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翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク Stub (electronics) ： ウィキペディア英語版 Stub (electronics) In microwave and radio-frequency engineering, a stub or resonant stub is a length of transmission line or waveguide that is connected at one end only. The free end of the stub is either left open-circuit or (always in the case of waveguides) short-circuited. Neglecting transmission line losses, the input impedance of the stub is purely reactive; either capacitive or inductive, depending on the electrical length of the stub, and on whether it is open or short circuit. Stubs may thus function as capacitors, inductors and resonant circuits at radio frequencies. Stubs work by means of standing waves of radio waves along their length. Their reactive properties are determined by their physical length in relation to the wavelength of the radio waves. Therefore stubs are most commonly used in UHF or microwave circuits in which the wavelengths are short enough that the stub is conveniently small. They are often used to replace discrete capacitors and inductors, because at UHF and microwave frequencies lumped components perform poorly due to parasitic reactance.〔 Stubs are commonly used in antenna impedance matching circuits, frequency selective filters, and resonant circuits for UHF electronic oscillators and RF amplifiers. Stubs can be constructed with any type of transmission line: parallel conductor line (where they are called Lecher lines), coaxial cable, stripline, waveguide, and dielectric waveguide. Stub circuits can be designed using a Smith chart, a graphical tool which can determine what length line to use to obtain a desired reactance. ==Short circuited stub== The input impedance of a lossless short circuited line is, ::$$ Z_\mathrm = j Z_0 \tan(\beta l)\,\! where j is the imaginary unit, $Z\_0$ is the characteristic impedance of the line, $\backslash beta\; =\; 2\backslash pi/\backslash lambda\backslash ,$ is the phase constant of the line, and $l$ is the physical length of the line. Thus, depending on whether $\backslash tan(\backslash beta\; l)$ is positive or negative, the stub will be inductive or capacitive, respectively. The length of a stub to act as a capacitor ''C'' at an angular frequency of $\backslash omega$ is then given by: ::$$ l = \frac \left(- \arctan \left(\frac\right) \right ) The length of a stub to act as an inductor ''L'' at the same frequency is given by: ::$$ l = \frac \left(n \pi + \arctan\left(\frac\right) \right ) 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Stub (electronics)」の詳細全文を読む スポンサード リンク 翻訳と辞書 : 翻訳のためのインターネットリソース Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.