Explanation The current at the time of discharging is given by, I i = E R ( e − ( R L t ) ) Here, the resistance is R , inductance is L , time is t and electric voltage is E . The current at the time of charging is given by, I i = E R ( 1 − e − ( R L t ) ) Apply t → 0 for the above equation.

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Author: ANNIN

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Chapter 1.7, Problem 7TFR

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Whether the statement “Given an alternating current in an RL circuit, the transient part of the current decays to zero with time, while the steady-state part of the current oscillates with the same frequency as the applied EMF” is true or false.

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Chapter 1.7, Problem 6TFR

Chapter 1.7, Problem 8TFR

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Whether the statement “Given an alternating current in an RL circuit, the transient part of the current decays to zero with time, while the steady-state part of the current oscillates with the same frequency as the applied EMF” is true or false.

Solution Summary: The author analyzes whether the statement is true or false. The transient part of the current decays to zero with time, while the steady-state part oscillates with the same frequency as the applied EMF.

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To find: Whether the statement “Given an alternating current in an RL circuit, the transient part of the current decays to zero with time, while the steady-state part of the current oscillates with the same frequency as the applied EMF” is true or false.

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Chapter 1 Solutions

To find:

Whether the statement “Given an alternating current in an RL circuit, the transient part of the current decays to zero with time, while the steady-state part of the current oscillates with the same frequency as the applied EMF” is true or false.