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@@ -15,8 +15,8 @@ Such functions are either energies (hence *potential*) or entropies.
Which potential (of many) decides the equilibrium states for a given system?
That depends which variables are assumed to already be in automatic equilibrium.
Such variables are known as the **natural variables** of that potential.
-For example, if a system can freely exchange heat with its surroundings,
-and is consequently assumed to be at the same temperature $$T = T_{\mathrm{sur}}$$,
+For example, if a system can freely exchange heat with its environment,
+and is consequently assumed to be at the same temperature $$T = T_{\mathrm{env}}$$,
then $$T$$ must be a natural variable.
The link from natural variables to potentials
@@ -32,6 +32,7 @@ Mathematically, the potentials are related to each other
by [Legendre transformation](/know/concept/legendre-transform/).
+
## Internal energy
The **internal energy** $$U$$ represents
@@ -76,6 +77,7 @@ to help keep track of which function depends on which variables.
They are meaningless; these are normal partial derivatives.
+
## Enthalpy
The **enthalpy** $$H$$ of a system, in units of energy,
@@ -115,6 +117,7 @@ $$\begin{aligned}
\end{aligned}$$
+
## Helmholtz free energy
The **Helmholtz free energy** $$F$$ represents
@@ -154,6 +157,7 @@ $$\begin{aligned}
\end{aligned}$$
+
## Gibbs free energy
The **Gibbs free energy** $$G$$ represents
@@ -192,6 +196,7 @@ $$\begin{aligned}
\end{aligned}$$
+
## Landau potential
The **Landau potential** or **grand potential** $$\Omega$$, in units of energy,
@@ -230,6 +235,7 @@ $$\begin{aligned}
\end{aligned}$$
+
## Entropy
The **entropy** $$S$$, in units of energy over temperature,