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相关概念视频

Characteristics of Series Resonant Circuit01:24

Characteristics of Series Resonant Circuit

250
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:
250
Parallel Resonance01:23

Parallel Resonance

205
The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
205
Series Resonance01:17

Series Resonance

174
The RLC circuit impedance is defined as the ratio of the supply voltage to the circuit current. Resonance in such a circuit occurs when the imaginary part of this impedance equals zero. This specific condition means that the inductive reactance is exactly equal to the capacitive reactance. The frequency at which this happens is known as the resonant frequency. Mathematically, the resonant frequency is inversely proportional to the square root of the product of the inductance (L) and capacitance...
174
Design Example: Underdamped Parallel RLC Circuit01:17

Design Example: Underdamped Parallel RLC Circuit

286
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...
286
Frequency Response of a Circuit01:20

Frequency Response of a Circuit

259
Inductive circuits present intriguing challenges in electrical engineering, particularly during the transition from the time domain to the frequency domain. This transformation involves converting inductors into impedances and utilizing phasor representation.
The transfer function is pivotal in characterizing how these circuits react to various frequencies, facilitating a profound understanding of their behavior. An essential parameter is the time constant, signifying the...
259
Resonance in an AC Circuit01:26

Resonance in an AC Circuit

2.0K
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...
2.0K

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Fabrication and Characterization of Superconducting Resonators
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具有频率转换的中红外微环共振器具有特点.

Li Chen, Dong Zhao, Kun Huang

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    此摘要是机器生成的。

    本研究引入了一种新的频率转换技术,以有效地表征中红外 (MIR) 集成设备. 这种方法克服了MIR激光器和探测器的局限性,为先进的MIR光学铺平了道路.

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    科学领域:

    • 光子学和光学工程 光子学和光学工程
    • 材料科学 材料科学 材料科学
    • 集成光学 集成光学 集成光学

    背景情况:

    • 中红外 (MIR) 集成设备的开发受到高成本和现有激光和探测器性能差的阻碍.
    • 描述MIR设备对于推进MIR集成光学至关重要.
    • 现有的表征方法在MIR频谱中面临局限性.

    研究的目的:

    • 展示一种有效的方法来表征中红外线 (MIR) 集成设备.
    • 为了利用频率转换技术进行增强的MIR设备参数提取.
    • 为了克服昂贵和低性能MIR激光器和探测器所带来的局限性.

    主要方法:

    • 设计和制造的上蓝宝石 (SOS) 肋骨波导和微环共振器 (MRR).
    • 通过使用差异频率生成 (DFG) 来生成一个MIR激光来进行测试.
    • 通过总频率生成 (SFG) 检测到MIR-MRR的传输频谱.

    主要成果:

    • 实现了4.5dB/cm的波导传输损失.
    • 测量了微环共振器的质量因子 (Q-因子),达到38,000个.
    • 实验结果与数值模拟有很好的一致性.

    结论:

    • 开发的频率转换技术为特征MIR集成设备提供了一种可行的方法.
    • 这种方法可以显著加快MIR集成光学的进展.
    • 展示的技术为克服MIR频段当前的技术障碍提供了一条途径.