Boundary conditions for a purely inductive load in an AC circuit

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SUMMARY

The discussion centers on the boundary conditions for a purely inductive load in an AC circuit, specifically analyzing the constant term 'c' in the equation I(t) = -V0/(Lω) cos(ωt) + c. Participants agree that 'c' is determined by initial conditions, particularly the current at t=0, which can be influenced by the system's history. The conversation highlights the importance of understanding how the initial conditions affect the behavior of the circuit, especially when the emf is a periodic function. Ultimately, the consensus is that the value of 'c' is context-dependent and should not be arbitrarily dropped without justification.

PREREQUISITES
  • Understanding of Kirchhoff's laws in electrical circuits
  • Familiarity with AC circuit analysis and inductive loads
  • Knowledge of differential equations and their application in circuit theory
  • Concept of initial conditions in the context of oscillatory systems
NEXT STEPS
  • Study the role of initial conditions in AC circuit analysis
  • Learn about transient responses in RLC circuits
  • Explore the mathematical derivation of current in purely inductive circuits
  • Investigate the effects of resistance on the behavior of inductive loads in AC circuits
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Electrical engineers, physics students, and anyone involved in circuit design or analysis, particularly those focusing on AC circuits and inductive components.

  • #31
FranzDiCoccio said:
Uhm. Right, but the standard derivation of a purely inductive circuit never mentions any resistor, and
<br /> I(0) = \frac{V_0}{\omega L}<br />
It seems hard to make contact with your answer.
The resistor is there just to set up the initial condition. When you apply your voltage ##V_0 sin(\omega t) ## it no longer forms any part of the inductor current.

You have set up an initial current and have then applied your voltage directly across the inductor.
 

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