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Chapter 7: MECHANICAL PROPERTIES * * c07f05 Linear Elastic

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Title: Chapter 7: MECHANICAL PROPERTIES * * c07f05 Linear Elastic


1
Chapter 7
  • MECHANICAL PROPERTIES

2
Chapter Outline
  • Terminology for Mechanical Properties
  • The Tensile Test Stress-Strain Diagram
  • Properties Obtained from a Tensile Test
  • True Stress and True Strain
  • The Bend Test for Brittle Materials
  • Hardness of Materials

3
Questions to Think About
  • Stress and strain What are they and why are
    they used instead of load and deformation?
  • Elastic behavior When loads are small, how much
    deformation occurs? What materials deform least?
  • Plastic behavior At what point do dislocations
    cause permanent deformation? What materials
    are most resistant to permanent deformation?
  • Toughness and ductility What are they and how
    do we measure them?
  • Ceramic Materials What special provisions/tests
    are made for ceramic materials?

4
Stress-Strain Test
  • specimen
  • machine

5
Tensile Test
6
Important Mechanical Properties from a Tensile
Test
  • Young's Modulus This is the slope of the linear
    portion of the stress-strain curve, it is usually
    specific to each material a constant, known
    value.
  • Yield Strength This is the value of stress at
    the yield point, calculated by plotting young's
    modulus at a specified percent of offset (usually
    offset 0.2).
  • Ultimate Tensile Strength This is the highest
    value of stress on the stress-strain curve.
  • Percent Elongation This is the change in gauge
    length divided by the original gauge length.

7
Terminology
  • Load - The force applied to a material during
    testing.
  • Strain gage or Extensometer - A device used for
    measuring change in length (strain).
  • Engineering stress - The applied load, or force,
    divided by the original cross-sectional area of
    the material.
  • Engineering strain - The amount that a material
    deforms per unit length in a tensile test.

8
Elastic Deformation
1. Initial
2. Small load
3. Unload
Elastic means reversible.
9
Plastic Deformation (Metals)
1. Initial
2. Small load
3. Unload
Plastic means permanent.
10
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Typical stress-strain behavior for a metal
showing elastic and plastic deformations, the
proportional limit P and the yield strength sy,
as determined using the 0.002 strain offset
method (where there is noticeable plastic
deformation). P is the gradual elastic to plastic
transition.
11
Plastic Deformation (permanent)
  • From an atomic perspective, plastic deformation
    corresponds to the breaking of bonds with
    original atom neighbors and then reforming bonds
    with new neighbors.
  • After removal of the stress, the large number of
    atoms that have relocated, do not return to
    original position.
  • Yield strength is a measure of resistance to
    plastic deformation.

12
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13
  • Localized deformation of a ductile material
    during a tensile test produces a necked region.
  • The image shows necked region in a fractured
    sample

14
Permanent Deformation
  • Permanent deformation for metals is accomplished
    by means of a process called slip, which involves
    the motion of dislocations.
  • Most structures are designed to ensure that only
    elastic deformation results when stress is
    applied.
  • A structure that has plastically deformed, or
    experienced a permanent change in shape, may not
    be capable of functioning as intended.

15
Yield Strength, sy
16

Stress-Strain Diagram
ultimate tensile strength
3
necking
Strain Hardening
SlopeE
Fracture
yield strength
5
2
Elastic region slope Youngs (elastic)
modulus yield strength Plastic region
ultimate tensile strength strain hardening
fracture
Plastic Region
Stress (F/A)
Elastic Region
4
1
Strain ( ) (DL/Lo)
17

Stress-Strain Diagram (cont)
  • Elastic Region (Point 1 2)
  • - The material will return to its original
    shape
  • after the material is unloaded( like a
    rubber band).
  • - The stress is linearly proportional to the
    strain in
  • this region.

or
Stress(psi) E Elastic modulus (Youngs
Modulus) (psi) Strain (in/in)
  • Point 2 Yield Strength a point where
    permanent
  • deformation occurs. ( If it is passed, the
    material will
  • no longer return to its original length.)

18

Stress-Strain Diagram (cont)
  • Strain Hardening
  • - If the material is loaded again from Point
    4, the
  • curve will follow back to Point 3 with the
    same
  • Elastic Modulus (slope).
  • - The material now has a higher yield
    strength of
  • Point 4.
  • - Raising the yield strength by permanently
    straining
  • the material is called Strain Hardening.

19


Stress-Strain Diagram (cont)
  • Tensile Strength (Point 3)
  • - The largest value of stress on the diagram
    is called
  • Tensile Strength(TS) or Ultimate Tensile
    Strength
  • (UTS)
  • - It is the maximum stress which the material
    can
  • support without breaking.
  • Fracture (Point 5)
  • - If the material is stretched beyond Point 3,
    the stress
  • decreases as necking and non-uniform
    deformation
  • occur.
  • - Fracture will finally occur at Point 5.

20
The stress-strain curve for an aluminum alloy.
21
  • Stress-strain behavior found for some steels with
    yield point phenomenon.

22
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T E N S I L E P R O P E R T I E S
23
Yield Strength Comparison
Room T values
a annealed hr hot rolled ag aged cd
cold drawn cw cold worked qt quenched
tempered
24
Tensile Strength, TS
  • After yielding, the stress necessary to continue
    plastic deformation in metals increases to a
    maximum point (M) and then decreases to the
    eventual fracture point (F).
  • All deformation up to the maximum stress is
    uniform throughout the tensile sample.
  • However, at max stress, a small constriction or
    neck begins to form.
  • Subsequent deformation will be confined to this
    neck area.
  • Fracture strength corresponds to the stress at
    fracture.
  • Region between M and F
  • Metals occurs when noticeable necking starts.
  • Ceramics occurs when crack propagation
    starts.
  • Polymers occurs when polymer backbones are
    aligned and about to break.

25
  • In an undeformed thermoplastic polymer tensile
    sample,
  • the polymer chains are randomly oriented.
  • When a stress is applied, a neck develops as
    chains become aligned locally. The neck
    continues to grow until the chains in the entire
    gage length have aligned.
  • The strength of the polymer is increased

26
Tensile Strength Comparison
Room T values
Based on data in Table B4, Callister 6e. a
annealed hr hot rolled ag aged cd cold
drawn cw cold worked qt quenched
tempered AFRE, GFRE, CFRE aramid, glass,
carbon fiber-reinforced epoxy composites, with 60
vol fibers.
27
Engineering Stress
Tensile stress, s
Shear stress, t
Stress has units N/m2 or lb/in2
27
28
VMSE
  • http//www.wiley.com/college/callister/0470125373/
    vmse/index.htm
  • http//www.wiley.com/college/callister/0470125373/
    vmse/strstr.htm

29
Example 1 Tensile Testing of Aluminum Alloy
Convert the change in length data in the table to
engineering stress and strain and plot a
stress-strain curve.
30
Example 1 SOLUTION
31
Ductility, EL
Ductility is a measure of the plastic deformation
that has been sustained at fracture
A material that suffers very little plastic
deformation is brittle.
Another ductility measure
  • Ductility may be expressed as either percent
    elongation ( plastic strain at fracture) or
    percent reduction in area.
  • AR gt EL is possible if internal voids form in
    neck.

32
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Toughness
Toughness is the ability to absorb energy up to
fracture (energy per unit volume of material).
A tough material has strength and
ductility. Approximated by the area under the
stress-strain curve.
Lower toughness ceramics
Higher toughness metals
33
Toughness
Energy to break a unit volume of material
Approximate by the area under the stress-strain
curve.
21
34
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Linear Elastic Properties
s E e
Hooke's Law
n ex/ey
Poisson's ratio metals n 0.33
ceramics n 0.25 polymers n 0.40
Modulus of Elasticity, E (Young's modulus)
Units E GPa or psi n dimensionless
35
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Engineering Strain
Strain is dimensionless.
35
36
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Axial (z) elongation (positive strain) and
lateral (x and y) contractions (negative strains)
in response to an imposed tensile stress.
36
37
True Stress and True Strain
  • True stress The load divided by the actual
    cross-sectional area of the specimen at that
    load.
  • True strain The strain calculated using actual
    and not original dimensions, given by et ln(l/l0).
  • The relation between the true stress-true strain
    diagram and engineering stress-engineering strain
    diagram.
  • The curves are identical to the yield point.

38
Stress-Strain Results for Steel Sample
39
Example 2 Youngs
Modulus - Aluminum Alloy
From the data in Example 1, calculate the modulus
of elasticity of the aluminum alloy.
40
Example 2 Youngs Modulus - Aluminum Alloy -
continued
  • Use the modulus to determine the length after
    deformation of a bar of initial length of 50 in.
  • Assume that a level of stress of 30,000 psi is
    applied.

41
Youngs Moduli Comparison
Graphite Ceramics Semicond
Metals Alloys
Composites /fibers
Polymers
E(GPa)
Composite data based on reinforced epoxy with 60
vol of aligned carbon (CFRE), aramid (AFRE), or
glass (GFRE) fibers.
42
Example 3 True Stress and True Strain Calculation
Compare engineering stress and strain with true
stress and strain for the aluminum alloy in
Example 1 at (a) the maximum load. The diameter
at maximum load is 0.497 in. and at fracture is
0.398 in. Example 3 SOLUTION
43
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Strain Hardening
An increase in sy due to plastic deformation.
44
Strain Hardening (n, K or C values)
45
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46
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47
Mechanical Behavior - Ceramics
  • The stress-strain behavior of brittle ceramics is
    not usually obtained by a tensile test.
  • It is difficult to prepare and test specimens
    with specific geometry.
  • It is difficult to grip brittle materials without
    fracturing them.
  • Ceramics fail after roughly 0.1 strain specimen
    have to be perfectly aligned.

48
The Bend Test for Brittle Materials
  • Bend test - Application of a force to the center
    of a bar that is supported on each end to
    determine the resistance of the material to a
    static or slowly applied load.
  • Flexural strength or modulus of rupture -The
    stress required to fracture a specimen in a bend
    test.
  • Flexural modulus - The modulus of elasticity
    calculated from the results of a bend test,
    giving the slope of the stress-deflection curve.

49
The stress-strain behavior of brittle materials
compared with that of more ductile materials
50
(a) The bend test often used for measuring the
strength of brittle materials, and (b) the
deflection d obtained by bending
51
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Flexural Strength
  • Schematic for a 3-point bending test.
  • Able to measure the stress-strain behavior and
    flexural strength of brittle ceramics.
  • Flexural strength (modulus of rupture or bend
    strength) is the stress at fracture.

See Table 7.2 for more values.
52
MEASURING ELASTIC MODULUS
Room T behavior is usually elastic, with
brittle failure. 3-Point Bend Testing often
used. --tensile tests are difficult for
brittle materials.
Determine elastic modulus according to
23
53
MEASURING STRENGTH
3-point bend test to measure room T strength.
Typ. values
Flexural strength
Si nitride Si carbide Al oxide glass (soda)
700-1000 550-860 275-550 69
300 430 390 69
Data from Table 12.5, Callister 6e.
24
54
Stress-Strain Behavior Elastomers
  • 3 different responses
  • A brittle failure
  • B plastic failure
  • C - highly elastic (elastomer)

--brittle response (aligned chain, cross
linked networked case) --plastic response
(semi-crystalline case)
55
Hardness of Materials
  • Hardness test - Measures the resistance of a
    material to penetration by a sharp object.
  • Macrohardness - Overall bulk hardness of
    materials measured using loads gt2 N.
  • Microhardness Hardness of materials typically
    measured using loads less than 2 N using such
    test as Knoop (HK).
  • Nano-hardness - Hardness of materials measured at
    110 nm length scale using extremely small (100
    µN) forces.

56
Hardness
  • Hardness is a measure of a materials resistance
    to localized plastic deformation (a small dent or
    scratch).
  • Quantitative hardness techniques have been
    developed where a small indenter is forced into
    the surface of a material.
  • The depth or size of the indentation is measured,
    and corresponds to a hardness number.
  • The softer the material, the larger and deeper
    the indentation (and lower hardness number).

57
Hardness
Resistance to permanently indenting the
surface. Large hardness means
--resistance to plastic deformation or cracking
in compression. --better wear
properties.
Adapted from Fig. 6.18, Callister 6e. (Fig. 6.18
is adapted from G.F. Kinney, Engineering
Properties and Applications of Plastics, p. 202,
John Wiley and Sons, 1957.)
58
Hardness Testers
59
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60
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Conversion of Hardness Scales
Also see ASTM E140 - 07 Volume 03.01 Standard
Hardness Conversion Tables for Metals
Relationship Among Brinell Hardness, Vickers
Hardness, Rockwell Hardness, Superficial
Hardness, Knoop Hardness, and Scleroscope Hardness
61
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Correlation between Hardness and Tensile Strength
  • Both hardness and tensile strength are indicators
    of a metals resistance to plastic deformation.
  • For cast iron, steel and brass, the two are
    roughly proportional.
  • Tensile strength (psi) 500BHR

62
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63
Summary
Stress and strain These are
size-independent measures of load and
displacement, respectively.
Elastic behavior This reversible behavior
often shows a linear relation between
stress and strain. To minimize deformation,
select a material with a large elastic
modulus (E or G).
Plastic behavior This permanent deformation
behavior occurs when the tensile (or
compressive) uniaxial stress reaches sy.
Toughness The energy needed to break a unit
volume of material.
Ductility The plastic strain at failure.
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