Doxygen update

-> fixing documentation for functions.

Cantera/src/thermo/HMWSoln.cpp

@@ -895,17 +895,24 @@ namespace Cantera {
   }
 
 
-  /**
+  /*
    * Returns an array of partial molar enthalpies for the species
    * in the mixture.
    * Units (J/kmol)
    *
-   * We calculate this quantity partially from the relation and
-   * partially by calling the standard state enthalpy function.
+   * For this phase, the partial molar enthalpies are equal to the
+   * standard state enthalpies modified by the derivative of the
+   * molality-based activity coefficent wrt temperature
+   *
+   *  \f[
+   * \bar h_k(T,P) = h^{\triangle}_k(T,P) - R T^2 \frac{d \ln(\gamma_k^\triangle)}{dT}
+   * \f]
+   * The solvent partial molar enthalpy is equal to 
+   *  \f[
+   * \bar h_o(T,P) = h^{o}_o(T,P) - R T^2 \frac{d \ln(a_o)}{dT}
+   * \f]
    *
-   *     hbar_i = - T**2 * d(chemPot_i/T)/dT 
    *
-   * We calculate 
    */
   void HMWSoln::getPartialMolarEnthalpies(doublereal* hbar) const {
     /*
@@ -932,7 +939,7 @@ namespace Cantera {
     }
   }
 
-  /**
+  /*
    *
    * getPartialMolarEntropies()        (virtual, const)
    *

Cantera/src/thermo/HMWSoln.h

@@ -1595,7 +1595,8 @@ namespace Cantera {
      * \f]
      * The solvent partial molar enthalpy is equal to 
      *  \f[
-     * \bar h_o(T,P) = h^{o}_o(T,P) - R T^2 \frac{d \ln(a_o}{dT}
+     * \bar h_o(T,P) = h^{o}_o(T,P) - R T^2 \frac{d \ln(a_o)}{dT}
+     *       = h^{o}_o(T,P) + R T^2  (\sum_{k \neq o} m_k)  \tilde{M_o} (\frac{d \phi}{dT})
      * \f]
      *
      *
@@ -1607,7 +1608,7 @@ namespace Cantera {
   
     //! Returns an array of partial molar entropies of the species in the
     //! solution. Units: J/kmol/K.
-    /**
+    /*!
      * Maxwell's equations provide an insight in how to calculate this
      *   (p.215 Smith and Van Ness)
      *