lecture 10 Flashcards

1
Q

slip can not occur in

A

a pure normal stress requires shear stress

can occur in a tensile test as force applied by normal stress causes shear stress at certain directions within material

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2
Q

critical shearing stress

A

stress required to start slip

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3
Q

shear stress =

A

tau c* sin (2 pi x /b)

where tau c is critical shear stress and b is the diameter of atoms or nearest neighbour distance

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4
Q

what does the frenkel model predict critical shear stress to be and why is this not very accurate

A

critical shear modulus tau c = shear modulus/2pi ie shear stress to cause slip is way above what it should be
but experimentally tc <= G/10^3 ie way lower

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5
Q

What is the issue with the frenkel model

A

way too simplistic something missing - overestimates the critical shear modulus by huge amount
sees it as breaking all bonds at once which requires alot of energy but can just move a defect along by only breaking a few bonds
linear defect seperating slipped and unslipped regions can move at much lower forces than bonding energy

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6
Q

plastic deformation occurs at

A

forces way below forces holding atoms together - yield shouldnt occur at such low forces

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7
Q

why was plastic deformation occuring at forces way below forces holding atoms together

A

defects in materials

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8
Q

what is the carpet analogy equivalent to

A

fenkel model sees it as breaking all bonds at once (moving the whole carpet) which requires alot of energy but can just move a defect along by only breaking a few bonds
linear defect seperating slipped and unslipped regions can move at much lower forces than bonding energy

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9
Q

edge dislocation diagram

A

extra plane of atoms somewhere in the middle
forces atoms around it out causing associated elastic energy
size of dislocation = nearest neighbour distance - one in powerpoint perfect unit disloaction

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10
Q

screw dislocation diagram

A

twisted the sample

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11
Q

types of dislocation

A

screw dislocation
edge dislocation
combination of both

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12
Q

how can edge dislocation lead to elongation

A

pushing the plane of atoms out to the end of material

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13
Q

screw dislocation

A

can be untwisted material gets a little bit longer

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14
Q

when screw dislocation and edge dislocation lead to elongation what forms

A

slip planes (close packed planes) crystal structure very similar but moved slightly

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15
Q

slip planes are

A

lowest energy path bonds are relatively weak

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16
Q

slip tends to occur on what plane for FCC

A

along close packed planes - the (111) plane - 4 of these in a unit cell {111}

17
Q

how many slip directions are there and therefore how many slipping systems are there in FCC

A

3 directions therefore 12 slipping systems 4 x 3 (12 directions the planes could slip along)

18
Q

close packed planes of atoms moving over due

A

to defects helping them

19
Q

not all dislocations are perfect may get

A

partial or imperfect dislocations where the passage of disloaction does not leave the structure unchange
locally change structure may start with FCC end with HCP (dont consider impartial dislocations)

20
Q

what are the three slip directions diagram for FCC

A

putting negatives put should be bar
[1 0 -1] same as [-1 0 1] (reverse direction)
[1 -1 0] same as [-1 1 0]
[0 1 -1] same as [0 -1 1]

21
Q

Slip in HCP and BCC

A

HCP close backed basal plane very complicated to calculate
BCC no defined slip planes
dont need to calculate

22
Q

Slip bands produced when

A

object exposed to normal force but at certain angles end up with shearing stress

23
Q

what is the benefit of resolving forces

A

design orientation of cut of material and orientation of force applied such that material fails at much higher load as slip planes are never activated

24
Q

greek letter phi symbol

A

angle from normal to slip plane

25
Q

greek letter Lambda

A

angle from force to slip direction

26
Q

shearing stress equal to

A

stress applied * cos phi * cos * Lambda
critical shear stress = 0 if lambda or phi equal 90 degrees (normal stress no shearing stress)
critical shear stress = maximum if lambda = phi = 45 degrees

27
Q

when resoled shear stress is greater than

A

critical resolved shear stress then slip will occur

28
Q

what equation can be used to calculate cos phi =

A

direction of force (dot) slip plane= magnitude of direction of forces * magnitude of slip plane * cos phi
if look at formula sheet cos phi is slip plane and force

29
Q

what equation can be used to calculate cos lambda =

A

direction of force (dot) slip direction = magnitude of direction of forces * magnitude of slip direction* cos phi
if look at formula sheet cos lambda is slip direction against force

30
Q

when finding whether direction is activated

A

calculate cos phi and cos lambda (cos lambda will be specific to this direction)
shear stress = applied stress * cos phi * cos lambda
if critical shear stress is lower than calculated value then plane is active (if its negative its in opposite direction)

31
Q

difference between calculating cos phi and cos lambda

A

cos phi only need to calculate once (direction of force in comparison to slip plane is constant need to calculate cos lambda for all 3 directions)

32
Q

what will the slip plane be

A

slip plane will always be (1 1 1) as we only look at the FCC term

33
Q

What will the slip directions be

A

they will be the three slip direction for FCC [1 -1 0] [0 1 -1] and [1 0 -1] (one zero one and negative one in three combinations)

34
Q

what will the applied force be

A

will be the vector direction of the force eg [2 1 0]

35
Q

if resolved stress is greater than critical shear stress but negative

A

slip will occur but in opposite direction to one specified

ie [1 -1 0] to [-1 1 0]

36
Q

EBSD image shows

A

crystal orienation

37
Q

texturing materials

A

make crystal structure all similar means slipping that occurs is very controlled