Dislocation: dynamics, interactions and plasticity Slip systems in bcc/fcc/hcp metals Dislocation dynamics: cross-slip, climb Interaction of dislocations.

Slides:



Advertisements
Similar presentations
DISLOCATIONS Edge dislocation Screw dislocation.
Advertisements

Forces B/w Dislocations Consider two parallel (//) edge dislocations lying in the same slip plane. The two dislocations can be of same sign or different.
Other Types of Dislocations in FCC
Single Crystal Slip Adapted from Fig. 7.9, Callister 7e.
PLASTICITY.
Point Defects Figure 10-4 illustrates four types of point defects.
ASE324: Aerospace Materials Laboratory Instructor: Rui Huang Dept of Aerospace Engineering and Engineering Mechanics The University of Texas at Austin.
Deformation Micromechanics DUCTILE DEFORMATION AND BRITTLE-DUCTILE TRANSITION.
Deformation and Strengthening Mechanisms
Dislocations – Linear Defects –Two-dimensional or line defect –Line around which atoms are misaligned – related to slip Edge dislocation: –extra half-plane.
What is it? What is it? (Quiz)
Chapter 7: Dislocation and Strengthening Mechanism
Dislocations and Strengthening
Crystallographic Aspects of Dislocations
Dislocations zBasic concepts yedge dislocation yscrew dislocation zCharacteristics of Dislocations ylattice strains zSlip Systems yslip in single crystals.
Most metals and alloys have either bcc or close-packed (fcc or hcp) crystal structures Close packed (hexagonal or cubic) hcp ccp Metals and Alloys: Mechanical.
CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality.
DISLOCATION MOVEMENT.
V Multiscale Plasticity : Dislocation Dynamics ta
Chapter 7: Dislocation and Strengthening Mechanism
Discussion Notes Farzana Ansari Feb 14 & 16, 2012.
Stress Fields and Energies of Dislocation. Stress Field Around Dislocations Dislocations are defects; hence, they introduce stresses and strains in the.
Lecture 3.0 Structural Defects Mechanical Properties of Solids.
Twinning Dislocation Reactions
1 Strength and Ductility. 2 Determining Tensile Strength from the stress-strain curve is easy. Just locate the highest point on the curve. TS = 82 ksi.
Fracture Mechanic Dr.Behzad Heidar shenas. Course Outline -An overview on the materials characteristics: 1.Types of crystal structures 2. Defects 3.Stress-Strain.
5/6/2002, Monday Summary: What we learned from this course?
Crystal defect classification point defects self-vacancy, self-interstitial interstitial interstitial and substitutional impurities point defect pairs,
IMPERFECTIONS IN SOLIDS
OBSTACLES IN DISLOCATION MOTION
Lecture 22: The mechanism of plastic deformation, part 2
Dislocation And Strengthening Mechanisms Plastic deformation through dislocation: Slip Ideal shear stress d a   ~ G d/a ~ 10 6 psi (calc.) ~ 10~10 3.
Last class More mechanical testing
Plastic Deformation Permanent, unrecovered mechanical deformation  = F/A stress Deformation by dislocation motion, “glide” or “slip” Dislocations –Edge,
Lecture 20: The mechanism of plastic deformation PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
PLASTIC DEFORMATION Dislocations and their role in plastic deformation.
Last lecture Introduction to materials science and engineering Atoms / electron configuration.
The Structure and Dynamics of Solids
Interactions of Quasiparticles
Objectives of Chapter 4 Introduce the three basic types of imperfections: point defects, line defects (or dislocations), and surface defects. Explore.
CHAPTER 10 Mechanical Properties: Dislocations and Plastic Deformation
Friday 12:00 Geology Seminar Dr. Lucy Flesch, Purdue University
Lectures 7 and 8 Dislocations: Foundations of Plastic Deformation ME 330 Engineering Materials Please read Chapters 4 and 7 Dislocation definitions Dislocation.
부산대학교 재료공학부 계면공학 연구실 [Mechanical Properties]  Mechanical Properties: mechanical properties of a material are those properties that involve a reaction.
부산대학교 재료공학부 계면공학 연구실 [Mechanical Properties]  Mechanical Properties: mechanical properties of a material are those properties that involve a reaction.
Nanomechanics Simulation Tool- Dislocations Make or Break Materials Michael Sakano, Mitchell Wood, David Johnson, Alejandro Strachan Department of Biomedical.
Plastic deformation Extension of solid under stress becomes
Technology for a better society 1 Imaging Dislocations.
Materials Science Chapter 8 Deformation and Fracture.
Material science & Metallurgy L D College of Engineering Mechanical Engineering 1.
Theoretical shear strength of a solid
Yield strength: the elongation of a mat'l
Sal College of Engineering
Play movie  LINE DEFECTS Dislocations: • are line defects,
Imperfections in ordered structures
Dislocations and Strengthening
Engineering materials lecture #12
Plastic Deformation Permanent, unrecovered mechanical deformation
Lecture 9/2: Dislocations
Basic Metallurgy Tomotsugu Sawai Director
Lecture 8: Dislocations
Structure and manufacturing Properties of Metals
مروري بر نابجايي ها صفحه اي كه خط نابجايي را در برمي گيرد صفحه لغزش ناميده مي شود. جهت لغزش در جهت حركت خط نابجايي است مقدار لغزش(slip distance) بوسيله.
The Ohio State University
Dislocations Dislocations Dislocations
Theoretical shear strength of a solid
CREEP CREEP Dr. Mohammed Abdulrazzaq Materials Engineering Department.
CRYSTAL IMPERFECTIONS
PLASTIC DEFORMATION & DISLOCATIONS
Presentation transcript:

Dislocation: dynamics, interactions and plasticity Slip systems in bcc/fcc/hcp metals Dislocation dynamics: cross-slip, climb Interaction of dislocations Intersection of dislocations

Edge/screw/mixed dislocations? Screw: Burgers vector parallel to the dislocation line. Edge: Burgers vector normal to the dislocation line.

Dislocation dynamics EdgeScrew Slip Direction|| to b|| to b  between line and b  || Line movement rel. to b||  How can disloc. leave slip planeclimb cross-slip n=( ) n=(111) b u b=n 1 xn 2 = (111)x ( ) = Climb: diffusion controlled. Important mechanism in creep.

Slip systems in crystals BCC FCC HCP {110} {211} {321} {0001} (10-10) (10-11) {111}  Fe, Mo, W,  brass  Fe, Mo, W, Na  Fe, K

b Superdislocation and partial dislocations Superdislocations in ordered material are connected by APB b Motio n of partial s Separation of partials Partial Dislocations b = b 1 + b 2 If energy is favorable, Gb 2 > Gb Gb 2 2 then partial dislocation form. ( Ga 2 /2 > Ga 2 /3)

Sessile dislocation in fcc n=(001) motion b Unless lock (sessile dislocation) is removed, dislocation on same plane cannot move past. n motion Lormer-Cottrell lockLormer lock

Sessile dislocation in bcc [001] is not a close-packed direction -> brittle fracture

Edge dislocation stress field y=x y=–x

Edge dislocations interaction edges dislocations with identical b X=Y repulsive attractive Stable at X=0 for identical b; Stable at X=Y for opposite b.

Edge dislocations interaction (general case) For an edge dislocations

Screw dislocations interaction Example: two attracting screws u (1) = (001) =u (2) b (1) = (001)b = –b (2) b1b1 radial force b1b1 r 1 2

Edge-Edge Interactions: creates edge jogs Dislocation 1 got a “jog” in direction of b 2e of the other dislocation; thus, it got longer. Extra atoms in half-plane increases length. This dislocation got a jog in direction of b 1e. after b 1e b 2e before b 1e b 2e **Dislocations each acquire a jog equal to the component of the other dislocation’s Burger’s vector that is normal to its own slip plane.

Dislocation intersection Interaction of two edges with parallel b Two screw kinks (screw) Edge jog on the edge Edge kink on the screw Edge jogs on screws