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8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 121
1
30 July 2007 1
CHAPTER5
PROPERTIES OF MATERIALS ndashPART 1
30 July 2007 2
OUTLINE
31 Mechanical Properties
311 Definition
312 Factors AffectingMechanical Properties
313 Kinds of MechanicalProperties
314 Stress and Strain
315 Elastic Deformation
316 Plastic Deformationamp Plasticity
317 Strength
318 BrittlenessToughness Resilience ampDuctility
319 Fatigue
3110 Creep andShrinkage Design andSafety Factors
32 Electrical Properties
33 Optical Properties
34 Magnetic Properties
35 Thermal Properties
36 Corrosion Properties
8122019 CH5 -Mechanical Properties of Matpdf
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30 July 2007 3
31 MECHANICAL PROPERTIES
311 DEFINITIONProperties or deformationobserved when a material issubjected
to an applied external force(F = ma)
to a mechanical force ofstretching compressingbending strikingare calledthe mechanical properties
eg Mechanical properties of airplane
wing made of aluminum alloy
Mechanical properties of a bridge made of steel
30 July 2007 4
312 FACTORS AFFECTING THE
MECHANICAL PROPERTIES
Nature of the applied load eg Tensilecompressive shear
Magnitude of the applied force
The duration (application time) may beless than a second may extend over aperiod of many years
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 3213
30 July 2007 5
313 KINDS OF MECHANICAL
PROPERTIESElasticity
he ability of a material to deform under load and return to its original size and shape when the
load is removed
Stiffness
the slope of the linear segment of stress ndash strain curve is Elastic Modulus or Youngrsquos Modulus
The value of the Modulus is the measure of STIFFNESS materialrsquos resistance to elastic
deformation (MPa)
Plasticity the property of a material to deform permanently under the application of a load
Yield Strength the stress level at which the plastic deformation begins (MPa)
Tensile Strengththe stress at the maximum on the engineering stress-strain curvethe ability of a material to
withstand tensile loads without rupture when the material is in tension (MPa)
Compressive Strengththe ability of a material to withstand compressive (squeezing) loads without being crushed
when the material is in compression (MPa)
Fracture Strength corresponds to the stress at fracture (MPa)
30 July 2007 6
313 KINDS OF MECHANICAL
PROPERTIES
Toughness the ability of a material to withstand shatter A material which easily shatters is brittle The ability of a
material to absorb energy (Jm3)
ResilienceThe capacity of material to absorb energy when it is deformed elastically and then upon unloading to
have this energy recovered (Jm3)
Ductilitythe ability of a material to stretch under the application of tensile load and retain the deformed shape on the
removal of the load Measure of ability to deform plastically without fracture (no units or mm)
Brittleness brittle materials approximately have a fracture strain of less than about 5
Malleabilityhe property of a material to deform permanently under the application of a compressive load A material
which is forged to its final shape is required to be malleable
Fatigue
Strengththe property of a material to withstand continuously varying and alternating loads
Hardnesshe property of a material to withstand indentation and surface abrasion by another hard object It is an
indication of the wear resistance of a material
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 4214
30 July 2007 7
314 STRESS amp STRAIN
Tension Compression Shear Torsion
Reference Callister Material Science and Eng 5th Ed p114
Types of force(load) applied on the object
30 July 2007 8
3141 ENGINEERING STRESS (σ)
(Gerilme)
Stress is defined as force F applied over the original cross-sectional area Ao
For a tensile test the stress is given by
Stress (MPa or psi)
Where F = applied tensile force (N or lbs) A0= original cross-sectional area of the test specimen (m2 or in2)
Units for Engineering Stress US customary pounds per square inch (psi) SI N m-2 = Pascal (Pa) 1psi = 689 x 10 3 Pa
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 5215
30 July 2007 9
3141 ENGINEERING STRESS (σ)
(Gerilme)
Example A 125 cm diameter bar is subjected to a load of2500 kg Calculate the engineering stress on the bar inmegapascal (MPa)
Solrsquon F= ma = 2500 x 981 = 24 500 N
Ao = π r 2 = π ( 00125 2 4 )
σ = Ft Ao = 2 x 10 8 Pa = 200 MPa
30 July 2007 10
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
When an unaxial tensile force is applied to a rod it causesthe rod to be elongated in the direction of the force
Engineering strain is the ratio of the change in the length ofthe sample in the direction of the force divided by the originallength
ε = ( l ndash lo ) lo = ∆ l lo Where ∆l = l - lo is the change in length l0 = original length of the specimen In engineering practice it is common to convert engineering
strain into percent strain or percent elongation engineering strain = engineering strain x 100 =
elongation Unit of engineering strain Inch inch or mm which is dimensionless
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 6216
30 July 2007 11
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
L
Engineeringstress
Engineering(normal) strain
==
== A
F
δ ε
σ
A
F
L
A
F
δ ε
σ
=
==2
2
LL
A
F
δ δ ε
σ
==
=
2
2
30 July 2007 12
3143 STRESS ndash STRAIN TESTING
Tension tests they are common since they are easier toperform for most structural materials steel etc
Compression tests are used when a materialrsquos under largeand permanent strains is desired or when the material is
brittle in tension concrete Shear and torsion tests Torsion test are performed on
cylindrical solid shafts or tubes machine axles and driveshafts
Typical tensile Specimen
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 7217
30 July 2007 13
3143 STRESS ndash STRAIN TESTINGHydraulic
Wedge
Grips
SpecimenExtensometer
Schematic representation of the apparatusused to conduct tensile stress - strain tests
Typical tensile test machine
30 July 2007 14
3144 YOUNGS MODULUS (E)
During ElasticDeformation Stress Strain = a constant
σ ε= E =Modulus ofelasticity (YoungrsquosModulus) (ElastisiteModuumlluuml) (MPa)
Modulus of Elasticitygives an idea aboutmaterialrsquos resistanceto elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 8218
30 July 2007 15
STIFFNESSMaterialrsquos resistance to
Elastic Deformation
Atomic Origin of Stiffness
Strongly Bonded
Weakly Bonded
N e t I n t e r a t o m i c F o r c e
Interatomic Distance
E prop dF
dr
r o
The value of the Modulus of Elasticity isthe measure of STIFFNESS
30 July 2007 16
Metal Alloy Modulus of Elasticity
E ( GPa)
Aluminum
Brass
Copper
Magnesium
Nickel
Steel
Titanium
Tungsten
69
97
110
45
207
207
107
407
3144 YOUNGS MODULUS (E)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2212
30 July 2007 3
31 MECHANICAL PROPERTIES
311 DEFINITIONProperties or deformationobserved when a material issubjected
to an applied external force(F = ma)
to a mechanical force ofstretching compressingbending strikingare calledthe mechanical properties
eg Mechanical properties of airplane
wing made of aluminum alloy
Mechanical properties of a bridge made of steel
30 July 2007 4
312 FACTORS AFFECTING THE
MECHANICAL PROPERTIES
Nature of the applied load eg Tensilecompressive shear
Magnitude of the applied force
The duration (application time) may beless than a second may extend over aperiod of many years
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 3213
30 July 2007 5
313 KINDS OF MECHANICAL
PROPERTIESElasticity
he ability of a material to deform under load and return to its original size and shape when the
load is removed
Stiffness
the slope of the linear segment of stress ndash strain curve is Elastic Modulus or Youngrsquos Modulus
The value of the Modulus is the measure of STIFFNESS materialrsquos resistance to elastic
deformation (MPa)
Plasticity the property of a material to deform permanently under the application of a load
Yield Strength the stress level at which the plastic deformation begins (MPa)
Tensile Strengththe stress at the maximum on the engineering stress-strain curvethe ability of a material to
withstand tensile loads without rupture when the material is in tension (MPa)
Compressive Strengththe ability of a material to withstand compressive (squeezing) loads without being crushed
when the material is in compression (MPa)
Fracture Strength corresponds to the stress at fracture (MPa)
30 July 2007 6
313 KINDS OF MECHANICAL
PROPERTIES
Toughness the ability of a material to withstand shatter A material which easily shatters is brittle The ability of a
material to absorb energy (Jm3)
ResilienceThe capacity of material to absorb energy when it is deformed elastically and then upon unloading to
have this energy recovered (Jm3)
Ductilitythe ability of a material to stretch under the application of tensile load and retain the deformed shape on the
removal of the load Measure of ability to deform plastically without fracture (no units or mm)
Brittleness brittle materials approximately have a fracture strain of less than about 5
Malleabilityhe property of a material to deform permanently under the application of a compressive load A material
which is forged to its final shape is required to be malleable
Fatigue
Strengththe property of a material to withstand continuously varying and alternating loads
Hardnesshe property of a material to withstand indentation and surface abrasion by another hard object It is an
indication of the wear resistance of a material
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 4214
30 July 2007 7
314 STRESS amp STRAIN
Tension Compression Shear Torsion
Reference Callister Material Science and Eng 5th Ed p114
Types of force(load) applied on the object
30 July 2007 8
3141 ENGINEERING STRESS (σ)
(Gerilme)
Stress is defined as force F applied over the original cross-sectional area Ao
For a tensile test the stress is given by
Stress (MPa or psi)
Where F = applied tensile force (N or lbs) A0= original cross-sectional area of the test specimen (m2 or in2)
Units for Engineering Stress US customary pounds per square inch (psi) SI N m-2 = Pascal (Pa) 1psi = 689 x 10 3 Pa
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 5215
30 July 2007 9
3141 ENGINEERING STRESS (σ)
(Gerilme)
Example A 125 cm diameter bar is subjected to a load of2500 kg Calculate the engineering stress on the bar inmegapascal (MPa)
Solrsquon F= ma = 2500 x 981 = 24 500 N
Ao = π r 2 = π ( 00125 2 4 )
σ = Ft Ao = 2 x 10 8 Pa = 200 MPa
30 July 2007 10
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
When an unaxial tensile force is applied to a rod it causesthe rod to be elongated in the direction of the force
Engineering strain is the ratio of the change in the length ofthe sample in the direction of the force divided by the originallength
ε = ( l ndash lo ) lo = ∆ l lo Where ∆l = l - lo is the change in length l0 = original length of the specimen In engineering practice it is common to convert engineering
strain into percent strain or percent elongation engineering strain = engineering strain x 100 =
elongation Unit of engineering strain Inch inch or mm which is dimensionless
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 6216
30 July 2007 11
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
L
Engineeringstress
Engineering(normal) strain
==
== A
F
δ ε
σ
A
F
L
A
F
δ ε
σ
=
==2
2
LL
A
F
δ δ ε
σ
==
=
2
2
30 July 2007 12
3143 STRESS ndash STRAIN TESTING
Tension tests they are common since they are easier toperform for most structural materials steel etc
Compression tests are used when a materialrsquos under largeand permanent strains is desired or when the material is
brittle in tension concrete Shear and torsion tests Torsion test are performed on
cylindrical solid shafts or tubes machine axles and driveshafts
Typical tensile Specimen
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 7217
30 July 2007 13
3143 STRESS ndash STRAIN TESTINGHydraulic
Wedge
Grips
SpecimenExtensometer
Schematic representation of the apparatusused to conduct tensile stress - strain tests
Typical tensile test machine
30 July 2007 14
3144 YOUNGS MODULUS (E)
During ElasticDeformation Stress Strain = a constant
σ ε= E =Modulus ofelasticity (YoungrsquosModulus) (ElastisiteModuumlluuml) (MPa)
Modulus of Elasticitygives an idea aboutmaterialrsquos resistanceto elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 8218
30 July 2007 15
STIFFNESSMaterialrsquos resistance to
Elastic Deformation
Atomic Origin of Stiffness
Strongly Bonded
Weakly Bonded
N e t I n t e r a t o m i c F o r c e
Interatomic Distance
E prop dF
dr
r o
The value of the Modulus of Elasticity isthe measure of STIFFNESS
30 July 2007 16
Metal Alloy Modulus of Elasticity
E ( GPa)
Aluminum
Brass
Copper
Magnesium
Nickel
Steel
Titanium
Tungsten
69
97
110
45
207
207
107
407
3144 YOUNGS MODULUS (E)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 3213
30 July 2007 5
313 KINDS OF MECHANICAL
PROPERTIESElasticity
he ability of a material to deform under load and return to its original size and shape when the
load is removed
Stiffness
the slope of the linear segment of stress ndash strain curve is Elastic Modulus or Youngrsquos Modulus
The value of the Modulus is the measure of STIFFNESS materialrsquos resistance to elastic
deformation (MPa)
Plasticity the property of a material to deform permanently under the application of a load
Yield Strength the stress level at which the plastic deformation begins (MPa)
Tensile Strengththe stress at the maximum on the engineering stress-strain curvethe ability of a material to
withstand tensile loads without rupture when the material is in tension (MPa)
Compressive Strengththe ability of a material to withstand compressive (squeezing) loads without being crushed
when the material is in compression (MPa)
Fracture Strength corresponds to the stress at fracture (MPa)
30 July 2007 6
313 KINDS OF MECHANICAL
PROPERTIES
Toughness the ability of a material to withstand shatter A material which easily shatters is brittle The ability of a
material to absorb energy (Jm3)
ResilienceThe capacity of material to absorb energy when it is deformed elastically and then upon unloading to
have this energy recovered (Jm3)
Ductilitythe ability of a material to stretch under the application of tensile load and retain the deformed shape on the
removal of the load Measure of ability to deform plastically without fracture (no units or mm)
Brittleness brittle materials approximately have a fracture strain of less than about 5
Malleabilityhe property of a material to deform permanently under the application of a compressive load A material
which is forged to its final shape is required to be malleable
Fatigue
Strengththe property of a material to withstand continuously varying and alternating loads
Hardnesshe property of a material to withstand indentation and surface abrasion by another hard object It is an
indication of the wear resistance of a material
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 4214
30 July 2007 7
314 STRESS amp STRAIN
Tension Compression Shear Torsion
Reference Callister Material Science and Eng 5th Ed p114
Types of force(load) applied on the object
30 July 2007 8
3141 ENGINEERING STRESS (σ)
(Gerilme)
Stress is defined as force F applied over the original cross-sectional area Ao
For a tensile test the stress is given by
Stress (MPa or psi)
Where F = applied tensile force (N or lbs) A0= original cross-sectional area of the test specimen (m2 or in2)
Units for Engineering Stress US customary pounds per square inch (psi) SI N m-2 = Pascal (Pa) 1psi = 689 x 10 3 Pa
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 5215
30 July 2007 9
3141 ENGINEERING STRESS (σ)
(Gerilme)
Example A 125 cm diameter bar is subjected to a load of2500 kg Calculate the engineering stress on the bar inmegapascal (MPa)
Solrsquon F= ma = 2500 x 981 = 24 500 N
Ao = π r 2 = π ( 00125 2 4 )
σ = Ft Ao = 2 x 10 8 Pa = 200 MPa
30 July 2007 10
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
When an unaxial tensile force is applied to a rod it causesthe rod to be elongated in the direction of the force
Engineering strain is the ratio of the change in the length ofthe sample in the direction of the force divided by the originallength
ε = ( l ndash lo ) lo = ∆ l lo Where ∆l = l - lo is the change in length l0 = original length of the specimen In engineering practice it is common to convert engineering
strain into percent strain or percent elongation engineering strain = engineering strain x 100 =
elongation Unit of engineering strain Inch inch or mm which is dimensionless
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 6216
30 July 2007 11
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
L
Engineeringstress
Engineering(normal) strain
==
== A
F
δ ε
σ
A
F
L
A
F
δ ε
σ
=
==2
2
LL
A
F
δ δ ε
σ
==
=
2
2
30 July 2007 12
3143 STRESS ndash STRAIN TESTING
Tension tests they are common since they are easier toperform for most structural materials steel etc
Compression tests are used when a materialrsquos under largeand permanent strains is desired or when the material is
brittle in tension concrete Shear and torsion tests Torsion test are performed on
cylindrical solid shafts or tubes machine axles and driveshafts
Typical tensile Specimen
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 7217
30 July 2007 13
3143 STRESS ndash STRAIN TESTINGHydraulic
Wedge
Grips
SpecimenExtensometer
Schematic representation of the apparatusused to conduct tensile stress - strain tests
Typical tensile test machine
30 July 2007 14
3144 YOUNGS MODULUS (E)
During ElasticDeformation Stress Strain = a constant
σ ε= E =Modulus ofelasticity (YoungrsquosModulus) (ElastisiteModuumlluuml) (MPa)
Modulus of Elasticitygives an idea aboutmaterialrsquos resistanceto elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 8218
30 July 2007 15
STIFFNESSMaterialrsquos resistance to
Elastic Deformation
Atomic Origin of Stiffness
Strongly Bonded
Weakly Bonded
N e t I n t e r a t o m i c F o r c e
Interatomic Distance
E prop dF
dr
r o
The value of the Modulus of Elasticity isthe measure of STIFFNESS
30 July 2007 16
Metal Alloy Modulus of Elasticity
E ( GPa)
Aluminum
Brass
Copper
Magnesium
Nickel
Steel
Titanium
Tungsten
69
97
110
45
207
207
107
407
3144 YOUNGS MODULUS (E)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 4214
30 July 2007 7
314 STRESS amp STRAIN
Tension Compression Shear Torsion
Reference Callister Material Science and Eng 5th Ed p114
Types of force(load) applied on the object
30 July 2007 8
3141 ENGINEERING STRESS (σ)
(Gerilme)
Stress is defined as force F applied over the original cross-sectional area Ao
For a tensile test the stress is given by
Stress (MPa or psi)
Where F = applied tensile force (N or lbs) A0= original cross-sectional area of the test specimen (m2 or in2)
Units for Engineering Stress US customary pounds per square inch (psi) SI N m-2 = Pascal (Pa) 1psi = 689 x 10 3 Pa
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 5215
30 July 2007 9
3141 ENGINEERING STRESS (σ)
(Gerilme)
Example A 125 cm diameter bar is subjected to a load of2500 kg Calculate the engineering stress on the bar inmegapascal (MPa)
Solrsquon F= ma = 2500 x 981 = 24 500 N
Ao = π r 2 = π ( 00125 2 4 )
σ = Ft Ao = 2 x 10 8 Pa = 200 MPa
30 July 2007 10
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
When an unaxial tensile force is applied to a rod it causesthe rod to be elongated in the direction of the force
Engineering strain is the ratio of the change in the length ofthe sample in the direction of the force divided by the originallength
ε = ( l ndash lo ) lo = ∆ l lo Where ∆l = l - lo is the change in length l0 = original length of the specimen In engineering practice it is common to convert engineering
strain into percent strain or percent elongation engineering strain = engineering strain x 100 =
elongation Unit of engineering strain Inch inch or mm which is dimensionless
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 6216
30 July 2007 11
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
L
Engineeringstress
Engineering(normal) strain
==
== A
F
δ ε
σ
A
F
L
A
F
δ ε
σ
=
==2
2
LL
A
F
δ δ ε
σ
==
=
2
2
30 July 2007 12
3143 STRESS ndash STRAIN TESTING
Tension tests they are common since they are easier toperform for most structural materials steel etc
Compression tests are used when a materialrsquos under largeand permanent strains is desired or when the material is
brittle in tension concrete Shear and torsion tests Torsion test are performed on
cylindrical solid shafts or tubes machine axles and driveshafts
Typical tensile Specimen
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 7217
30 July 2007 13
3143 STRESS ndash STRAIN TESTINGHydraulic
Wedge
Grips
SpecimenExtensometer
Schematic representation of the apparatusused to conduct tensile stress - strain tests
Typical tensile test machine
30 July 2007 14
3144 YOUNGS MODULUS (E)
During ElasticDeformation Stress Strain = a constant
σ ε= E =Modulus ofelasticity (YoungrsquosModulus) (ElastisiteModuumlluuml) (MPa)
Modulus of Elasticitygives an idea aboutmaterialrsquos resistanceto elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 8218
30 July 2007 15
STIFFNESSMaterialrsquos resistance to
Elastic Deformation
Atomic Origin of Stiffness
Strongly Bonded
Weakly Bonded
N e t I n t e r a t o m i c F o r c e
Interatomic Distance
E prop dF
dr
r o
The value of the Modulus of Elasticity isthe measure of STIFFNESS
30 July 2007 16
Metal Alloy Modulus of Elasticity
E ( GPa)
Aluminum
Brass
Copper
Magnesium
Nickel
Steel
Titanium
Tungsten
69
97
110
45
207
207
107
407
3144 YOUNGS MODULUS (E)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 5215
30 July 2007 9
3141 ENGINEERING STRESS (σ)
(Gerilme)
Example A 125 cm diameter bar is subjected to a load of2500 kg Calculate the engineering stress on the bar inmegapascal (MPa)
Solrsquon F= ma = 2500 x 981 = 24 500 N
Ao = π r 2 = π ( 00125 2 4 )
σ = Ft Ao = 2 x 10 8 Pa = 200 MPa
30 July 2007 10
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
When an unaxial tensile force is applied to a rod it causesthe rod to be elongated in the direction of the force
Engineering strain is the ratio of the change in the length ofthe sample in the direction of the force divided by the originallength
ε = ( l ndash lo ) lo = ∆ l lo Where ∆l = l - lo is the change in length l0 = original length of the specimen In engineering practice it is common to convert engineering
strain into percent strain or percent elongation engineering strain = engineering strain x 100 =
elongation Unit of engineering strain Inch inch or mm which is dimensionless
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 6216
30 July 2007 11
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
L
Engineeringstress
Engineering(normal) strain
==
== A
F
δ ε
σ
A
F
L
A
F
δ ε
σ
=
==2
2
LL
A
F
δ δ ε
σ
==
=
2
2
30 July 2007 12
3143 STRESS ndash STRAIN TESTING
Tension tests they are common since they are easier toperform for most structural materials steel etc
Compression tests are used when a materialrsquos under largeand permanent strains is desired or when the material is
brittle in tension concrete Shear and torsion tests Torsion test are performed on
cylindrical solid shafts or tubes machine axles and driveshafts
Typical tensile Specimen
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 7217
30 July 2007 13
3143 STRESS ndash STRAIN TESTINGHydraulic
Wedge
Grips
SpecimenExtensometer
Schematic representation of the apparatusused to conduct tensile stress - strain tests
Typical tensile test machine
30 July 2007 14
3144 YOUNGS MODULUS (E)
During ElasticDeformation Stress Strain = a constant
σ ε= E =Modulus ofelasticity (YoungrsquosModulus) (ElastisiteModuumlluuml) (MPa)
Modulus of Elasticitygives an idea aboutmaterialrsquos resistanceto elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 8218
30 July 2007 15
STIFFNESSMaterialrsquos resistance to
Elastic Deformation
Atomic Origin of Stiffness
Strongly Bonded
Weakly Bonded
N e t I n t e r a t o m i c F o r c e
Interatomic Distance
E prop dF
dr
r o
The value of the Modulus of Elasticity isthe measure of STIFFNESS
30 July 2007 16
Metal Alloy Modulus of Elasticity
E ( GPa)
Aluminum
Brass
Copper
Magnesium
Nickel
Steel
Titanium
Tungsten
69
97
110
45
207
207
107
407
3144 YOUNGS MODULUS (E)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 6216
30 July 2007 11
3142 ENGINEERING STRAIN
(Şekil Değiştirme)
L
Engineeringstress
Engineering(normal) strain
==
== A
F
δ ε
σ
A
F
L
A
F
δ ε
σ
=
==2
2
LL
A
F
δ δ ε
σ
==
=
2
2
30 July 2007 12
3143 STRESS ndash STRAIN TESTING
Tension tests they are common since they are easier toperform for most structural materials steel etc
Compression tests are used when a materialrsquos under largeand permanent strains is desired or when the material is
brittle in tension concrete Shear and torsion tests Torsion test are performed on
cylindrical solid shafts or tubes machine axles and driveshafts
Typical tensile Specimen
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 7217
30 July 2007 13
3143 STRESS ndash STRAIN TESTINGHydraulic
Wedge
Grips
SpecimenExtensometer
Schematic representation of the apparatusused to conduct tensile stress - strain tests
Typical tensile test machine
30 July 2007 14
3144 YOUNGS MODULUS (E)
During ElasticDeformation Stress Strain = a constant
σ ε= E =Modulus ofelasticity (YoungrsquosModulus) (ElastisiteModuumlluuml) (MPa)
Modulus of Elasticitygives an idea aboutmaterialrsquos resistanceto elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 8218
30 July 2007 15
STIFFNESSMaterialrsquos resistance to
Elastic Deformation
Atomic Origin of Stiffness
Strongly Bonded
Weakly Bonded
N e t I n t e r a t o m i c F o r c e
Interatomic Distance
E prop dF
dr
r o
The value of the Modulus of Elasticity isthe measure of STIFFNESS
30 July 2007 16
Metal Alloy Modulus of Elasticity
E ( GPa)
Aluminum
Brass
Copper
Magnesium
Nickel
Steel
Titanium
Tungsten
69
97
110
45
207
207
107
407
3144 YOUNGS MODULUS (E)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 7217
30 July 2007 13
3143 STRESS ndash STRAIN TESTINGHydraulic
Wedge
Grips
SpecimenExtensometer
Schematic representation of the apparatusused to conduct tensile stress - strain tests
Typical tensile test machine
30 July 2007 14
3144 YOUNGS MODULUS (E)
During ElasticDeformation Stress Strain = a constant
σ ε= E =Modulus ofelasticity (YoungrsquosModulus) (ElastisiteModuumlluuml) (MPa)
Modulus of Elasticitygives an idea aboutmaterialrsquos resistanceto elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 8218
30 July 2007 15
STIFFNESSMaterialrsquos resistance to
Elastic Deformation
Atomic Origin of Stiffness
Strongly Bonded
Weakly Bonded
N e t I n t e r a t o m i c F o r c e
Interatomic Distance
E prop dF
dr
r o
The value of the Modulus of Elasticity isthe measure of STIFFNESS
30 July 2007 16
Metal Alloy Modulus of Elasticity
E ( GPa)
Aluminum
Brass
Copper
Magnesium
Nickel
Steel
Titanium
Tungsten
69
97
110
45
207
207
107
407
3144 YOUNGS MODULUS (E)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 8218
30 July 2007 15
STIFFNESSMaterialrsquos resistance to
Elastic Deformation
Atomic Origin of Stiffness
Strongly Bonded
Weakly Bonded
N e t I n t e r a t o m i c F o r c e
Interatomic Distance
E prop dF
dr
r o
The value of the Modulus of Elasticity isthe measure of STIFFNESS
30 July 2007 16
Metal Alloy Modulus of Elasticity
E ( GPa)
Aluminum
Brass
Copper
Magnesium
Nickel
Steel
Titanium
Tungsten
69
97
110
45
207
207
107
407
3144 YOUNGS MODULUS (E)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 9219
30 July 2007 17
3144 YOUNGS MODULUS (E)
Engineering Strain ε = ∆LLo)0002
E n g i n e e r i n g
S t r e s s σ = F A o
Total Elongation
E
30 July 2007 18
315 ELASTIC DEFORMATION
Elasticity or elastic deformation is defined as ability of returning toan initial state or form after deformation
In most engineering materials however there will also exist a time-dependent elastic strain component That is elastic deformation willcontinue after the stress application and upon load release some
finite time is required for complete recovery This time-dependentelastic behavior is known as ANELASTICITY and it is due to time-dependent microscopic and atomistic processes that are attendant tothe deformation
For metals the inelastic component is normally small and is oftenneglected However for some polymeric materials its magnitude issignificant in this case it is termed VISCOELASTIC BEHAVİOR
A simplified view of ametal bars structure
P
The same metal bar thistime with an applied load
After the load is releasedthe bar returns to itsoriginal shape This iscalled elastic deformation
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 102110
30 July 2007 19
315 ELASTIC DEFORMATION EXAMPLE A piece of copper originally 305 mm (12 in) long is
pulled in tension with a stress of 276 MPa (40000 psi)If the deformation is entirely elastic what will be theresultant elongation
Solrsquon
Since the deformation is elastic strain is linearlydependent on stress the magnitude of E for copper is
110 GPa ε= (l ndash lo ) lo = ∆ l lo 991750l = (276 MPa) (305 mm) 110 x 103 MPa = 077 mm
= E ε εε ε σ
30 July 2007 20
316 PLASTIC DEFORMATION ampPLASTICITY
For most metallic materialselastic deformation existsonly to strains of about0005 As the material isdeformed beyond this
point the stress is notproportional to strain Andpermanent nonrecoverabledeformations PLASTICDEFORMATION occurs
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 112111
30 July 2007 21
316 PLASTIC DEFORMATION amp
PLASTICITY
30 July 2007 22
317 STRENGTH3171 YIELD STRENGTH ( Y ) ( MPa or psi )
Stress at which noticeable plastic deformation hasoccurred
The magnitude of the yield strength for a metal is ameasure of its resistance to plastic deformation
A straight line is drawn parallel to the elastic deformation
part of the curve from the engineering strain value of0002 The stress corresponding to the intersection pointof these two lines is YIELD STRENGTH
Yield strengths may range from 35 MPa for a low strengthAl to over 1400 MPa for high strength steels
Comparison of Yield Strength σy (ceramics) gtgt σ y (metals) gtgt σ y (polymers)
gtgt σ y (composites)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 122112
30 July 2007 23
3172 TENSİLE STRENGTH (TS)
( MPa or psi )
The stress at the maximum on the engineering stress-strain curve
This corresponds to the maximum stress that can beresisted by a structure in tension It is the maximumstress without fracture
Examples metals occurs when noticeable ldquoneckingrdquo starts ceramics occurs when crack propagation starts polymers occurs when polymer backbones are all
aligned and about to break
Tensile Strengths may vary from 50 MPa to 3000 MPa
30 July 2007 24
3173 COMPRESSIVE (CRUSHING)STRENGTH
It is important inceramics used instructures such asbuildings or refractory
bricks Thecompressive strengthof a ceramic is usuallymuch greater thantheir tensile strength
Tensile compressiveand bending testingfor materials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 132113
30 July 2007 25
3173 COMPRESSIVE (CRUSHING)
STRENGTHComparisonof Stress -
StrainCurves for
MetalsCeramicsPolymers
andElastomers
30 July 2007 26
3173 COMPRESSIVE (CRUSHING)STRENGTH
The Relationship between Elastic Modulus and Melting Temperature
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 142114
30 July 2007 27
318 BRITTLENESS TOUGHNESS RESILIENCEamp DUCTILITY
3181 BRITTLENESS
A material that experiences very little or no plasticdeformation upon fracture is termed brittle
Ductile vs Brittle Materials
bull Only Ductile materials will exhibit necking
bull Ductile if ELgt8 (approximately)
bull Brittle if EL lt 5 (approximately)
X
XX A
B C
XDBrittle Ductile
A amp B C amp D
E n g i n e e r i n g S t r e s s
Engineering Strain
30 July 2007 28
3181 BRITTLENESS
Brittle Fracture Surfaces
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 152115
30 July 2007 29
3182 TOUGHNESS
A measure of the ability of a material to absorb energywithout fracture
(Jm3 or N mm3= MPa) It is a measure of the ability of a material to absorb
energy up to fracture Energy needed to break a unit volume of material Area under stress-strain curve For a material to be tough it must display both
strength and ductility Often ductile materials are tougher than brittle ones Examples
smaller toughness (ceramics) larger toughness(metals PMCs) smaller toughness unreinforced ( polymers)
30 July 2007 30
3182 TOUGHNESS
Toughness Ut
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s S = P A o
X
U t = S deo
e f
int
asymp(S y + S u )
2
EL
100
SuSy
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 162116
30 July 2007 31
3182 TOUGHNESS
Toughness is really ameasure of the energy asample can absorbbefore it breaks
30 July 2007 32
3183 RESILIENCE
A measure of the ability of a material to absorb energywithout plastic or permanent deformation (Jm3 or Nmm3= MPa)
X
Resilience Ur
Engineering Strain e = ∆LLo)
E n g i n e e r i n g S t r e s s
S = P A o
U r = S deo
e y
int
asymp S y e y
2
= S y
2
2 E
SuSy
E
ey
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 172117
30 July 2007 33
3184 DUCTILITY ( EL)
Ductility is another important mechanical property
It is a measure of the degree of plastic deformationthat has been sustained at fracture
30 July 2007 34
3184 DUCTILITY ( EL)
Stress-Strain diagrams fortypical (a) brittle and (b) ductile
materials
Stress- StrainCurves for Brittle
and DuctileMaterials
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 182118
30 July 2007 35
3184 DUCTILITY ( EL)Ductile Materials
Brittle Materials
30 July 2007 36
3184 DUCTILITY ( EL)
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 192119
30 July 2007 37
STRESS ndash STRAIN CURVES
Stress- Strain Curves for Different Materials
CURVE EXAMPLEA Stiff but Weak CERAMICB Stiff and Strong CERAMICC Stiff and Strong METALC Moderately Stiff and Strong METALD Flexible and Moderately Strong POLYMERE Flexible and Weak POLYMER
30 July 2007 38
319 FATIGUE
If placed under too large of a stress metals will mechanicallyfail or fracture This can also result over time from manysmall stresses The most common reason (about 80) formetal failure is fatigue
The most common reason (about 80) for metal failure isfatigue
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 202120
30 July 2007 39
FATIGUE MECHANISM
30 July 2007 40
FATIGUE MECHANISM
This front brake assembly broke off under braking and severely injured the cyclistPoor maintenance had allowed the brake bolt to loosen and allow the assembly to
chatter when braking imposing cyclic loads instead of steady stress on the fasteningbolt
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition
8122019 CH5 -Mechanical Properties of Matpdf
httpslidepdfcomreaderfullch5-mechanical-properties-of-matpdf 2121
30 July 2007 41
MECHANICAL PROPERTIES
Typical Mechanical Properties
Material Yield Stress(MPa)
UltimateStress (MPa)
DuctilityEL
Elastic Modulus(MPa)
PoissonrsquosRatio
1040 Steel 350 520 30 207000 030
1080 Steel 380 615 25 207000 0302024 Al Alloy 100 200 18 72000 033
316 Stainless Steel 210 550 60 195000 030
7030 Brass 75 300 70 110000 035
6-4 Ti Alloy 942 1000 14 107000 036AZ80 Mg Alloy 285 340 11 45000 029
Metals in annealed (soft) condition