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関連する概念動画

Oscillations In An LC Circuit01:30

Oscillations In An LC Circuit

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
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
RLC Circuit as a Damped Oscillator01:30

RLC Circuit as a Damped Oscillator

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...
Design Example: Underdamped Parallel RLC Circuit01:17

Design Example: Underdamped Parallel RLC Circuit

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...
Characteristics of Series Resonant Circuit01:24

Characteristics of Series Resonant Circuit

Series resonance occurs in a circuit containing inductive (L), capacitive (C), and resistive (R) elements connected sequentially. At the resonance frequency, the inductive and capacitive reactances are equal in magnitude but opposite in sign, effectively canceling each other. This causes the circuit's impedance is minimal, primarily determined by the resistance R. The resonant frequency of an RLC circuit is defined as:
Resonance in an AC Circuit01:26

Resonance in an AC Circuit

The property of an inductor makes it resist any change in the current passing through it, while the property of a capacitor is to build up the charge across its terminals. Hence, if an inductor and capacitor are connected in series, they have opposite effects on the relative phase between current and voltage. The current through the circuit undergoes forced oscillation at the frequency of the source. The resistance term in an R-L-C circuit acts as a damping term because power is dissipated...

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関連する実験動画

Updated: Jun 14, 2026

Fabrication and Testing of Microfluidic Optomechanical Oscillators
09:10

Fabrication and Testing of Microfluidic Optomechanical Oscillators

Published on: May 29, 2014

電子回路ベースの共振器で振動するマイクロキャビティレーザー.

Christoph Walther1, Giacomo Scalari, Maria Ines Amanti

  • 1Institute for Quantum Electronics, ETH Zurich, Wolfgang-Pauli-Strasse 16, 8093 Zurich, Switzerland. walther@phys.ethz.ch

Science (New York, N.Y.)
|March 20, 2010
PubMed
まとめ

研究者らは,サブ波長電子誘導電容器 (LC) 共振回路を用いた超小型テラヘルツレーザーを開発した. このコンパクトで低消費電力の装置は,電場を制限し,超高速の変調速度を実現する可能性を秘めています.

科学分野:

  • フォトニクス フォトニクスとは
  • 電気工学 電気工学とは
  • 応用物理学 応用物理学

背景:

  • マイクロキャビティレーザーは,コンパクト性と低電力消費などの利点を提供しています.
  • 超高速変調速度は,高度な通信システムにとって極めて重要です.
  • テラヘルツ (THz) 周波数は,スペクトロスコピーと画像処理のためのユニークな機会を提供します.

研究 の 目的:

  • テラヘルツ範囲で動作する超小型,電気的に注入されたレーザーを実証するために.
  • 極端な電場収束のために,電子誘導電容器 (LC) 共振回路のサブ波長の電子誘導電容器を使用します.
  • より高い周波数およびその他の光電子機器のためのこの設計の可能性を調査する.

主な方法:

  • 亜波長電子LC共鳴回路を組み込んだ超小型レーザー装置の製造.
  • レーザー操作のための電気注入.
  • レーザーの動作周波数とモードボリュームの特徴.

主要な成果:

  • 1.5テラヘルツで動作する電気注入レーザーの実証が成功しました.
  • 亜波長LC共振器により,電場の極端な閉じ込めが達成されました.

さらに関連する動画

Microwave Photonics Systems Based on Whispering-gallery-mode Resonators
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Microwave Photonics Systems Based on Whispering-gallery-mode Resonators

Published on: August 5, 2013

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators
09:46

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators

Published on: August 8, 2025

関連する実験動画

Last Updated: Jun 14, 2026

Fabrication and Testing of Microfluidic Optomechanical Oscillators
09:10

Fabrication and Testing of Microfluidic Optomechanical Oscillators

Published on: May 29, 2014

Microwave Photonics Systems Based on Whispering-gallery-mode Resonators
12:18

Microwave Photonics Systems Based on Whispering-gallery-mode Resonators

Published on: August 5, 2013

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators
09:46

Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators

Published on: August 8, 2025

  • レーザーのモードボリュームは,強烈にサブ波長であり,小型化を可能にしました.
  • 結論:

    • 開発された超小型LC共振器レーザーは,テラヘルツ光電子学の重要な進歩です.
    • 設計原理は,より高い周波数にスケーラブルであり,検出器やモデュレータに適応できます.
    • この技術は,コンパクトで高速なTHzアプリケーションに期待されます.