Mechanical Properties - Stresses & Strains - NC State: …murty/NE509/NOTES/Ch4a-mechanica… ·...
Transcript of Mechanical Properties - Stresses & Strains - NC State: …murty/NE509/NOTES/Ch4a-mechanica… ·...
Mechanical Properties - Stresses & Strains
Types of Deformation : Elasic Plastic Anelastic Elastic deformation is defined as instantaneous recoverable deformation
Hooke's law : For tensile loading, σ = E ε where σ is stress defined as the load per unit area : σ = P/Ao, N/m2, Pa
and strain is given by the change in length per unit length ε = ∆llo , %
The proportionality constant E is the Young's modulus or modulus of Elasticity :
E ~ 10x106 psi [68.9 GPa] for metals [varying from 10x106 psi for Al, 30x106 for Fe
and 59x106 for W].
Poisson's Ratio [ν] : ratio of lateral contraction to longitudinal elongation ν = - εx / εz = - εy / εz [for isotropic materials]; in general, ν ~ 0.3
Thus the total contractile strains is less than the expansion along the tensile axis thereby resulting in a slight increase in the volume of the material under stress - this is known as Elastic Dilation .
Modulus Of Rigidity or Shear Modulus [G] : G = τ / γ ; G is the shear modulus and is related to E andν , G = E / 2(1+ν ).
Bulk Modulus [κ] : the change in volume to the original volume is proportional to the hydrostatic pressure [σhyd] : ∆V/V = β σhyd , where β is the compressibility .
The inverse of the compressibility is the bulk modulus [κ] : κ = 1/β .
κ is also related to E and ν : κ = E / 3(1-2ν ) = 2G(1+ν ) / 3(1-2ν ). • • • Thus one can evaluate the various elastic moduli from one or more experimentally evaluated constants. Note that the elastic moduli are related to the interatomic bonding and thus decrease [slightly] with increasing temperature. Any change in the crystal structure, for example following a phase change [polymorphism], one notes a distinct change in the elastic moduli
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Stress - Strain Curve
Definitions
Nominal (engineering) vs True
S = P
Ao , e =
∆llo σ =
PA , ε = ln (
llo )
Proportional limit (PL) Yield strength (Sy) 0.2% offset; (SLY)
Tensile strength (TS or UTS or SUTS) Fracture strength (SF) Uniform elongation (eu)
Total elongation (ductility) (et or ef in 2” )
Necking strain (en = et - eu)
Reduction in area (ductility) (RA) Volume increases (Elastic Dilation)
σ = S (1+e) & ε = ln (1+e) true Yield stress (σy) 0.2% offset
true Tensile strength (TS or UTS or σUTS)
true Fracture strength (σF)
true Uniform strain (εu)
true Total elongation (ductility) (εt or ef in 2” )
true Necking strain (εn = εt - εu)
Volume is conserved Aolo = Al
Energy to fracture
Elastic (σ = E ε ) Plastic (σ = K εn )
Resilience (Uel = σ2
2E ) units (J/m3) Toughness (J = K εn+1
n+1 )
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σ - ε curves smooth (SSs & fcc) with yield point (steels & bcc)
Rate Effects
Plastic deformation is rate dependent (generally at high temperatures) : σ ≡ f( ε& ) = A ε& m, m = SRS = )
lnd(
ε&lnd σ
T,ε
m ~ 0 at low temperatures m|max = 1
m↑ et↑ vs n↑ eu↑
Group Work :
left of the instructor : (1) Derive relation between σ and S :
right of the instructor : (2) Derive relation between ε and e :
all (3) Show that εu= n
KL Murty
from Ashby and Jones
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⇒ ⇒
0dedS n
TSu =
⇔ε=
1nKU
1npl
+ε
=+
σ = Kεn where n is the work-hardening parameter and K is the strength coefficient.
n = 0 perfect plastic solid and n = 1 perfect elastic solid
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Hardness Def. Resistance to surface penetration
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Charpy Impact Test
Fracture Surfaces
T, C
Effect of C-content on CV for steel
(note decreased energy and increased DBTT
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