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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 susceptance ： ウィキペディア英語版 susceptance In electrical engineering, susceptance (''B'') is the imaginary part of admittance. The inverse of admittance is impedance, and the real part of admittance is conductance. In SI units, susceptance is measured in siemens. Oliver Heaviside first defined this property, which he called ''permittance'', in June 1887. ==Formula== The general equation defining admittance is given by :$Y\; =\; G\; +\; j\; B\; \backslash ,$ where :''Y'' is the admittance, measured in siemens. :''G'' is the conductance, measured in siemens. :''j'' is the imaginary unit, and :''B'' is the susceptance, measured in siemens. The admittance (''Y'') is the inverse of the impedance (''Z'') :$Y\; =\; \backslash frac\; =\; \backslash frac\; =\; \backslash left(\; \backslash frac\; \backslash right)\; +\; j\; \backslash left(\; \backslash frac\; \backslash right)\; \backslash ,$ or :$B\; =\; Im(Y)\; =\; \backslash left(\; \backslash frac\; \backslash right)\; =\; \backslash frac$ where :$Z\; =\; R\; +\; j\; X\; \backslash ,$ :''Z'' is the impedance, measured in ohms :''R'' is the resistance, measured in ohms :''X'' is the reactance, measured in ohms. Note: The susceptance is the imaginary part of the admittance. The magnitude of admittance is given by: :$\backslash left\; |\; Y\; \backslash right\; |\; =\; \backslash sqrt\; \backslash ,$ 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「susceptance」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.