√2: That is the RMS of a sinusoid with peak V, not applicable here.
- V/2: Not the fundamental RMS; it is just the DC magnitude half, irrelevant here.
- (2/π) * V ≈ 0.637V: That is the average of a ±V square wave magnitude, not the fundamental RMS.
Common Pitfalls:- Confusing total RMS of square wave with fundamental RMS.
- Dropping the factor of 1/2 for half-bridge amplitude.
Final Answer:(√2/π) * V (≈ 0.450 V) (Option B).
Discussion & Comments