1. Material science & Metallurgy L D College of Engineering Mechanical Engineering 1

2. Prepared by:- Aghera Raj M. 140280119001 Khambhala Sahil R. 140280119039 Khodifad Kaushal V. 140280119041 Parmar Dipak 140280119061 2

3. Imperfections in Solids

4. The properties of some materials are profoundly influenced by the presence of imperfections. It is important to have knowledge about the types of imperfections that exist and the roles they play in affecting the behavior of materials. 4

5. 5 Atom Purity and Crystal Perfection If we assume a perfect crystal structure containing pure elements, then anything that deviated from this concept or intruded in this uniform homogeneity would be an imperfection. 1.There are no perfect crystals. 2.Many material properties are improved by the presence of imperfections and deliberately modified (alloying and doping).

6. 6 Vacancy atoms Interstitial atoms Substitutional atoms Point defects 1-2 atoms Types of Imperfections Dislocations Line defects 1-dimensional Grain Boundaries Area defects 2-dimensional

7. 7 Vacancies: -vacant atomic sites in a structure. Self-Interstitials: -"extra" atoms positioned between atomic sites. Point Defects in Metals Vacancy distortion of planes self- interstitial distortion of planes

8. In metals, a self interstitial introduces relatively large distortions (strain) in the surrounding lattice since the atom is substantially larger than the interstitial site. Self Interstitials

9. 9 Vacancies -- vacancies exist in ceramics for both cations and anions Interstitials -- interstitials exist for cations -- interstitials are not normally observed for anions because anions are large relative to the interstitial sites Adapted from Fig. 5.2, Callister & Rethwisch 3e. (Fig. 5.2 is from W.G. Moffatt, G.W. Pearsall, and J. Wulff, The Structure and Properties of Materials, Vol. 1, Structure, John Wiley and Sons, Inc., p. 78.) Point Defects in Ceramics Cation Interstitial Cation Vacancy Anion Vacancy

10. 10 Frenkel Defect To maintain the charge neutrality, a cation vacancy-cation interstitial pair occur together. The cation leaves its normal position and moves to the interstitial site. Schottky Defect To maintain the charge neutrality, remove 1 cation and 1 anion; this creates 2 vacancies. Adapted from Fig. 5.3, Callister & Rethwisch 3e. (Fig. 5.3 is from W.G. Moffatt, G.W. Pearsall, and J. Wulff, The Structure and Properties of Materials, Vol. 1, Structure, John Wiley and Sons, Inc., p. 78.) Point Defects: Frenkel and Schottky Schottky Defect Frenkel Defect

11. 11 We can get Q v from an experiment.  N v N = exp  Q v kT       Measuring Activation Energy Measure this... N v N T exponential dependence! defect concentration Replot it... 1/T N N v ln - Q v /k/k slope

12. 12 Point Defects in Polymers Defects due in part to chain packing errors and impurities such as chain ends and side chains Adapted from Fig. 5.7, Callister & Rethwisch 3e.

13. 13 What are the outcomes if impurity (B) is added to host (A)? Solid solution of B in A (random distribution of point defects) Solid solution of B in A plus particles of a new phase (usually for a larger amount of B) OR Substitutional solid solution. (e.g., Cu in Ni) Interstitial solid solution. (e.g., C in Fe) Second phase particle -- different composition -- often different structure. Imperfections in Metals

14. 14 Since there are both anions and cations in ceramics, a substitutional impurity will replace the host ion most similar in terms of charge. Charge balance must be maintained when impurities are present. Ex: NaCl Imperfections in Ceramics Na + Cl - Substitutional cation impurity without impurityCa 2+ impurity with impurity Ca 2+ Na + + Ca 2+ cation vacancy Substitutional anion impurity without impurity O 2- impurity O 2- Cl - anion vacancy Cl - with impurity

15. Point Defects: Impurities

16. 16 are line defects, slip between crystal planes result when dislocations move, produce permanent (plastic) deformation. Dislocations: Schematic of Zinc (HCP): before deformation after tensile elongation slip steps Line Defects

17. 17 Imperfections in Solids Linear defects (Dislocations) are one-dimensional defects that cause misalignment of nearby atoms. Linear defects are associated primarily with mechanical deformation. Types of dislocations: edge, screw, mixed. Burger’s vector, b: measure of lattice distortion Edge dislocation:  extra half-plane of atoms inserted in a crystal structure; the edge of the plane terminates within the crystal.  Around the dislocation line there is some localized distortion.  b perpendicular (  ) to dislocation line

18. 18 Dislocation motion requires the successive bumping of a half plane of atoms (from left to right). Bonds across the slipping planes are broken and remade in succession. The (plastic) permanent deformation of most crystalline materials is by dislocation movement. Most contain some dislocations that were introduced during solidification, plastic deformations, and rapid cooling (thermal stresses). To deform plastically means to slide atomic planes past each other. Atomic view of edge dislocation motion from left to right as a crystal is sheared. Motion of Edge Dislocation

19. The strength of a material with no dislocations is 20-100 times greater than the strength of a material with a high dislocation density. So, materials with no dislocations may be very strong, but they cannot be deformed.

20. 20 Imperfections in Solids Screw dislocation: –Named for the spiral stacking of crystal planes around the dislocation line; results from shear deformation –b parallel (  ) to dislocation line

21. Produces plastic deformation, Depends on incrementally breaking bonds. Plastically stretched zinc single crystal. If dislocations don't move, deformation doesn't happen! Dislocation Motion

22. 22 Dislocations During Cold Working Ti alloy after cold working. Dislocations entangle with one another during cold work. Dislocation movement becomes more difficult. Dislocations are visible in electron micrographs

23. 23 THANK YOU…