Mechanical Properties of Metals
➢ TYPES OF LOADING
Deformation occurs when forces are applied to a material. There are three principal ways in which a load may be applied: tension,
compression and shear.
==> Tension
Load: As the ends of material are pulled apart to make the
material longer, the load is called a tension load.
==> Compression
Load: As the ends of material are pushed in to make the
material shorter, the load is called a compression load.
==> Shear
Load: The load imposed parallel to the upper and lower faces.
Torsion is a variation of pure shear, wherein a structural member is twisted.
Torsional forces produce a rotational motion about the longitudinal axis of
one end of the member relative to the other end.
Tensile load
produces an elongation and compressive load
produces contraction.
==> Strain : Amount of deformation per unit length. Strain is the response of materials to stress, since strain is the ratio of two
lengths, it is dimensionless
. Strain can be negative for compressive loads.
➢ MODULUS OF ELASTICITY
Deformation in which stress and strain are
proportional is called elastic deformation. The constant of proportionality E is the modulus of elasticity or Young’s Modulus. The slope of linear region of stress-strain curve corresponds to the modulus of elasticity. The modulus of elasticity is stiffness or materials resistance to elastic deformation. The greater the modulus, the stiffer the material (or smaller the elastic strain produced applied load).
➢ SHEAR MODULUS
Shear stress and shear strain are proportional each other. The constant of proportionality G is the shear modulus. G = Shear Stress / Shear Strain
Poission’s
ratio is defined as the ratio of the lateral
and axial strains. For the isotropic materials the shear and elastic moduli are related to each other and to Paisson's ratio. Poisson’s ratio ranges between 0.25 to 0.35.
Elastic deformation (Reversible):
Stress removed ==> material returns to original shape
Plastic deformation (Irreversible):
Stress removed ==> material does not return to original dimensions.
➢ TENSILE TEST
The applied stress versus the strain
or elongation of the specimen
shows the initial elastic response of
the material, followed by yielding,
plastic deformation and finally
necking and failure. Several
measurements are taken from the
plot, called the Engineering
Stress-Strain Diagram.
These
include:
==> Modulus of elasticity
==> Yield strength
==> Tensile strength
==> Modulus of resilience
==> Failure stress
==> Ductility
==> Toughness
Sometimes yield strength may not be determined exactly. In this case, to determine
yield strength, straight line is
drawn parallel to the elastic
portion of stress-strain curve
at strain of 0.002 point. The stress corresponding
to the intersection of this
line and the stress-strain
curve is the yield strength.
➢ DUCTILITY
Ductile materials experience plastic
deformation. Material that experiences very little or no
plastic deformation upon fracture is termed
brittle. If the strain 5%, the material is brittle. Ductility
percent
may be expressed as either
elongation
reduction
in area.
➢ RESILIENCE
Resilience is the capacity of a material
to absorb energy when it is deformed
elastically and then, upon unloading, to
have this energy recovered. The
associated property is the modulus of
resilience, Ur, which is the strain energy
per unit volume required to stress a
material from an unloaded state up to the
point of yielding. Ur is the area
under the
stress-strain curve taken to
yielding. Resilient materials are those having high yield strengths and low moduli of elasticity.
➢ TOUGHNESS
Toughness
is
energy up
absorbed
to fracture. It is the area under the
stress-strain curve up to the
point of fracture. For a material to be tough, it
must display both strength
and ductility. Often, ductile materials are tougher than brittle ones.
➢ TRUE
STRESS-TRUE STRAIN CURVE
The engineering stress is on the basis of the original cross-sectional area before any deformation, and does not take into account the reduction in area at the neck.
➢ COMPRESSION TEST
A compression test is conducted in a manner similar to the tensile test except that the force is compressive and the specimen contracts along the direction of the stress.
Brittle materials ==> Tensile test are more common. Compression tests are
used when the material is brittle in tension. Brittle materials such as cast irons usually reach much
higher ultimate stresses in compression than intension. The brittle fracture is performed by separation and is
not accompanied by noticeable plastic deformation.
Ductile materials ==> The ductile materials such as steel, Al, and Cu
have stress–strain diagrams similar to one swhich for
tensile test. When a small specimen of the ductile material is
compressed, it begins to bulge on sides and
becomes barrel shaped as shown in the figure
above. With increasing load, the specimen is flattened out,
thus offering increased resistance to further
shortening (which means that the stress–strains
curve goes upward) this effect is indicated in the
diagram.
➢ HARDNESS
Hardness is a measure of material’s resistance to localized plastic deformation. Hardness tests are simple, cheap, nondestructive.
Hardness Techniques
==> Brinell Hardness Test
==> Vickers Hardness Test
==> Knoop and Vickers Microhardness Tests
➢ FRACTURE
Separation of a material into two or
more pieces in response to imposed stress. For engineering materials, two fracture modes
are possible: ductile and brittle.
==> Ductile materials: Extensive plastic deformation
with high energy absorption (toughness) before
fracture.
==> Brittle materials: Little plastic deformation with
low energy absorption before fracture.
➢ IMPACT TESTING
Impact testing was commonly used to assess fracture characteristics of materials.
Impact Parameters
==> Test Temperature
==> Specimen Geometry
==> Crack or Notch length
==> Impact Energy
Ductile to Brittle Transition
For many materials, the impact energy is
correlated with the toughness determined in
a tensile test . However, as temperature drops,
some materials show a transition from ductile
to brittle behavior. Impact test determine whether or not a
material experiences a ductile to brittle
transition with decreasing temperature. Temperature at which a material changes
from ductile to brittle failure is called
transition temperature. Transition temperature is usually taken as
the point where 50% of the fracture is brittle.
Transition Temperature
Materials must be used above
their ductile to brittle transition
temperatures
to avoid brittle failure. Increasing the carbon content of the steels raises the transition temperature. Grain size reduction decreases the
transitiontemperatureofsteels.
➢ FATIGUE
In many applications, materials are subjected to vibrating
or oscillating
forces. The behavior of materials under such load conditions differs from
the behavior under a static load. The material is subjected to repeated load cycles in actual use. Fatigue
is a form of failure that occurs in structures subjected to
dynamic
and fluctuating stresses. Fatigue failure occurs at a stress
level lower than tensile and yield
strength
for a static load. It is estimated that 90% of all material failure is due to fatigue. Polymers and ceramics are also susceptible to this
type of failure. Fatigue is catastrophic, occurring
without
warning.
CYCLIC STRESSES
==> Reversed stress cycle
==> Repeated stress cycle
==> Randomstresscycle
➢ FATIGUE TEST
The applied stress maybe axial (tension-compression), flexural (bending), or torsinal
(twisting) in nature. Data are plotted as stress(S) versus logarithm of the number
(N) of cycles to failure for each of the specimens.
S-N Curve
There are two general types of S-N curve.
Fatigue Limit (endurance limit) ==> Ferrous and Ti alloys
Fatigue strength ==> Non-ferrous alloys
Another important parameter is fatigue
life.
Factors That Affect Fatigue Life
==> Magnitude
of stress: Increasing
in
fatigue life.
==> Environmental effects: If a corrosive environment is present during the
cyclic stress of a metal, the chemical attack greatly accelerates the rate at
which fatigue cracks propagate.
The combination of corrosion attack and
cyclic stresses on a metal is known as corrosion
fatigue. Solutions for corrosion fatigue
:
==> decrease corrosiveness of medium
==> add protective surface coating
==> Surface
Effects: Most cracks leading to fatigue failure originate at surface
positions. Therefore, fatigue life is sensitive to surface conditions. Surface
factors include;
==> Design Factors
==> Surface treatments
➢ CREEP
Materials are often placed in service at
elevated temperatures
and exposed
to static mechanical stresses. Deformation under
such circumstances is termed creep. Creep is the
load
time-dependent deformation due to constant
at high temperature (> 0.4 Tm). A specimen is subjected to a constant load while maintaining
the temperature constant; deformation or strain is measured
and plotted as a function of elapsed time. Creep specimens have the same
geometry as for tensile tests.
CREEP PARAMETERS
==> Secondary/ steady-state creep rate
==> Rupture lifetime
With increasing stress or temperature:
==> The instantaneous strain increases
==> The steady-state creep rate increases
==> The time to rupture decreases
➢ TORSION TEST
Torsion
test is not widely used as
much as tensile test. Because
it is not
possible to generate a uniform shear
stress; when
the surface plastic, the
interior
is still elastic because shear stress
on
surface is larger than the interior. Torsion
test is made to determine
such properties as the shear modulus
elasticity
,
shear
of
strain, and shear
strength.
Often used for testing brittle materials
and can
be tested in full sized parts such
as
shafts, axles and twist drills which are
subjected to torsional loading in use. A twisting
moment is applied to one end of a specimen while measuring the deformation
as angular
displacement at the other end. During the test the angle
of twist and the applied torque
test proceeds.
Shear stress-shear strain in torsion;
==> Using the appropriate formulae
, relationships
and the measured
dimensions, we can
determine the shear stress and shear strain on the specimen.
==> Then, one can plot the torque
vs. angle of twist, and shear
which one can find the material properties previously mentioned.
==> The
stress vs. shear strain from
twisting moment is resisted by shear stresses set up in the cross section of the bar
(zero
at the center, maximum at the surface).
Elastic properties and yield strength
in torsion;
==> The elastic
properties in torsion
can be obtained by using the torque at
the proportional
limit where the shear
stress is calculated corresponding to
the twisting moment from the shear
stress equation.
==> The torsional
elastic limit or yield
strength
can be obtained from testing a tubular specimen since the stress gradient are practically eliminated.
Types of torsion failures;
Torsion failures are different from tensile failure in that there is little localised reduction of area or elongation.
Torsion failures are different from tensile failure in that there is little localised reduction of area or elongation.
==> Ductile (shear) failure is along the maximum shear plane (perpendicular to
longitudinal axis of the specimen).
==> Brittle (tensile) failure is perpendicular to the maximum tensile stress (at 45°),
resulting in a helical fracture.
➢ BEND TEST for brittle materials
In many brittle materials, the normal tensile test cannot easily be performed because of the presence of flaws at the surface. Often, just placing a brittle material in the grips of the tensile testing machine causes cracking. These materials maybe tested using the bend test.
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.
➢ BEND TEST
Flexural strength or modulus of rupture: The stress required to fracture a
specimen in a bend test. Flexural modulus: The modulus of
elasticity in bending calculated from the results
of a bend test, giving the slope of the stress
deflection curve.
The Science and Engineering of Materials, D.R. Askeland
Materials Science and Engineering: An Introduction, W.D. Callister, 8th ed., John Wiley, 2007