L2324BinaryPhDi145s10

L2324BinaryPhDi145s10 - Lectures 23 & 24,...

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Unformatted text preview: Lectures 23 & 24, spring 2010 ENGR 145, Chemistry of Materials Case Western Reserve University Reading assignment : C&R 10.7-9, 10.11, 10.12 Learning objectives: Know and use new concepts for binary phase diagrams Liquidus curve Solidus curve Lever rule Compositions of phases Fractions of each phase Understand the changes that occur during solidification Apply these concepts for a continuous solid solution Understand binary eutectic phase diagrams New feature: solvus curve What happens at the eutectic temperature and composition Difference between primary solid and eutectic solid Use the lever rule to compute fractions of primary, eutectic, or total fractions of two different solid phases Lectures 23 & 24: Two-Component Phase Diagrams 1 Lectures 23 & 24, spring 2010 ENGR 145, Chemistry of Materials Case Western Reserve University Phases & Components Whats the Difference? Phase: a chemically and structurally homogeneous portion of a system Diamond and graphite: distinct solid phases of carbon Silica glass, quartz, and cristobalite: distinct phases of SiO 2 Number of components: the minimum number of chemical species needed to describe the composition of every phase Examples: Pure ice in pure water: two phases, one component In a one-component system, all phases have the same composition Ethanol in water: one phase, two components Dry air: one phase, many components 2 Lectures 23 & 24, spring 2010 ENGR 145, Chemistry of Materials Case Western Reserve University A map Areas: ranges of T and P for which a single phase is the equilibrium assemblage for the system Curves: combinations of T and P for which two phases coexist at equilibrium Triple point: unique values of T and P for which three phases coexist OGC Fig. 10.21 Review: One-Component Phase Diagrams [OGC 10.6] 3 4 Lectures 23 & 24, spring 2010 ENGR 145, Chemistry of Materials Case Western Reserve University Coexistence of phases phases have equal Gibbs free energy ( G transformation = 0) determines the location of the curves and triple point(s) on one-component phase diagrams OGN Fig. 13.10 ( ) ( ) 2 2 H O H O s ( ) ( ) 2 2 H O H O s Review: Gibbs Free Energy in One-Component Systems [OGN 13.7] G freezing >0 G freezing <0 = freezing freezing freezing G H T S G freezing = 0 Lectures 23 & 24, spring 2010 ENGR 145, Chemistry of Materials Case Western Reserve University Two-component (a.k.a....
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This note was uploaded on 01/30/2011 for the course EMSE 103 taught by Professor Ggh during the Spring '10 term at Case Western.

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L2324BinaryPhDi145s10 - Lectures 23 & 24,...

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