Mechanically Oscillating Capacitor in LC circuit

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SUMMARY

The discussion centers on modeling a mechanically oscillating capacitor within a series LC circuit, where one plate of the capacitor is attached to a spring. Two primary methods for determining the resonant frequency were proposed: equating a homogeneous second-order differential equation for the spring to the driving force from charged plates, and applying a similar approach to the LC circuit. The complexity arises from the relationship between plate distance and spring motion, complicating the calculation of resonant frequencies. Insights suggest that total system resonance occurs when the circuit and spring frequencies align, though this may oversimplify the underlying differential equations.

PREREQUISITES
  • Understanding of LC circuit theory and resonant frequency
  • Familiarity with differential equations, particularly second-order equations
  • Knowledge of electrostatics, specifically the relationship between charge density and force
  • Basic principles of mechanical oscillation and spring dynamics
NEXT STEPS
  • Research the derivation of resonant frequency in LC circuits with mechanical components
  • Study the application of second-order differential equations in mechanical systems
  • Explore the relationship between charge density and force in electrostatic systems
  • Investigate the effects of varying plate separation on the behavior of parallel-plate capacitors
USEFUL FOR

Physicists, electrical engineers, and students studying circuit dynamics and mechanical oscillations will benefit from this discussion, particularly those interested in the integration of mechanical systems with electrical circuits.

thebaron
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I have been thinking about a scenario in which I might have a series LC circuit, but where one plate on the parallel-plate capacitor is attached to a spring. How would I model such a scenario, and how would I determine the ideal resonant frequency of the entire system?

I have attempted two methods:

1) Basically take a homogeneous second-order differential for any spring, and equate it to a "driving" force equal to the force between two charged plates as a function of the distance between them;

2) And to take the homogeneous second order differential for any LC circuit, and equate it to the charge on any capacitor as a function of the distance between the plates.

My problem in case one is that the distance between plates is in fact equal to the amplitude of the spring's motion minus its actual position, quantity squared; and I simply have no idea where to begin solving that. The second attempt certainly looks less complex, but the distance between plates in that case is in fact equal to the entire solution to a homogeneous spring equation, which just makes it as complex as case one.

As for the resonant frequencies, my intuition wants to say that if the circuit and spring w's are equal that should represent total system resonance; but then, that seems too simple considering the differential models I just delineated. Any insights?
 
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Where the plate separation is sufficiently small compared to the length of the sides, the force will not depend upon the distance between the plates. The force will be directly proportional to the charge density on a plate, or equivalently, the total charge.

If you want the force to depend upon displacement, that's OK too, and has a physical analogy such as the force between two conductive spheres.
 

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