Maximum Current in LC Circuit: Solving for the Peak Amplitude

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SUMMARY

The maximum current in an LC circuit can be calculated using the formula I_{max} = V_{max} \sqrt{C/L}. In this discussion, a capacitor of 18.0 μF charged to 22.5 V is connected to a 12.0 mH inductor, resulting in a peak current of 871 mA. The relationship between the energy stored in the capacitor and the inductor is crucial, as energy conservation principles dictate that the energy transitions between the capacitor and the inductor during oscillations.

PREREQUISITES
  • Understanding of LC circuits and their components
  • Familiarity with energy conservation in electrical systems
  • Knowledge of angular frequency and its role in oscillations
  • Proficiency in using formulas related to capacitors and inductors
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  • Study the derivation of the angular frequency in LC circuits
  • Explore energy transfer mechanisms in oscillating circuits
  • Learn about the effects of resistance in RLC circuits
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Students studying electrical engineering, physics enthusiasts, and professionals working with oscillating circuits will benefit from this discussion.

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[SOLVED] Finding current in LC circuit

Homework Statement


A [itex]18.0 \mu {\rm F}[/itex] capacitor is placed across a [itex]22.5 {\rm V}[/itex] battery for a few seconds and is then connected across a [itex]12.0 \rm mH[/itex] inductor that has no appreciable resistance.

After connecting the capacitor and inductor together, find the maximum current in the circuit.

Homework Equations



[tex]i=-\omega*Q*sin(\omega*t+\varphi)[/tex]

The Attempt at a Solution



This sounds like a pretty simple question and I think I'm complicating it too much. Does this have anything to do with finding the angular frequency. I know current is maximum when capacitor potential and induced emf is zero. But I don't know what the relationship using an equation. Do I have to derive one? I can't seem to find one.
 
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The trick here is to realize that during the oscillations that ensue when the charged capacitor is connected to the inductor, at certain instants of time the voltage on the capacitor will cross through zero volts. That leaves zero energy stored in the capacitor at those instants. So where did the energy go? It all ended up stored in the inductor's magnetic field thanks to the current flowing through it.

Equating the maximal stored energies:

##½~C V_{max}^2 = ½~L I_{max}^2##

##I_{max} = V_{max} \sqrt{C/L}##

##I_{max} = 871~mA##
 
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