10.2 - Recovery & recrystallisation

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Last updated 9:39 AM on 6/22/26
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6 Terms

1
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What’s cold deformation?

What does it lead to?

A deformation that occurs at temperatures below the recrystallisation temperature

→ highly increases dislocation density :)

→ decreases plastic deformability :(

Note: high dislocations density = high energy = thermodynamically unstable

2
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What if the (“low”) temperature is maintained after cold deformation?

What can we do to overcome this?

The metal keeps its changes it underwent during cold deformation, including the plastic deformability decrease :(

→ a heat treatment allows to counteract / undo the damage

→ = annealing (recovery OR recrystallisation)

3
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What is the heat treatment used after cold deformation to counteract damage called?

What are the 2 different stages of it? Explain them. How are they activated?

Annealing: recovery OR recrystallisation

Recovery = rearrangement of lattice defects (dislocations) to a more stable state (lower energy) w/ changing grains shape & size → slight reduction of the dislocations density

→ occurs at LOW temperatures

Recrystallisation = complete microstructure reconstruction

→ the old, stressed, deformed grains completely disappear, being consumed by new forming grains

→ occurs at HIGH temperatures

They’re thermally activated

4
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What are the prerequisites for recovery?

(Mechanisms, how the lattice defects move to rearrange)

Explain how they work.

  • climbing of edge dislocations

→ at high temperatures, thermal energy drives diffusion, which makes atoms move towards less dense areas

→ atoms diffuse towards vacancies

→ if a vacancy appears at the end of the edge dislocation, it has “climbed” up of one atom and is no longer on the slip plane

Non-conservative” because it needs to absorb or release point defects (vacancies or interstitial atoms)

Requires high temperatures

  • cross slip of screw dislocations

→ gliding of dislocations is not constrained to a single slip plane

→ when a screw dislocation is gliding forward on its primary plane & encounters a hindrance (obstacle), it simply switches onto an intersecting slip plane that crosses its original path

→ the dislocation glides along this alternative “detour” plane & and then switch back onto a plane parallel to its original path

Conservative” because it doesn’t need any atom diffusion

Can happen with lower temperatures

The metals gets softer because both edge & screw dislocations use their thermal energy to overcome obstacles → lower energy = more stable state = less internal stresses

<ul><li><p><strong>climbing of edge dislocations</strong></p></li></ul><p>→ at high temperatures, thermal energy drives diffusion, which makes atoms move towards less dense areas</p><p>→ atoms diffuse towards vacancies</p><p>→ if a vacancy appears at the end of the edge dislocation, it has “climbed” up of one atom and is no longer on the slip plane</p><p></p><p><em>“<u>Non-conservative</u>” because it needs to absorb or release point defects (vacancies or interstitial atoms)</em></p><p><em>Requires high temperatures</em></p><p></p><ul><li><p><strong>cross slip of screw dislocations</strong></p></li></ul><p>→ gliding of dislocations is not constrained to a single slip plane</p><p>→ when a screw dislocation is gliding forward on its primary plane &amp; encounters a hindrance (obstacle), it simply switches onto an intersecting slip plane that crosses its original path</p><p>→ the dislocation glides along this alternative “detour” plane &amp; and then switch back onto a plane parallel to its original path</p><p></p><p><em>“<u>Conservative</u>” because it doesn’t need any atom diffusion</em></p><p><em>Can happen with lower temperatures</em></p><p></p><p>The metals gets softer because both edge &amp; screw dislocations use their thermal energy to overcome obstacles → lower energy = more stable state = less internal stresses</p>
5
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When does recovery occur?

What are the 2 key recovery mechanisms? (How do dislocations rearrange?)

Occurs at low temperatures

  • polygonisation

→ edge dislocations with the same sign arrange themselves into subgrain boundaries (small angle)

  • annihilation: small reduction of dislocation density

→ edge / screw dislocations with opposite signs cancel out

Scenario 1: edge dislocations with same dislocation line but different slip planes

→ atoms diffuse to region of tensions (in between the 2 edge dislocations) which cancels both of them, leading to a normal crystal lattice

Scenario 2: an edge dislocation encounters an obstacle on its path

→ the dislocation climbs up to another slip plane with diffusion

→ if it meets another dislocation with opposite sign on this slip plane, they cancel out

Scenario 3: a screw dislocation changes its slip plane by cross-slip

→ a screw dislocation goes onto another slip plane by cross-slip and can cancel out if it encounters another dislocation with opposite sign

<p>Occurs at <strong>low</strong> <strong>temperatures</strong></p><p></p><ul><li><p><strong>polygonisation</strong></p></li></ul><p>→ edge dislocations with the same sign arrange themselves into subgrain boundaries (small angle)</p><p></p><ul><li><p><strong>annihilation: <u>small</u> reduction of dislocation density</strong></p></li></ul><p>→ edge / screw dislocations with opposite signs cancel out</p><p><u>Scenario 1</u>: edge dislocations with same dislocation line but different slip planes</p><p>→ atoms diffuse to region of tensions (in between the 2 edge dislocations) which cancels both of them, leading to a normal crystal lattice</p><p></p><p><u>Scenario 2</u>: an edge dislocation encounters an obstacle on its path</p><p>→ the dislocation climbs up to another slip plane with diffusion</p><p>→ if it meets another dislocation with opposite sign on this slip plane, they cancel out</p><p></p><p><u>Scenario 3</u>: a screw dislocation changes its slip plane by cross-slip</p><p>→ a screw dislocation goes onto another slip plane by cross-slip and can cancel out if it encounters another dislocation with opposite sign</p>
6
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When and how does the recrystallisation occur?

Occurs at high temperatures

  1. The initial structure contains deformed grains with high dislocation density → recrystallisation begins with the formation of nuclei (new, dislocation-free grains)

  1. Grain growth: nuclei grow by consuming the surrounding deformed grains

  1. When the deformed grains are fully consumed, the final recrystallised microstructure consists of large, dislocation-free grains (large-angle grain boundaries)

<p>Occurs at <strong>high temperatures</strong></p><p></p><ol><li><p>The initial structure contains deformed grains with high dislocation density → recrystallisation begins with the formation of nuclei (new, dislocation-free grains)</p></li></ol><p></p><ol start="2"><li><p>Grain growth: nuclei grow by consuming the surrounding deformed grains</p></li></ol><p></p><ol start="3"><li><p>When the deformed grains are fully consumed, the final recrystallised microstructure consists of large, dislocation-free grains (large-angle grain boundaries)</p></li></ol><p></p>