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Stress, strain and more on peak broadening

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Title: Stress, strain and more on peak broadening


1
Stress, strain and more on peak broadening
  • Learning Outcomes
  • By the end of this section you should
  • be familiar with some mechanical properties of
    solids
  • understand how external forces affect crystals at
    the Angstrom scale
  • be able to calculate particle size using both the
    Scherrer equation and stress analysis

2
Material Properties
  • What happens to solids under different forces?
  • The lattice is relatively rigid, but.

Note materials properties will be considered
mathematically in PX3508 Energy and Matter
3
Mechanical properties of materials
  • Tensile strength tensile forces acting on a
    cylindrical specimen act divergently along a
    single line.

Compressive strength compressive forces on a
cube act convergently in a single line
4
Mechanical properties of materials
  • Shear strength shear is created by off-axis
    convergent forces.

Slipping of crystal planes
5
Stress
  • Stress force/area
  • In simplest form

Normal (or tensile) stress perpendicular to
material Shear stress parallel to material
6
Stress
  • Thus can resolve into tensile and shear
    components

Tensile stress, ? Shear stress, ?
7
Strain
  • Strain result of stress
  • Deformation divided by original dimension

8
The Stress-Strain curve
9
Elastic region
  • In the elastic region, ideally, if the stress is
    returned to zero then the strain returns to zero
    with no damage to the atomic/molecular structure,
    i.e. the deformation is completely reversed

10
Plastic region
  • In the plastic region, under plastic deformation,
    the material is permanently deformed/damaged as a
    result of the loading.

In the plastic region, when the applied stress is
removed, the material will not return to original
shape.
The transition from the elastic region to the
plastic region is called the yield point or
elastic limit
11
Failure
  • At the onset of yield, the specimen experiences
    the onset of failure (plastic deformation), and
    at the termination of the range of plastic
    deformation, the sample experiences a structural
    level failure failure point

12
Example
  • www.iop.org

13
Tensile strength
  • Maximum possible engineering stress in tension.
  • Metals occurs when noticeable necking starts.
  • Ceramics occurs when crack propagation starts.

14
Modulus
  • The slope of the linear portion of the curve
    describes the modulus of the specimen.
  • Youngs modulus (E) slope of stress-strain
    curve with sample in tension (aka Elastic
    modulus)
  • Shear modulus (G) - slope of stress-strain curve
    with sample in torsion or linear shear
  • Bulk modulus (H) slope of stress-strain curve
    with sample in compression

Hookes law ? E ?
15
Modulus - properties
  • Higher values of modulus (steeper gradients of
    slope in stress-strain curve) relates to a more
    stiff/brittle material more difficult to deform
    the material
  • Lower values of modulus (shallow gradients of
    slope in stress-strain curve) relates to a more
    ductile material.
  • e.g. (GPa)
  • Teflon 0.5 Bone 10-20
  • Concrete 30
  • Copper 120
  • Diamond 1100

Spider silk
16
Now back to diffraction
  • X-ray diffraction patterns can give us some
    information on strain
  • Remember..

Scherrer formula where k0.9
17
(micro) Strain uniform
  • Uniform strain causes the lattice to
    expand/contract isotropically
  • Thus unit cell parameters expand/contract
  • Peak positions shift

18
(micro) Strain non-uniform
  • Leads to systematic shift of atoms
  • Results in peak-broadening
  • Can arise from
  • point defects (later)
  • poor crystallinity
  • plastic deformation

19
Williamson-Hall plots
  • Take the Scherrer equation and the strain effect

So if we plot Bcos? against 4sin ? we (should)
get a straight line with gradient ? and intercept
0.9?/t
20
A Williamson-Hall plot (figure 2) indicates that
the cause of the broadening is strain, and most
of this will be the result of chemical disorder
the mean particle size is 4 pm, leading to
insignificant size broadening. . The increase in
slope with decreasing temperature clearly
indicates an increase in the rhombohedral
distortion with falling temperature.
C N W Darlington and R J Cernik J. Phys.
Condens. Matter 1 (1989) 6019-6023.
21
Example
  • 0.138 0.9?/t
  • gradient ?

22
Crystallite size
Halfwidth as before
Can give misleading results
23
Crystallite size
Integral breadth
24
Summary
  • External forces affect the underlying crystal
    structure
  • Strained materials show broadened diffraction
    peaks
  • Width of peaks can be resolved into components
    due to particle size and strain
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