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

Combined thermal, solutal and momentum transport. Assume a rigid mold. Imperfect contact and air gap formation at metal/mold interface Design of mold surface.
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.
Solidification and Grain Size Strengthening
Solidification of Pb-Sn Alloys Teri Mosher University of Illinois Advisor: Professor Krane.
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 Nov
Chapter 9 Preview Objectives Defining Temperature Thermal Equilibrium
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.
Introduction to Materials Science, Chapter 9, Phase Diagrams University of Virginia, Dept. of Materials Science and Engineering 1 Growth of Solid Equilibrium.
Materials science I - Metallic materials Metallic materials Solid state atomic structure atomic arrangement microstructure macrostructure Pure materials.
Numerical Simulation of Dendritic Solidification
27 October 2005 Konstantin Blyuss, University of Exeter 1 Konstantin Blyuss, University of Exeter 1 Spatio-temporal dynamics in a phase- field model with.
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.
Analysis of DTA data for binary alloys
Lecture 7 Review of Difficult Topics MATLS 4L04: Aluminum Section.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Chapter 17 Honors Chemistry Thermochemistry.
Agenda 4/16/2013 Turn in Test Corrections Part 1 – Rates of Reaction Slip Quiz part 1 Objectives Study Guide – switch and grade – to turn in. Related Released.
 Course number: 527 M1700  Designation: Graduate course  Instructor: Chao-Sung Lin, MSE Dept., (office), (lab)  Office hours: 2 ~
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 14: Interface Stability
MIT Microstructural Evolution in Materials 12: Nucleation
Phase diagrams of unary and binary systems
Chapter 10: Phase Transformations
Topic Name : Solid solution
MSE 440/540: Processing of Metallic Materials
Engineering Materials and Processes Lecture 9 – Equilibrium diagrams
MIT Microstructural Evolution in Materials 13: Precipitate Growth
Material Science & Metallurgy Non Equilibrium Cooling
definite volume definite shape regular geometric pattern
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 Amorphous Materials 3: Glass Forming Theories
MIT Microstructural Evolution in Materials 8: Ionic Conductivity
Metals & Alloys.
States of Matter Solid Liquid Gas definite volume definite shape
Sr. no. Name Enrollment no. Roll no. 1 Jay sureja Hardik tanna 44
Solid Solution Thermal Equilibrium Diagram
Solid Solutions and Phase Equilibrium
MIT Microstructural Evolution in Materials 2: Solid Solutions
Nucleation & Growth Driving Force
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
MIT Microstructural Evolution in Materials 6: Substitutional Diffusion
Solidification of Metals and Alloys
Bell Work: Exo or Endo? Absorbs heat. Releases heat.
MIT Microstructural Evolution in Materials 8: Ionic Conductivity
MIT Microstructural Evolution in Materials 16: Glass Transition
MIT Amorphous Materials 3: Glass Forming Theories
MIT Microstructural Evolution in Materials 13: Precipitate Growth
2/16/2019 9:54 PM Chapter 9 Phase Diagrams Dr. Mohammad Abuhaiba, PE.
Single solid phase binary alloy -1
Liquids and Solids Chapter 12.
CHAPTER 8 Phase Diagrams 1.
CHAPTER 8 Phase Diagrams 1.
Non equilibrium systems
Hypoeutectoid Steel T(°C) d L +L g (austenite) Fe3C (cementite) a
CHAPTER 8 Phase Diagrams 1.
Working with Phase Diagrams
Eutectic Type Phase Diagrams
Phase Diagram.
The simplest picture of the atomic structure of metallic crystals is one of spherical ions closely packed and existing in a ‘sea’ of conduction electrons.
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 © Aqueous Technologies

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 melt

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 Image credit: University of Cambridge CC BY-NC-SA 2.0 UK Image credit: Alexey Kljatov CC BY-SA 4.0

“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 (C0) C0 TL (CL) 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)

R ALL 3.022 PARTICIPANTS ® THE FOLLOWING PREVIEW HAS BEEN APPROVED FOR RESTRICTED VIEWERS WHO HAVEN’T TAKEN KINETICS REQUIRE ACCOMPANYING MIT DMSE STUDENTS STRONG MATERIALS SCIENCE COMPONENTS ® www.classratings.com dmse.mit.edu

“Microstructural Evolution in Foods” We proudly present “Microstructural Evolution in Foods” Image Credit: profkarim CC BY-SA 2.0

List of symbols DT – supercooling, defined as the difference between the liquidus temperature and the phase transition temperature Tm – melting point or liquidus temperature T – temperature x – coordinate along the x-axis kS / kL – thermal conductivity of solid / liquid phase R – precipitate growth rate measured by the velocity of the solid-liquid interface DHm – enthalpy of fusion per unit volume CB – concentration of component B C0 – concentration of B in the starting liquid phase

List of symbols T0 – temperature at which the solidification takes place Ca / CL – equilibrium concentration of component B in the a / liquid phase at T0 D – diffusion coefficient of B in the liquid phase TL – liquidus temperature of the A-B binary alloy, which is a function of the alloy composition CB