Thermodynamics Of Materials Pdfkeyclever

'Thermodynamics of Materials' introduces the basic underlying principles of thermodynamics as well as their applicability to the behavior of all classes of materials, while providing an integrated approach from macro- (or classical) thermodynamics to meso- and nanothermodynamics, and microscopic (or statistical) thermodynamics. Treatment of the laws of thermodynamics and their applications to equilibrium and the properties of materials. Provides a foundation to treat general phenomena in materials science and engineering, including chemical reactions, magnetism, polarizability, and elasticity. Develops relations pertaining to multiphase equilibria as determined by a treatment of solution thermodynamics.

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34 Full PDFs related to this paper. Introduction to the Thermodynamics of Materials.
34 Full PDFs related to this paper. Introduction to the Thermodynamics of Materials.

Photo showing gas bubbles form and collapse when a liquid is energized by ultrasound. (Courtesy of K.S. Suslick and K. J. Kolbeck, University of Illinois; National Science Foundation.)

Instructor(s)

Prof. W. Craig Carter

MIT Course Number

3.00

As Taught In

Fall 2002

Level

Undergraduate

Some Description
Instructor(s)	Prof.
As Taught In	Spring 2002
Course Number	2.24
Level	Undergraduate/Graduate
Features	Lecture Notes, Student Work

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Course Description

Course Features

Course Description

Treatment of the laws of thermodynamics and their applications to equilibrium and the properties of materials. Provides a foundation to treat general phenomena in materials science and engineering, including chemical reactions, magnetism, polarizability, and elasticity. Develops relations pertaining to multiphase equilibria as determined by a treatment of solution thermodynamics. Develops graphical constructions that are essential for the interpretation of phase diagrams. Treatment includes electrochemical equilibria and surface thermodynamics. Introduces aspects of statistical thermodynamics as they relate to macroscopic equilibrium phenomena.

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(Redirected from Material property (thermodynamics))

Thermodynamics

Equilibrium / Non-equilibrium

State
Processes
Cycles

Process functions
Functions of state
Temperature / Entropy (introduction) Pressure / Volume Chemical potential / Particle number

Specific heat capacity

{displaystyle c=}

${displaystyle T}$	${displaystyle partial S}$
${displaystyle N}$	${displaystyle partial T}$

Compressibility

{displaystyle beta =-}

${displaystyle 1}$	${displaystyle partial V}$
${displaystyle V}$	${displaystyle partial p}$

Thermal expansion

{displaystyle alpha =}

${displaystyle 1}$	${displaystyle partial V}$
${displaystyle V}$	${displaystyle partial T}$

Internal energy
${displaystyle U(S,V)}$
Enthalpy
${displaystyle H(S,p)=U+pV}$
Helmholtz free energy
${displaystyle A(T,V)=U-TS}$
Gibbs free energy
${displaystyle G(T,p)=H-TS}$

History
Philosophy
Theories
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'An Experimental Enquiry Concerning .. Heat' 'Reflections on the Motive Power of Fire'
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Art Education

The thermodynamic properties of materials are intensive thermodynamic parameters which are specific to a given material. Each is directly related to a second order differential of a thermodynamic potential. Examples for a simple 1-component system are:

Compressibility (or its inverse, the bulk modulus)

Isothermal compressibility

{displaystyle beta _{T}=-{frac {1}{V}}left({frac {partial V}{partial P}}right)_{T}quad =-{frac {1}{V}},{frac {partial ^{2}G}{partial P^{2}}}}

Adiabatic compressibility

{displaystyle beta _{S}=-{frac {1}{V}}left({frac {partial V}{partial P}}right)_{S}quad =-{frac {1}{V}},{frac {partial ^{2}H}{partial P^{2}}}}

Specific heat (Note - the extensive analog is the heat capacity)

Specific heat at constant pressure

{displaystyle c_{P}={frac {T}{N}}left({frac {partial S}{partial T}}right)_{P}quad =-{frac {T}{N}},{frac {partial ^{2}G}{partial T^{2}}}}

Specific heat at constant volume

{displaystyle c_{V}={frac {T}{N}}left({frac {partial S}{partial T}}right)_{V}quad =-{frac {T}{N}},{frac {partial ^{2}A}{partial T^{2}}}}

Coefficient of thermal expansion

{displaystyle alpha ={frac {1}{V}}left({frac {partial V}{partial T}}right)_{P}quad ={frac {1}{V}},{frac {partial ^{2}G}{partial Ppartial T}}}

where P is pressure, V is volume, T is temperature, S is entropy, and N is the number of particles.

For a single component system, only three second derivatives are needed in order to derive all others, and so only three material properties are needed to derive all others. For a single component system, the 'standard' three parameters are the isothermal compressibility ${displaystyle beta _{T}}$ , the specific heat at constant pressure ${displaystyle c_{P}}$ , and the coefficient of thermal expansion ${displaystyle alpha }$ .

For example, the following equations are true:

{displaystyle c_{P}=c_{V}+{frac {TValpha ^{2}}{Nbeta _{T}}}}

{displaystyle beta _{T}=beta _{S}+{frac {TValpha ^{2}}{Nc_{P}}}}

The three 'standard' properties are in fact the three possible second derivatives of the Gibbs free energy with respect to temperature and pressure.

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