thermodynamics and the phase rule

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1 Thermodynamics and the Phase Rule GLY 4200 Fall, 2012

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Thermodynamics and the Phase Rule. GLY 4200 Fall, 2012. Thermodynamic Background. System : The portion of the universe that is being studied Surroundings : The part of the universe not included in the system. Free Energy. Any change in the system involves a transfer of energy - PowerPoint PPT Presentation

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Page 1: Thermodynamics and the Phase Rule

1

Thermodynamics and the Phase Rule

GLY 4200

Fall, 2012

Page 2: Thermodynamics and the Phase Rule

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Thermodynamic Background

• System: The portion of the universe that is being studied

• Surroundings: The part of the universe not included in the system

Page 3: Thermodynamics and the Phase Rule

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Free Energy

• Any change in the system involves a transfer of energy

• All chemical systems tend naturally toward states of minimum Gibbs free energy

Page 4: Thermodynamics and the Phase Rule

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Gibbs Free Energy

• G = H - TS

• Where: G = Gibbs Free Energy H = Enthalpy (heat content) T = Temperature in Kelvin S = Entropy (a measure of randomness)

Page 5: Thermodynamics and the Phase Rule

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Alternative Equation

• For other temperatures and pressures we can use the equation: dG = VdP – SdT where V = volume and S = entropy (both molar)

• This equation can be used to calculate G for any phase at any T and P by integrating GT2P2

- GT1P1 = ∫P1

P2VdP - ∫T1T2SdT

Page 6: Thermodynamics and the Phase Rule

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Using Thermodynamics

• G is a measure of relative chemical stability for a phase We can determine G for any phase by measuring H and S

for the reaction creating the phase from the elements (SiO2 from silicon and oxygen, for example)

We can then determine G at any T and P mathematically• How do V and S vary with P and T?

dV/dP is the coefficient of isothermal compressibility dS/dT is the heat capacity at constant pressure (Cp)

Page 7: Thermodynamics and the Phase Rule

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Applying Thermodynamics

• If we know G for various phases, we can determine which is most stable

• With appropriate reactions comparing two or more phases, we can answer questions like: Why is melt more stable than solids at high T? Which polymorphic phase will be stable under

given conditions? What will be the effect of increased P on melting?

Page 8: Thermodynamics and the Phase Rule

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High Pressure

High pressure favors low volume, so which phase should be stable at high P?

• Hint: Does the liquid or solid have the larger volume?

Figure 5-2. Schematic P-T phase diagram of a melting reaction. Winter (2001) An Introduction to Igneous and Metamorphic Petrology. Prentice Hall.

Page 9: Thermodynamics and the Phase Rule

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High Temperature

• High temperature favors randomness, so which phase should be stable at higher T?

• Hint: Does liquid or solid have a higher entropy?

Figure 5-2. Schematic P-T phase diagram of a melting reaction. Winter (2001) An Introduction to Igneous and Metamorphic Petrology. Prentice Hall.

Page 10: Thermodynamics and the Phase Rule

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Stability

• Does the liquid or solid have the lowest G at point A? at point B?

Figure 5-2. Schematic P-T phase diagram of a melting reaction. Winter (2001) An Introduction to Igneous and Metamorphic Petrology. Prentice Hall.

Page 11: Thermodynamics and the Phase Rule

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Intensive Property

• An intensive property does not depend on the amount of material present Examples: Temperature, density, electric or

magnetic field strength

Page 12: Thermodynamics and the Phase Rule

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Phase

• Phase: Any homogeneous region, characterized by certain intensive properties, and separated from other phases by discontinuities in one or more of those intensive properties Solid, often a mineral Liquid Vapor

• Note: # of regions is not important, just the # of kinds of regions

Page 13: Thermodynamics and the Phase Rule

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Reaction

• Some change in the nature or types of phases in a system

Page 14: Thermodynamics and the Phase Rule

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Josiah Willard Gibbs

• Josiah Willard Gibbs (1839 - 1903) has been reckoned as one of the greatest American scientists of the 19th century

• He provided a sound thermodynamic foundation to much of Physical Chemistry

• Yale educated, he was awarded the first Doctor of Engineering in the U.S., and was appointed Professor of Mathematical Physics at Yale in 1871

Page 15: Thermodynamics and the Phase Rule

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Phase Rule

• The Phase Rule (J. Willard Gibbs) f = c - p System of c components and pphases has

variance “f”, the degrees of freedom f = # degrees of freedom = The number of

intensive parameters that must be specified in order to completely determine the system

Intensive variables are pressure, temperature, and composition, that can be changed independently without loss of a phase

Page 16: Thermodynamics and the Phase Rule

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Phase Rule 2

p =number of phasesp =number of phases• phases are mechanically separable constituentsphases are mechanically separable constituents

c = minimum number of c = minimum number of componentscomponents, which are , which are chemical constituents that must be specified in chemical constituents that must be specified in order to define all phasesorder to define all phases

Page 17: Thermodynamics and the Phase Rule

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3000K

• Two components are present - since the other can be made from whichever of the two have been chosen• Thus, a stoichiometric relationship between substances reduces the number of components necessary

H2O ↔ H2 + ½O2

Page 18: Thermodynamics and the Phase Rule

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Alternative Definition of Number of Components

• The minimum number of pure chemical substances that are required for arbitrary amounts of all phases of the system

Page 19: Thermodynamics and the Phase Rule

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Extended Phase Rule

f = c - px

• Where x is the number of intensive variables, pressure, temperature, composition, and possibly magnetic and electric fields, that can be changed independently without loss of a phase