ギブス自由エネルギーの記事 | jwiki.wiki

The thermodynamicists of the original eight founding schools of thermodynamics. The schools with the most-lasting influence on the modern versions of thermodynamics are the Berlin school, particularly Rudolf Clausius's 1865 textbook The Mechanical Theory of Heat, the Vienna school, with the statistical mechanics of Ludwig Boltzmann, and the Gibbsian school at Yale University of Willard Gibbs' 1876 and his book On the Equilibrium of Heterogeneous Substances which launched chemical thermodynamics.[8]

熱力学の基礎から応用までエネルギーとエントロピーの科学

熱力学エントロピー熱力学第一法則熱力学第二法則

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ภาพประกอบบทความ

化学平衡の原理と応用熱力学から実用的な分析手法まで

化学平衡平衡定数ギブス自由エネルギー酸塩基平衡

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Solid phase transitions which transform reversibly without passing through the liquid or gaseous phases are called enantiotropic. In contrast, if the modifications are not convertible under these conditions, the system is monotropic. Experimental data are used to differentiate between enantiotropic and monotropic transitions and energy/temperature semi-quantitative diagrams can be drawn by applying several rules, principally the heat-of-transition rule, the heat-of-fusion rule and the density rule. These rules enable the deduction of the relative positions of the H and G isobars in the E/T diagram. [1]

多形現象（ポリモーフィズム）の科学結晶構造の多様性と物性への影響

多形現象ポリモーフィズム結晶構造相転移

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Geoffroy's Affinity Table (1718): At the head of the column is a substance with which all the substances below can combine, where each column below the header is ranked by degrees of "affinity"

化学親和性の本質歴史的変遷から現代の熱力学まで

化学親和性ギブス自由エネルギー化学反応熱力学

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熱力学的平衡の原理と状態の定義

熱力学的平衡エントロピーギブス自由エネルギー熱平衡

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