@@ -1607,9 +1607,9 @@ z
, respectively.
-Molar masses and thermal conductivity of the pure substances are listed in table 1.
+Molar masses and thermal conductivity of the pure substances are listed in table
1 .
The structure of this expression illustrates the nonlinear dependence of the interaction term on
-both the molar mass ratio and the square root of the conductivity ratio of the involved species.
+both the molar mass ratio and the square root of the conductivity ratio of the involved species.
Table 1: Properties of some gases
@@ -1657,7 +1657,7 @@ both the molar mass ratio and the square root of the conductivity ratio of the i
-
This formulation acknowledges that the transport properties of a gas mixture are not a simple
+
This formulation acknowledges that the transport properties of a gas mixture are not a simple
linear combination of the individual conductivities. Rather, they are governed by intermolecular
interactions, which affect the energy exchange and diffusion behavior of each component. These
interactions are particularly significant at elevated pressures or in cases where the gas components
@@ -1666,7 +1666,7 @@ exhibit widely differing molecular masses or transport properties.
dominate the behavior of the mixture, while higher-order (three-body or more) interactions are
neglected. It also presumes that the gases approximate ideal behavior, although in practical
applications, moderate deviations from ideality are tolerated without significant loss of accuracy.
-In figure 1 the resulting thermal conductivity of an H2/CO2-mixture is shown.