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→Introduction 引言
X = m_1 \frac{\partial X}{\partial
X = m_1 \frac{\partial X}{\partial
m_1} + m_2 \frac{\partial X}{\partial m_2} + \cdots , </math>
m_1} + m_2 \frac{\partial X}{\partial m_2} + \cdots , </math>
{{NumBlk|:|<math>X = m_1 \frac{\partial X}{\partial
任何广度函数<math>X(T, p, m_1, m_2, \ldots)\ ,</math>（如体积<math>V\ ,</math>或者吉布斯自由能<math>E+pV-TS\ ,</math>）在等温等压状态下，对<math>m_i</math>都是一次齐次的，因此{{NumBlk|:|<math>X = m_1 \frac{\partial X}{\partial
m_1} + m_2 \frac{\partial X}{\partial m_2} + \cdots ,</math>|{{EquationRef|6}}}}
m_1} + m_2 \frac{\partial X}{\partial m_2} + \cdots ,</math>|{{EquationRef|6}}}}
an
an
important class of relations.
important class of relations.
是重要的一类关系。
== Scaling laws ==
== Scaling laws ==