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The thermodynamic properties of materials are intensive thermodynamic parameters which are specific to a given material. Each is directly related to a second order differential of a thermodynamic potential. Examples for a simple 1-component system are: * Compressibility (or its inverse, the bulk modulus) : * Isothermal compressibility :: : * Adiabatic compressibility :: * Specific heat (Note - the extensive analog is the heat capacity) : * Specific heat at constant pressure :: : * Specific heat at constant volume :: * Coefficient of thermal expansion :: where ''P'' is pressure, ''V'' is volume, ''T'' is temperature, ''S'' is entropy, and ''N'' is the number of particles. For a single component system, only three second derivatives are needed in order to derive all others, and so only three material properties are needed to derive all others. For a single component system, the "standard" three parameters are the isothermal compressibility , the specific heat at constant pressure , and the coefficient of thermal expansion . For example, the following equations are true: : : The three "standard" properties are in fact the three possible second derivatives of the Gibbs free energy with respect to temperature and pressure. ==Sources== The Dortmund Data Bank is a factual data bank for thermodynamic and thermophysical data. See thermodynamic databases for pure substances. 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「Material properties (thermodynamics)」の詳細全文を読む スポンサード リンク
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