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?
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Acos α = (π/(2Vm)) * (R I0 + E)
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Bcos α = (2Vm/π) * (R I0 + E)
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Ccos α = (π/(2Vm)) * (E − R I0)
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Dcos α = (π/Vm) * (R I0 + E)
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E—
Answer
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)