Single-phase fully controlled bridge feeding an R–L–E load (continuous current) Given v_s(t) = Vm sin(ωt), firing angle α, and average current I0, which relation is correct?

Difficulty: Medium

Correct Answer: cos α = (π/(2Vm)) * (R I0 + E)

Explanation:


Introduction / Context:
For a fully controlled bridge supplying an R–L–E load (e.g., a DC motor back-emf), the average DC output voltage depends on firing angle α and equals the sum of the average resistive drop and the back-emf. This relation is the cornerstone for speed and torque control in drives.


Given Data / Assumptions:

  • Input: v_s(t) = Vm sin(ωt).
  • Fully controlled bridge (four SCRs), continuous current.
  • Ideal devices, no overlap; average load current = I0; series R and back-emf E.


Concept / Approach:

For continuous current and no overlap, the average output voltage is V_avg = (2Vm/π) cos α. KVL for the DC side gives V_avg = R I0 + E. Combining these two expressions yields the desired relation for cos α in terms of R, I0, E, and Vm.


Step-by-Step Solution:

Use converter average: V_avg = (2Vm/π) * cos α.Use DC KVL: V_avg = R I0 + E.Equate: (2Vm/π) * cos α = R I0 + E.Solve for cos α: cos α = (π/(2Vm)) * (R I0 + E).


Verification / Alternative check:

Limit checks: with E = 0 and α = 0°, cos α = 1 ⇒ V_avg = 2Vm/π, the well-known maximum. Increasing α reduces V_avg linearly with cos α as expected.


Why Other Options Are Wrong:

Options with incorrect proportionality (e.g., multiplied by 2Vm/π instead of divided) or sign errors (E − R I0) do not satisfy both the converter equation and DC KVL simultaneously.


Common Pitfalls:

Mixing up Vm (peak) with V_rms; forgetting continuous conduction assumption; ignoring the back-emf term.


Final Answer:

cos α = (π/(2Vm)) * (R I0 + E)

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