Recent experimental observations of the phase behavior of methane-n-paraffin hydrocarbon binary systems are used to make a phase rule analysis of such systems. The vapor-liquid equilibria of light hydrocarbon systems are complicated by liquid-liquid immiscibility and solids formation at low temperatures.The system studied here has limited liquid phase miscibility with a quadruple point involving o gas phase, two liquid phases, and a solid phase.Experimental techniques were developed to sample and analyze gas phases containing concentrations of n-heptane in the range of 0.00001 mole fraction with good precision. Binary K values for methane and n-heptane are reported at intervals of 20°F. from 0" to -100°F. for pressures up to the criticals for the mixtures. The results are reported numerically and illustrated graphically. Additional phase observations were made below the critical temperature of methane to confirm and extend the phase behavior of the methane-n-heptane system as reported by Kohn.Since the review of the vapor-liquid equilibria of light hydrocarbons at low temperatures by Price and Kobayashi ( 1 2 ) , studies on the phase behavior of the methane-nhexane ( 4 ) , methane-n-heptane ( 5 ) , and methane-noctane (6) systems by Kohn and co-workers have appeared. The methane-n-decane systems were reported by Stalkup et al. ( 1 7 ) and also studied by Koonce and Kobayashi ( 7 ) . Koonce et al. (8) reported vapor-liquid equilibria data on the ternary methane-propane-n-decane and the methanepropane-n-heptane systems in 1965.
GENERAL DISCUSSION OF PHASE BEHAVIOR IN METHANE-n-PARAFFIN HYDROCARBON BINARIESThe experimental results reported by Kohn (5, 6) and by Stalkup and Kobayashi ( I 7 ) and in this paper indicate that the binary pha* behavior of methane with other nparaffin hydrocarbons through n-decane offers at least three types of phase behavior:1. S stems in which the critical locus runs continuously higher boiling constituent with complete liquid phase miscibility.2. Systems in which the critical locus runs from the critical of the higher boiling constituent to a liquid-liquid from t E e critical of pure methane to the critical of the Lewis J. Hurt is at Rohm and Haas Company, Huntsville, Alabama.critical locus occurring at a temperature below the critical temperature of pure methane and at a pressure considerably in excess of the critical for pure methane; that is, when a liquid-liquid-solid-gas quadruple point occurs in the binary system.3. Systems in which the critical locus starting from the critical of the heavier component is severed by the intrusion of the solid-liquid-gas phase relationship upon the vapor-liquid equilibrium region, giving a second critical locus which extends from the critical point of pure methane to a gas-liquid critical point with solids present.These three types of systems are exemplified by the pressure-temperature projection of the methane-propane, methane-n-heptane, and methane-n-decane systems, respectively, as shown in Figures 1, 2, and 3.It has been verified experimental...