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Design Example: Underdamped Parallel RLC Circuit01:17

Design Example: Underdamped Parallel RLC Circuit

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Consider designing an oscillator circuit, a crucial component in various electronic devices and systems. The objective is to create an oscillator circuit with specific characteristics: a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. To accomplish this, a parallel RLC circuit is employed, known for its ability to sustain oscillations at a resonant frequency. In this case, the damping factor is pivotal in achieving the desired performance.
Starting with a fixed...
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LC Circuits01:21

LC Circuits

3.2K
An LC circuit consists of an inductor and a capacitor, either in series or parallel. Consider a charged capacitor connected with an inductor in series. Before the switch is closed, all the energy of the circuit is stored in the electric field of the capacitor. When the switch is closed, the capacitor begins to discharge, producing a current in the circuit. The current, in turn, creates a magnetic field in the inductor. Because of the induced emf in the inductor, the current cannot change...
3.2K
Oscillations In An LC Circuit01:30

Oscillations In An LC Circuit

3.0K
An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
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RLC Circuit as a Damped Oscillator01:30

RLC Circuit as a Damped Oscillator

2.1K
An RLC circuit combines a resistor, inductor, and capacitor, connected in a series or parallel combination.
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
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RLC Series Circuits01:30

RLC Series Circuits

3.7K
An RLC series circuit comprises an inductor, a resistor, and a charged capacitor connected in series. When the circuit is closed, the capacitor begins to discharge through the resistor and inductor by transferring energy from the electric field to the magnetic field. Here, the resistor connected to the circuit causes energy losses; therefore, on the complete discharge of the capacitor, the magnetic field energy acquired by the inductor is less than the original electric field energy of the...
3.7K
Parallel RLC Circuits01:14

Parallel RLC Circuits

1.6K
Street lamps equipped with RLC surge protectors are an excellent example of applying circuit analysis in practical scenarios. These surge protectors safeguard the lamp's components against sudden voltage spikes.
A simplified parallel RLC circuit model with a DC input source generating a step response is employed in this context. When the switch is turned on, Kirchhoff's current law is applied, leading to a second-order differential equation.
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Related Experiment Video

Updated: Jan 15, 2026

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators
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Inductive Displacement Sensor Operating in an LC Oscillator System Under High Pressure Conditions-Basic Design

Janusz Nurkowski1, Andrzej Nowakowski1

  • 1Strata Mechanics Research Institute of the Polish Academy of Sciences, Reymonta 27, PL-30-059 Kraków, Poland.

Sensors (Basel, Switzerland)
|October 16, 2025
PubMed
Summary
This summary is machine-generated.

This study details an inductive displacement transducer for measuring rock deformation under high pressure. The sensor uses a solenoid and LC oscillator to achieve ~100 nm strain resolution at pressures over 400 MPa.

Keywords:
LC oscillatorinductive displacement sensoroptimizationquality factor (Q-factor)resonant systemsensor geometry

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Area of Science:

  • Geotechnical Engineering
  • Materials Science
  • Sensor Technology

Background:

  • Measuring rock specimen displacement under high hydrostatic pressure is crucial for understanding geological processes.
  • Existing methods may lack the required precision or robustness for extreme pressure environments.

Purpose of the Study:

  • To present design principles for a novel inductive displacement transducer capable of high-precision rock deformation measurement.
  • To analyze the interplay between electrical and mechanical parameters for optimizing sensor performance.

Main Methods:

  • Development of a coreless solenoid-based inductive sensor integrated with an LC oscillator.
  • Utilizing a reference coil to enable differential measurement and enhance accuracy.
  • Mathematical modeling of sensor parameters to understand interdependencies.

Main Results:

  • Achieved a strain resolution of approximately 100 nm at pressures exceeding 400 MPa.
  • Identified key design challenges including electrical (Q-factor, sensitivity) and mechanical (stability, size) factors.
  • Demonstrated the necessity of balancing competing sensor parameters for specific applications.

Conclusions:

  • The developed inductive transducer offers a viable solution for precise rock displacement measurement under extreme hydrostatic pressures.
  • Optimized sensor design requires careful consideration of trade-offs between sensitivity, stability, and miniaturization.
  • The presented mathematical framework aids in tailoring the sensor design to specific experimental conditions.