MIT Microstructural Evolution in Materials 14: Interface Stability

Slides:



Advertisements
Similar presentations
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.
Advertisements

Alloy Solidification Def. Partition coefficient k
Water, Steam, and Ice 1 Water, Steam, and Ice. Water, Steam, and Ice 2 Introductory Question A glass of ice water contains both ice and water. After a.
Chapter 10 Phase Transformations in Metals (1)
Solidification and Strengthening Chapter 9
Viscoelastic response in soft matter Soft matter materials are viscoelastic: solid behavior at short time – liquid behavior after a time  Shear strain;
Class 4a: Atmospheric moisture. Introduction to water Earth’s temperature  special properties of water.
Solidification and Grain Size Strengthening
An Enthalpy—Level-set Method Vaughan R Voller, University of Minnesota + + speed def. Single Domain Enthalpy (1947) Heat source A Problem of Interest—
Solidification of Pb-Sn Alloys Teri Mosher University of Illinois Advisor: Professor Krane.
Carnegie Mellon October 23, 2001Robert F. Sekerka for the Materials Science DWG 1 Presentation to the Committee on Microgravity Research by Robert F.
Nucleation Don H. Rasmussen Box 5705 Clarkson University
NC State University Department of Materials Science and Engineering1 MSE 440/540: Processing of Metallic Materials Instructors: Yuntian Zhu Office: 308.
SOLIDIFICATION OF CASTING TEHCHNOLOGY
Materials Process Design and Control Laboratory Sibley School of Mechanical and Aerospace Engineering 169 Frank H. T. Rhodes Hall Cornell University Ithaca,
Changes of State Solid to Liquid to Gas and Back.
NTNU Short Course on solidification at IISc October – November 2012 Lars Arnberg, NTNU 1.Introduction – basic concepts 29/10 1.Nucleation - grain refinement.
Lecture 26: Crystallization PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
Growing Numerical Crystals Vaughan Voller, SAFL Feb
NTNU 1 Solidification, Lecture 4 Three phase solidification Eutectic growth Types of eutectics Peritectic growth Segregation Macro / microsegregation Lever.
Materials science I - Metallic materials Metallic materials Solid state atomic structure atomic arrangement microstructure macrostructure Pure materials.
The Solid State Solids have both definite volume and definite shape. The geometric stability of a solid: is not due to any difference in compactness between.
Schmid's Law F r = F cos λ A 0 = Acos ψ τ r = σ cos ψ cos λ.
PHASE DIAGRAMS THEORY AND APPLICATIONS. Some basic concepts u Phase A homogeneous region with distinct structure and physical properties In principle,
Mechanical & Aerospace Engineering West Virginia University 9 – Phase Diagram (2) (Phase Reactions)
Numerical Simulation of Dendritic Solidification
Crystal Growth General Formalism    Phase growing into  with velocity v : f ( “site factor” ) : fraction of sites where a new atom can be incorporated.
NTNU 1 Solidification, Lecture 3 1 Interface stability Constitutional undercooling Planar / cellular / dendritic growth front Cells and dendrites Growth.
Sensible Heat and Enthalpy Calculations. constant = A Enthalpy increment equation.
Lecture 7 Review of Difficult Topics MATLS 4L04: Aluminum Section.
Materials Process Design and Control Laboratory MULTISCALE COMPUTATIONAL MODELING OF ALLOY SOLIDIFICATION PROCESSES Materials Process Design and Control.
Phase Transformation by Dr.Srimala.
MIT Microstructural Evolution in Materials 6: Substitutional Diffusion Juejun (JJ) Hu
MIT Microstructural Evolution in Materials 16: The Science of Ice Cream Juejun (JJ) Hu Ice Cream.
MIT Microstructural Evolution in Materials 12: Nucleation
Chapter 10: Phase Transformations
MSE 440/540: Processing of Metallic Materials
Dynamic methods to construct phase diagrams
MIT Microstructural Evolution in Materials 13: Precipitate Growth
Material Science & Metallurgy Non Equilibrium Cooling
MIT Microstructural Evolution in Materials 15: Glass Transition
Juejun (JJ) Hu MIT Microstructural Evolution in Materials 10: Faceted and Non-Faceted Growth Juejun (JJ) Hu
DR S. & S. S. GHANDHY GOVERNMENT ENGINEERING COLLEGE , SURAT.
MIT Microstructural Evolution in Materials 8: Ionic Conductivity
Metals & Alloys.
Sr. no. Name Enrollment no. Roll no. 1 Jay sureja Hardik tanna 44
Fundamentals of Metal-Casting
Solid Solution Thermal Equilibrium Diagram
Solid Solutions and Phase Equilibrium
MIT Microstructural Evolution in Materials 2: Solid Solutions
Nucleation & Growth Driving Force
23-1 Atmospheric moisture.
MIT Microstructural Evolution in Materials 12: Nucleation
MIT Microstructural Evolution in Materials 2: Solid Solutions
Numerical Simulation of Dendritic Solidification
Growth Kinetics Byeong-Joo Lee Microstructure Evolution POSTECH - MSE
Solidification of Metals and Alloys
MIT Microstructural Evolution in Materials 13: Precipitate Growth
Phase Diagram Vocabulary Triple Point: Only point at which all three phases (solid, liquid, gas) exist at equilibrium Critical Point: Point at which.
Atmospheric Moisture Atmospheric moisture is a very important topic under the theme of climatic system. In this presentation, you can make use of photos.
2/16/2019 9:54 PM Chapter 9 Phase Diagrams Dr. Mohammad Abuhaiba, PE.
Single solid phase binary alloy -1
CHAPTER 8 Phase Diagrams 1.
CHAPTER 8 Phase Diagrams 1.
MIT Microstructural Evolution in Materials 14: Interface Stability
CHAPTER 8 Phase Diagrams 1.
Working with Phase Diagrams
Eutectic Type Phase Diagrams
13.4 Sublimation The change of a substance from a solid to a vapor without passing through the liquid state is called sublimation. Sublimation occurs.
Mechanical Properties of Isomorphous Alloys
Presentation transcript:

Juejun (JJ) Hu hujuejun@mit.edu MIT 3.022 Microstructural Evolution in Materials 14: Interface Stability Juejun (JJ) Hu hujuejun@mit.edu

Dendritic growth during solidification

Condition for dendritic growth: interface instability Solid Liquid x A B Stable interface: planar growth Solid Liquid Interface stability deals with macroscopic interface morphology, whereas the Jackson model evaluates atomic scale interface roughness x A B Unstable interface: dendritic growth

Example 1: Bridgman-Stockbarger crystal growth From Ames Lab 101: Single Crystal Growth

Example 1: Bridgman-Stockbarger crystal growth Solid Liquid T Heat flux Tm Single-component system x

Example 1: Bridgman-Stockbarger crystal growth Heat flux continuity at solid-liquid interface Supercooling in liquid Solid Liquid T Heat flux Tm Single-component system Planar interface results in Bridgman growth x

Example 2: Solidification in a supercooled liquid Heat flux continuity at solid-liquid interface Supercooling in liquid Solid Supercooled liquid T Heat flux Tm Heat extraction is more efficient at dendrites Single-component system x

Dendrite branching and crystallography <100> Directionally solidified Co-Sm-Cu alloy W. Kurz, EPFL, Switzerland Snowflake under microscope

“At sub-zero temperature, moisture from the surrounding atmosphere condenses almost immediately. The dendritic form of the crystallization is a natural fractal pattern.” – Francis Chee / Science Photo Library

Example 3: constitutional supercooling Ca CL Solid a Liquid L L CB T0 CL a b C0 Ca x A C0 B x = 0

Example 3: constitutional supercooling Steady state solution Solid a Liquid L Growth rate is determined by diffusion of solute away from the interface RDt CB CL C0 Ca x x = 0

Example 3: constitutional supercooling Liquidus temperature Supercooling in liquid B T0 b L A C0 Ca CL a Interface stability condition

Example 3: constitutional supercooling Solid a Liquid L Solid a Liquid L CB TL Critical T (x) CL Supercooling zone DT (x) > 0 TL (CL) C0 TL (C0) Ca x x x = 0 x = 0

Summary Interface stability criterion: supercooling decreases away from the solid-liquid interface Single-component system: Binary or multi-component system: In single component systems, latent heat removal from the solid phase side usually indicates stable interface Phase transition occurring at condition far away from equilibrium (large supercooling) is often accompanied by dendritic growth Impurities can lead to constitutional supercooling and dendrite growth (even in nominally ‘single-component’ alloys)