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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 Anharmonicity ： ウィキペディア英語版 Anharmonicity In classical mechanics, anharmonicity is the deviation of a system from being a harmonic oscillator. An oscillator that is not oscillating in simple harmonic motion is known as an anharmonic oscillator where the system can be approximated to a harmonic oscillator and the anharmonicity can be calculated using perturbation theory. If the anharmonicity is large, then other numerical techniques have to be used. As a result, oscillations with frequencies $2\backslash omega$ and $3\backslash omega$ etc., where $\backslash omega$ is the fundamental frequency of the oscillator, appear. Furthermore, the frequency $\backslash omega$ deviates from the frequency $\backslash omega\_0$ of the harmonic oscillations. As a first approximation, the frequency shift $\backslash Delta\; \backslash omega=\backslash omega-\backslash omega\_0$ is proportional to the square of the oscillation amplitude $A$: :$\backslash Delta\; \backslash omega\backslash propto\; A^2$ In a system of oscillators with natural frequencies $\backslash omega\_\backslash alpha$, $\backslash omega\_\backslash beta$, ... anharmonicity results in additional oscillations with frequencies $\backslash omega\_\backslash alpha\backslash pm\; \backslash omega\_\backslash beta$. Anharmonicity also modifies the profile of the resonance curve, leading to interesting phenomena such as the foldover effect and superharmonic resonance. == General principle == A generalized version of harmonic oscillator in which the relationship between force and displacement is linear. The harmonic oscillator is a highly idealized system that oscillates with a single frequency, irrespective of the amount of pumping or energy injected into the system. Consequently, the harmonic oscillator's fundamental frequency of vibration is independent of the amplitude of the vibrations. Applications of the harmonic oscillator model abound in various fields, but perhaps the most commonly studied system is the Hooke's law mass-spring system. In the Hooke's law system the restoring force exerted on the mass is proportional to the displacement of the mass from its equilibrium position. This linear relationship between force and displacement mandates that the oscillation frequency of the mass will be independent of the amplitude of the displacement. In a mechanical anharmonic oscillator, the relationship between force and displacement is not linear but depends upon the amplitude of the displacement. The nonlinearity arises from the fact that the spring is not capable of exerting a restoring force that is proportional to its displacement because of, for example, stretching in the material comprising the spring. As a result of the nonlinearity, the vibration frequency can change, depending upon the system's displacement. These changes in the vibration frequency result in energy being coupled from the fundamental vibration frequency to other frequencies through a process known as parametric coupling. 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「Anharmonicity」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.