To study the mechanical properties of NANOPERM and FINEMET alloys.

Slides:



Advertisements
Similar presentations
Changes in Matter Chapter 3 sections 1 and 3. Solid Definite Shape and Definite Volume.
Advertisements

Acero 2000 PHYSICAL METALLURGY AND THERMAL PROCESSING OF STEEL
11 MODIFICATION OF AMORPHOUS Co-BASED METAL ALLOY BY SHOCK-WAVE LOADING A.Z.Bogunov, R.S.Iskhakov, V.I.Kirko, A.A.Kuzovnikov JSC « Pulse technologies »
Bonding in Metals OBJECTIVES:
Ionic, Covalent and Metallic structures of solids
Chapter 7 “Ionic and Metallic Bonding”
Chapter 7 “Ionic and Metallic Bonding”. Metallic Bonds are… l How metal atoms are held together in the solid. l Metals hold on to their valence electrons.
Metallic Bonding Strong forces of attraction are responsible for the high melting point of most metals.
The Structure of Metallic Glasses David Poerschke Materials 286g Final Presentation May 19, 2010.
Metallic Bonding Strong forces of attraction are responsible for the high melting point of most metals.
Group 2 Steels: Medium Carbon Alloy Steels (0.25 – 0.55 %C)
Deformation and Strengthening Mechanisms
PY3090 Preparation of Materials Lecture 3 Colm Stephens School of Physics.
Dislocations and Strengthening
Solidification of Pb-Sn Alloys Teri Mosher University of Illinois Advisor: Professor Krane.
IRON IRON-CARBON DIAGRAM
The Effects of Straining on Copper-Silver Hardness By: Dhanvir Aujla Advisor: Dr. Anthony Rollett Graduate Student: Samuel Lim.
Materials for Femtospin Project Colin Forbes
Electrons and Holes ECE Intrinsic Carrier Concentration Intrinsic carriers are the free electrons and holes that are generated when one or more.
Heat Treatment of Metals
Structures and Types of Solids
Chapter 5: Metals. Uses of Metals Metals in different forms are very noticeable all around us. We can see that: – The strength of metals is useful when.
Alloys and Solid Solutions Chemistry 123 Spring 2008 Dr. Woodward.
Metallic Bonds Chemistry Mrs. Coyle.
Force chemical mixing during severe plastic deformation Robert S. Averback, University of Illinois at Urbana-Champaign, DMR Understanding how atoms.
Alloys.
Synthesis and Characterization of Permanent Magnetic Nanocomposites Kunpeng Su, Xuehong Cui, Zhongwu Liu, and Dechang Zeng Introduction Suction cast magnets.
Physical Metallurgy 24 th Lecture MS&E 410 D.Ast
Structural featureDimension (m) atomic bonding missing/extra atoms crystals (ordered atoms) second phase particles crystal texturing <
Ni-Ti AND Ni-Mn-Ga NANOCRYSTALLINE SHAPE MEMORY ALLOYS AND COMPOSITES FOR NEXT GENERATION SENSORS AND ACTUATORS Teodor M. Breczko Lab of Functional Materials.
Dispersion Strengthening by Heat Treatment Chapter 11a – 4 th Edition Chapter 12a- 5 th Edition.
Metallic Glasses in Cell Phones Angelika Franz. Outline what is a metallic glass structure properties processing cell phone cases cell phone hinges.
The Nature of Solids. A Model for Solids The particles in solids are not free to move about. They tend to vibrate about fixed points. In most solids,
THE NATURE OF SOLIDS by Mike, Marc & Alex. A Model for Solids - Atoms, Ions or molecules are packed tightly together - dense and not easy to compress.
Europe Materials Collaboration Atomic Structure of Nanosize crystalline grains in diamond-SiC compsites Award Num: Intellectual Merit The primary.
M. Kopcewicz and T. Kulik a ) Institute of Electronic Materials Technology, Warszawa, Wólczyńska Street 133, Poland, a ) Faculty of Materials Science.
Types of Materials Metals : –Strong, ductile –high thermal & electrical conductivity –opaque Polymers/plastics : Covalent bonding  sharing of e’s –Soft,
Defects in Solids 0-D or point defects –vacancies, interstitials, etc. –control mass diffusion 1-D or linear defects –dislocations –control deformation.
CHAPTER 13 Kinetic Molecular Theory (K.M.T.). Kinetic Theory: Kinetic Theory: –The tiny particles in all forms of matter are in constant motion. constant.
Metallic Bonding Intermolecular Forces. Basic metallic properties Malleable: metals can be shaped into thin sheets Ductile: metals can be drawn into wires.
Chapter 7 “Metallic Bonding” Chemistry Grade 10. Bonding in Metals OBJECTIVES: –Explain the importance of alloys.
Amorphous Nanocomposite Materials Presented by: Renée E. Gordon Advisor: Professor Michael McHenry Graduate Student: Changyong Um.
Deformation and Strengthening Mechanisms of Materials
Discontinuities of Plastic Deformation in Metallic Glasses Ing. Mária Huráková školiteľ: RNDr. Kornel Csach, CSc. Ústav experimentálnej fyziky Slovenská.
Solids  Metallic Crystals  Alloys – mixtures of metals – done to strengthen or make a metal less brittle or subject to oxidation.  2 types  Substitutional.
Ch. 7.3 Bonding in Metals CHM 1. Metallic Bonds and properties Metals are made up of closely packed cations and free floating valence electrons –Sea of.
Fe-Carbon Diagram, TTT Diagram & Heat Treatment Processes
Metallurgy Background. Lesson Objectives When you finish this lesson you will understand: Phases of mater Crystal Structure & Crystal Defects Phase changes.
Enhanced hardness and fracture toughness of the laser-solidified FeCoNiCrCuTiMoAlSiB 0.5 high-entropy alloy by martensite strengthening Advisor : Tzu-Yao.
Lecture 7 Review of Difficult Topics MATLS 4L04: Aluminum Section.
Part I: Define in terms of crystal formation, alignment of the atoms. Then give an example where this might be used in everyday life, or an example of.
Materials Science Chapter 4 Disorder in solid Phases.
Wednesday, February 27, 2008 Section 14.3 Homework: Pg. 515: 34, 35, 38, 41.
Material science & Metallurgy L D College of Engineering Mechanical Engineering 1.
MatSE 259 Exam 1 Review Session 1.Exam structure – 25 questions, 1 mark each 2.Do NOT forget to write your student I.D. on the answer sheet 3.Exams are.
Materials Science Metals and alloys.
Chapter 10 – Liquids and Solids 10.4 – 10.5 Notes AP Chemistry.
Fe-Carbon Diagram, TTT Diagram & Heat Treatment Processes
CH. 12 SOLIDS & MODERN MATERIALS
Metals & Alloys.
Metals - Bonding and Crystal Structure
Metallic Bonds.
Chapter 4 Section 2 – Part 1.
Electronegativity and the types of bonds that form.
Liquids And Solids.
States of Matter Ch
Determination of Grain Size
MATERIALS SCIENCE Materials science investigates the relationships between the structures and properties of materials.
The Solid-State Structure of Metals and Ionic Compounds
Presentation transcript:

To study the mechanical properties of NANOPERM and FINEMET alloys. Mechanical Properties of Nanocomposite Alloys presented by Jennifer Barrow Goals: To study the mechanical properties of NANOPERM and FINEMET alloys. To prepare the materials for experiments at the NHMFL. Methods Used: Melt spinning, Calorimetry, Nanoindentation

Rapid Solidification Processing Amorphous Tape Wound Core Nanocrystallization & Calorimetry Magnetic properties are well known for FINEMET and NANOPERM Mechanical properties are not. A. Hsiao CMU Ph.d Thesis

Background Composition: Nanocrystallization reaction (primary): NANOPERM Fe88Zr7B4Cu1 FINEMET Fe73.53Si16.07B6.43Cu1.09Nb2.88 Nanocrystallization reaction (primary): NANOPERM AmorphousαFe+amorphous’ (amorphous’ being rich in B, Zr) FINEMET AmorphousFeSi +amorphous’ (amorphous’ being rich in Nb, B) Nanocrystallization on heating Material has interesting soft magnetic properties ~10 nm Fe-Zr liquid is quenched to its amorphous phase. Alpha iron crystallizes

Strengthening mechanisms (Fe,Fe3Si or FeCo based glass) Dense Random Packing of Hard Spheres (DRPHS): Amorphous Structure Crystalline periodicity:(Fe,Fe3Si or FeCo) Atom substitution puts strain on the crystal structure Explain how dense random packing structure comes about. Smaller atom substituted interstitially (B) Larger atom substituted (Zr)

NANOPERM Hardness Data Nanoindenter setup 19% vol Unique hardness trend is due to strengthening mechanisms within the amorphous structure. (interstitial or substitutional) 38% vol 0% vol 2% vol

Other observations in hardness data Surface crystallization skews hardness data at beginning of Hardness vs. X curve (don’t have X = 0 at the surface) Strengthening mechanisms (interstitial and substitutional) are cause for general increase in hardness. Drop in hardness at large X is due to the fact that with increased crystallization, the material takes on mechanical properties of the softer nanocrystals

Future Work Annealing samples to obtain X(t), or % composition vs. time and a complete TTT curve. Polishing samples in order to eliminate surface crystallization. Determining mechanical properties at large X

Acknowledgements Amy Hsiao’s Thesis Changyong Um Michael McHenry http://vulcan2.cwru.edu/classes/emse201/overheads/StreMech.pdf