Single-phase half-wave controlled rectifier with resistive load As the firing angle α increases, how do the DC output voltage and the RMS output voltage change?

Difficulty: Easy

Correct Answer: Both decrease (not in the same proportion)

Explanation:


Introduction / Context:
Phase control changes the conduction interval of a controlled rectifier. For a purely resistive load in a half-wave circuit, increasing the firing angle delays conduction, thereby reducing both the average (DC) and the RMS values of the output.


Given Data / Assumptions:

  • Input: v(t) = Vm sin(ωt).
  • Resistive load (no energy storage).
  • Conduction over θ ∈ [α, π] each cycle.


Concept / Approach:

Average and RMS values are computed by integrating the output over the effective conduction interval. As α increases, the interval shortens. The RMS depends on the square of the waveform, so it does not scale linearly with the average.


Step-by-Step Solution:

V_dc = (Vm / 2π) * (1 − cos α) for a half-wave controlled rectifier.V_rms^2 = (1 / 2π) * ∫_α^π Vm^2 sin^2 θ dθ = (Vm^2 / 4π) * (π − α + sin 2α / 2).As α increases, both V_dc and V_rms decrease, but with different mathematical dependences (linear in 1 − cos α vs. a combination of interval and sin 2α term).


Verification / Alternative check:

Check limiting cases: α = 0 gives maximum V_dc and V_rms; α → π gives both tending to zero.


Why Other Options Are Wrong:

“Increase” options contradict the physics of delayed conduction; “same proportion” is incorrect due to differing functional forms.


Common Pitfalls:

Confusing average with RMS or assuming a fixed proportionality between them; forgetting the squared nature of RMS calculation.


Final Answer:

Both decrease (not in the same proportion)

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