The - phase diagram of a pure substance Q is specified by the following readings

PHYSICS · Multi-part · Fermi University Physics · Thermal, Statistical & Complex Systems · Interacting systems, real gases and phase equilibria · Interacting systems, real gases and phase equilibria

Thermal Physics, Ch Phase coexistence and the Clausius-Clapeyron relation

Problem

The pp-TT phase diagram of a pure substance Q is specified by the following readings. Triple point: 210.0 K210.0\,\mathrm{K} at 8.00 kPa8.00\,\mathrm{kPa}. Critical point: 560 K560\,\mathrm{K} at 5.00 MPa5.00\,\mathrm{MPa}. Solid-liquid line: a straight line of slope dp/dT=+2.00 MPa K−1\mathrm{d}p/\mathrm{d}T = +2.00\,\mathrm{MPa\,K^{-1}} through the triple point. Liquid-vapour line: passes through 101.3 kPa101.3\,\mathrm{kPa} at 320.0 K320.0\,\mathrm{K}. Latent heat of vaporisation at 320.0 K320.0\,\mathrm{K}: L=27.0 kJ mol−1L = 27.0\,\mathrm{kJ\,mol^{-1}}. A separate temperature-composition diagram, at fixed pressure, is given for solid-liquid coexistence of Q with a second substance R, whose mole fraction is xx. At one temperature the tie line runs from xL=0.25x_L = 0.25 in the liquid to xS=0.62x_S = 0.62 in the solid. ((a)) A sealed sample of pure Q is warmed slowly at a constant pressure of 101.3 kPa101.3\,\mathrm{kPa} from 150 K150\,\mathrm{K} to 500 K500\,\mathrm{K}. Give, to the nearest 0.1 K0.1\,\mathrm{K}, the two temperatures at which it changes phase (melting first, then boiling). ((b)) On this isobar the molar Gibbs functions gliq(T)g_{\rm liq}(T) and gvap(T)g_{\rm vap}(T) cross at the boiling point. Using (∂g/∂T)p=−s(\partial g/\partial T)_p = -s, find the magnitude of the difference between the slopes of the two curves at the crossing. ((c)) A mixture of Q and R of overall composition x0=0.40x_0 = 0.40 sits on the given tie line. Find the fraction of the material that is solid.

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