HANDOUT 4 - Dislocations and other stuff Flashcards
How do dislocations move in a material? Give a diagram (atomic level).
Dislocations move by the action of shear stress parallel to the slip plane.
Note that when a dislocation moves:
- no atom moves more than a fraction of the atomic spacing
- the adjacent set of atoms become the “half-plane”
Draw the process of a slip step being produced by the passage one dislocation (Burgers vector b).
Dislocations enable incremental slip by extending a few bonds at a time, which is why the stress required is so much less than the ideal strength.
Draw, describe and explain edge dislocations.
- shear stress and Burgers vector both at right angles to the dislocation
- dislocation moves in the direction of the stress
Draw, describe and explain screw dislocations.
- shear stress and Burgers vector both parallel to the dislocation.
- dislocation moves at right angles to the stress
- same slip step produced as for edge dislocation
Draw, describe and explain mixed dislocations.
More generally dislocations are mixed:
- curved, and varying between pure edge and pure screw
- move in a direction normal to the curve under the action of a shear stress (curved sections expand)
- net effect remains a slip step in the direction of the shear stress.
Explain why dislocations lead to specimens failing under loads smaller than theoretically calculated?
- crystals contain very man dislocations, with many different planes on which they can glide.
- in (virtually) any stress state, shear stresses exist to move dislocations.
Consider a crystal loaded in tension, with two dislocations crossing at 45o.
Net effect: crystal becomes longer and thinner by a small increment.
Replicating this increment x 1000s of dislocations on multiple slip planes produces continuum bulk plasticity.
Explain why plastic deformation occurs at constant volume.
Blocks of material slip past one another(dislocations) but the crystal packing is unaffected.
Give the equation relating the shear stress (tau), movement of dislocation b, and the resitance force f.
tb = f
t= tau
Why is the intrinsic lattice resistance to dislocation motion greater in technical ceramics (e.g. diamond) than metals?
Ceramics have covalent bonds which have high intrinsic resitance: high hardness
Metals have metallic bonds which have low intrinsic resistance: annealed pure metals are soft.
What is the equation that gives the energy(per unit length) T?
T ≈ Gb2/2
G = shear modulus
b = Burgers vector
Explain how dislocation pinning (with diagram) increases resistance to dislocations moving.
- It is pinned by the obstacles, and is forced to bow out between them, increasing the resistance per unit length.
- an additional shear stress ∆t (tau) is needed to overcome this resistance
As the dislocations bows out it applies a force to the obstacle:
force on obstacle = 2Tcos(theta)
dislocation escapes when either:
- force > obstacle strength ( theta > 0o )
- dislocation forms a semi-circle ( theta = 0o)
Show and explain how dislocation pass through weak obstacles.
Dislocations cut through or pass the obstacle.
Show(diagram) and explain how a dislocation passes through a “strong obstacle”.
Dislocations escape by leaving a loop of dislocation round the obstacle.
The contribution to the yield stress due to dislocation pinning depends directly on what 2 fixed paramaters and what 2 variable parameters?
Fixed paramaters:
- G: elastic shear modulus
- Burgers vector(atomic spacing)
Can be manipulated by processing parameters:
- L: obstacle spacing
- α: obstacle strength
Name the three different methods used on metals to pin dislocations.
- other dislocations: work hardening
- solute atoms: solid solution hardening
- particles of another solid (e.g. a compound): precipitation hardening