Non equilibrium systems

Slides:



Advertisements
Similar presentations
The thermodynamics of phase transformations
Advertisements

Gases, Liquids and Solids
Lecture 15. Phases of Pure Substances (Ch.5) Up to now we have dealt almost exclusively with systems consisting of a single phase. In this lecture, we.
Physical Transformations of Pure Substances
Behavior of Substance During A Process P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Selection of Substance for A Happening…..
Chapter 10 Phase Transformations in Metals (1)
Thermodynamics of surfaces and interfaces Atkins (ed. 10): §16C.2 Atkins (ed. 9): § Atkins (ed. 8): § Atkins (ed. 7): §
Chapter 6 Interpretation of Phase Diagrams Phase diagrams summarize in graphical form the ranges of temperature (or pressure) and composition over which.
I. Intermolecular Forces (Ch. 6, p )
LIQUIDS AND SOLIDS. LIQUIDS: Why are they the least common state of matter? 1. Liquids and K.M.T.  Are particles in constant motion? Spacing? Kinetic.
Phase Transitions: Liquid- Liquid Unmixing– Equilibrium Phase Diagram Soft-Condensed Matter Department of Physics,Tunghai-University.
Solidification and Grain Size Strengthening
A - 1 and kinetic particularities structural, thermodynamic The glassy "state",
Physical Transformations of Pure Substances
Liquids The particles that make up liquids are in constant motion too. Liquid particles are free to slide past one another. This allows liquids, as well.
Solids & Liquids. NM Standards Students know the atoms and molecules in liquids move in a random pattern relative to one another because the intermolecular.
Lecture 26: Crystallization PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
Materials science I - Metallic materials Metallic materials Solid state atomic structure atomic arrangement microstructure macrostructure Pure materials.
Dispersion Strengthening by Heat Treatment Chapter 11a – 4 th Edition Chapter 12a- 5 th Edition.
Schmid's Law F r = F cos λ A 0 = Acos ψ τ r = σ cos ψ cos λ.
Liquids and Solids The Condensed States of Matter Chapter 10.2 – 10.3.
CRYSTALLIZATION BY: TAHSEEN ISMAIL.
Solidification, Crystallization & Glass Transition  Cooling the Melt  solidification  Crystallization versus Formation of Glass  Parameters related.
Section 14.1 Intermolecular Forces and Phase Changes Steven S. Zumdahl Susan A. Zumdahl Donald J. DeCoste Gretchen M. Adams University of Illinois at Urbana-Champaign.
Nucleation and Growth of Crystals
Liquids and Solids 1. To learn about dipole-dipole, hydrogen bonding and London dispersion forces 2. To understand the effect of intermolecular forces.
Condensed States of Matter: Liquids and Solids Chapter 14
CHAPTER 14: LIQUIDS AND SOLIDS.  Condensed State- substances in these states have much higher densities than they do in the gaseous state CONDENSED.
Phase Transformation by Dr.Srimala.
1 Vanessa N. Prasad-Permaul Valencia College CHM 1046.
Liquids and Solids. Intermolecular Forces  Intermolecular Forces are the attraction between molecules  They vary in strength, but are generally weaker.
MIT Microstructural Evolution in Materials 12: Nucleation
Liquids and solids.
MIT Microstructural Evolution in Materials 15: Glass Transition
Liquids and Solids H2O (g) H2O (s) H2O ().
Liquids and Solids.
Liquids and Solids Chapter 12.
S as an energy relationship
Metals & Alloys.
College Prep Chemistry Mr. Pompilii
Heating Curves & Phase Change Diagrams
Nucleation & Growth Driving Force
Intermolecular Forces and
HEAT TREATMENT Improves properties of materials as it modifies the microstructure. Service performance of gears, cams, shafts, tools, dies and molds.
Chemistry Unit V Objectives Ch.13
Properties of Liquids The attraction between liquid particles is caused by the intermolecular forces: London dispersion forces dipole-dipole forces hydrogen.
MIT Microstructural Evolution in Materials 12: Nucleation
Lecture PowerPoint Chemistry The Molecular Nature of Matter and Change
Phase Changes.
Posibilities of strength-enhancing
Gases, Liquids and Solids
Phase Changes Friday, September 4th, 2015.
MIT Microstructural Evolution in Materials 13: Precipitate Growth
Properties of Solids and Liquids
Liquids and Solids Chapter 13.
Liquids and Solids Chapter 12.
Heating Curves & Phase Change Diagrams
Hypoeutectoid Steel T(°C) d L +L g (austenite) Fe3C (cementite) a
Introduction to the Phase Diagrams MME 293: Lecture 05
MIT Amorphous Materials 7: Viscoelasticity and Relaxation
Chapter 10 Two Types of Solids
Chapter 13.3 The Nature of Solids.
Units Matter, Energy, and Changes
Copyright©2000 by Houghton Mifflin Company. All rights reserved.
BASIC THERMODYNAMIC PRINCIPLES
Liquids and Solids Chapter 12.
CHAPTER 12 Liquids and Solids.
Thermodynamics Phase Changes.
Advanced material and technologies, MSc
States of Matter.
Presentation transcript:

Non equilibrium systems Advanced material and technologies, MSc 2017

What is the meaning of „equilibrium state"? phenomenology thermodynamic consideration The water-ice system is popular example 1 atm is 0 oC, T 0:supercooled liquid (metastable) Supersaturated solution: metastable. How metastability evolves generally? Atomic rearangements do not be able to succeed the cooling rate.

Fundamental terms: - stability - unstability - metastability Unstable materials are avoided by engineering practice, metastable states are often used. Examples: - unstable: highly deformed, high purity materials - metastability: diamond, martensite

Characters of metastable states They have a role in strength-enhancing. CHARACTER OF METASTABLE STATE EXAMPLES EXCESS ENERGY (RTm) EXCESS ENERGY J/mol) COMPOSITIONAL SUPERSATURATED SOLUTIONS  1 10 STRUCTURAL OVERCOOLED MELTS, AMORPHOUS METALS AND INTERMETALLIC PHASES  0.5 5 MORPHOLOGICAL OR TOPOLOGICAL NANO SIZED DISPERSION OF PHASES WITH HIGH SURFACES (TO VOLUME)  0.1 1

Kinetic consideration for the metastability formation Basic concept: relation between the rate of the energy subtraction and time-scale necessary for the atomic rearrangements in the case of delay Gm state will be frozen

Formation of metastable structure by melt quenching:

Property modification by grain size: Hall―Petch-equation:

Morphological metastability: nanostructured materials

Morphological metastability: clusters in condensed materials Materials with high specific surfaces Cluster: a set of small number of atoms that permanently or temporarily coincide during an observation process. Binding strength depends significantly on the number of atoms that form the cluster. The “size-related” properties between the individual properties of constituent atoms and the thermodynamically stable macroscopic properties. All properties are valid (in the thermodynamic sense) only for the macroscopic material!

Sintering (example for morphological metastability and technology based on it)

Tsintering  2/3 Tmelting The driving force behind the sintering process is to reduce surface energy: For example: in the case of Al2O3 powder with particle size of1μ, the surface of 10 cm3 material ≈ 1000 m2, and the interfacial energy is approx. 1 kJ. The change of density as a function of time and temperature: a: particle size C: constant Q: activation energy

Compositional metastability: k0: compositional partition coefficient in equilibrium state v: cooling rate

How does free enthalpy change during phase transition How does free enthalpy change during phase transition? (amorphous-crystalline, liquid-crystalline, crystallization from supersaturated solid solution) Assumed free enthalpy diagram for depicting the formation conditions of amorphous and crystalline states (am – amorphous phase,  – solid solution,  – compound) [21]

Slope of T0 curves and maximum supersaturation, solidification without compositional partition, phenomenon of glass forming What are the boundary conditions? Forming of supersaturated, crystalline solid solutions. Forming of metallic amorphous states (glassy alloys)