翻訳と辞書 Words near each other ・ Internal Medicine (Springer journal) ・ Internal migration ・ Internal Military Service ・ Internal model ・ Internal model (motor control) ・ Internal monologue ・ Internal nasal branches of infraorbital nerve ・ Internal obturator muscle ・ Internal occipital crest ・ Internal occipital protuberance ・ Internal organization of the Central Commission for Discipline Inspection ・ Internal orifice of the uterus ・ Internal oxidation ・ Internal passport ・ Internal passport of Russia ・ Internal pressure ・ Internal pterygoid ・ Internal pudendal ・ Internal pudendal artery ・ Internal pudendal veins ・ Internal Punishment Programs ・ Internal quest ・ Internal RAM ・ Internal rate of return ・ Internal ratings-based approach (credit risk) ・ Internal reconstruction ・ Internal rent ・ Internal resistance ・ Internal resistance to apartheid ・ Internal Revenue Allotment Dictionary Lists mini英和辞書 mini和英辞書 Webster 1913 Latin-English FOLDOC Wikipedia English ウィキペディア

翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク Internal pressure ： ウィキペディア英語版 Internal pressure Internal pressure is a measure of how the internal energy of a system changes when it expands or contracts at constant temperature. It has the same dimensions as pressure, the SI unit of which is the pascal. Internal pressure is usually given the symbol $\backslash pi\_T$. It is defined as a partial derivative of internal energy with respect to volume at constant temperature: $\backslash pi\; \_T\; =\; \backslash left\; (\; \backslash frac\; \backslash right\; )\_T$ ==Thermodynamic equation of state== Internal pressure can be expressed in terms of temperature, pressure and their mutual dependence: $\backslash pi\_T\; =\; T\; \backslash left\; (\; \backslash frac\; \backslash right\; )\_V\; -\; p$ This equation is known as the thermodynamic equation of state for it expresses pressure in terms of thermodynamic properties of the system. : \right )_V \operatornameS + \left ( \frac \right )_S \operatornameV. Dividing this equation by $\backslash operatorname\; V$ at constant temperature gives: $\backslash left\; (\; \backslash frac\; \backslash right\; )\_T\; =\; \backslash left\; (\; \backslash frac\; \backslash right\; )\_V\; \backslash left\; (\; \backslash frac\; \backslash right\; )\_T\; +\; \backslash left\; (\; \backslash frac\; \backslash right\; )\_S$ Comparing the above differential with the fundamental thermodynamic equation $\backslash operatornameU\; =\; T\; \backslash operatorname\; S\; -\; p\; \backslash operatorname\; V$ gives $\backslash left\; (\; \backslash frac\; \backslash right\; )\_V\; =\; T$ and $\backslash left\; (\; \backslash frac\; \backslash right\; )\_S\; =\; -p$. This, and the definition of internal pressure, leads to $\backslash pi\_T\; =\; T\; \backslash left\; (\; \backslash frac\; \backslash right\; )\_T\; -\; p$ One of the Maxwell relations states that $\backslash left\; (\; \backslash frac\; \backslash right\; )\_T\; =\; \backslash left\; (\; \backslash frac\; \backslash right\; )\_V$ Inserting this into the above relation completes the proof. |} 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「Internal pressure」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.