Mechanical Properties of Metals How do metals respond to external - - PowerPoint PPT Presentation

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Mechanical Properties of Metals How do metals respond to external loads? Chapter Outline Stress and Strain Tension Compression Shear Torsion Elastic deformation Plastic Deformation Yield Strength Tensile


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Mechanical Properties of Metals How do metals respond to external loads?

Chapter Outline ►Stress and Strain

  • Tension
  • Compression
  • Shear
  • Torsion

► Elastic deformation ► Plastic Deformation

  • Yield Strength
  • Tensile Strength
  • Ductility
  • Toughness
  • Hardness
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To understand and describe how materials deform (elongate, compress, twist) or break as a function of applied load, time, temperature, and other conditions we need first to discuss standard test methods and standard language for mechanical properties of materials.

Introduction

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Concepts of Stress and Strain (tension and compression)

To compare specimens of different sizes, the load is calculated per unit area.

Engineering stress: σ = F / Ao

F is load applied perpendicular to specimen cross-section; A0 is cross-sectional area (perpendicular to the force) before application of the load.

Engineering strain: ε = (Δl / lo) × 100 %

Δl is change in length, lo is the original length. These definitions of stress and strain allow one to compare test results for specimens of different cross- sectional area A0 and of different length l0. Stress and strain are positive for tensile loads,negative for compressive loads

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Types of loading

Torsion Shear Tensile compressive

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Hardness (I) Hardness is a measure of the material’s resistance to localized plastic deformation (e.g. dent or scratch) A qualitative Moh’s scale, determined by the ability of a material to scratch another material: from 1 (softest = talc) to 10 (hardest = diamond).

Different types of quantitative hardness test has been designed (Rockwell, Brinell, Vickers, etc.). Usually a small indenter (sphere, cone, or pyramid) is forced into the surface of a material under conditions of controlled magnitude and rate of loading. The depth or size of indentation is measured. The tests somewhat approximate, but popular because they are easy and non-destructive (except for the small dent).

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Hardness

  • Resistance to permanently indenting the surface.
  • Large hardness means:
  • - resistance to plastic deformation or cracking in

compression.

  • - better wear properties.

e.g., 10 mm sphere apply known force measure size

  • f indent after

removing load

d

D

Smaller indents mean larger hardness.

increasing hardness

most plastics brasses Al alloys easy to machine steels file hard cutting tools nitrided steels diamond

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  • Rockwell

– No major sample damage – Each scale runs to 130 but only useful in range 20-100. – Minor load 10 kg – Major load 60 (A), 100 (B) & 150 (C) kg

  • A = diamond, B = 1/16 in. ball, C = diamond
  • HB = Brinell Hardness

– TS (psia) = 500 x HB – TS (MPa) = 3.45 x HB

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Hardness (II)

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Both tensile strength and hardness may be regarded as degree of resistance to plastic deformation. Hardness is proportional to the tensile strength – but note that the proportionality constant is different for different materials.

For most steels TS (MPa) = 3.45 x HB

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Hardness tests are performed more frequently than any

  • ther mechanical test for several reasons:

1. Inexpensive and simply performed 2. No special specimen need be prepared 3. Nondestructive type of tests ( a small indentation is the only deformation) 4. Other mechanical properties may be estimated from hardness data.

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True Stress & Strain

Note: S.A. changes when sample stretched

  • True stress
  • True strain

i T

A F  

 

  • i

T

  ln  

   

         1 ln 1

T T

Adapted from Fig. 6.16, Callister & Rethwisch 8e.

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Hardening

  • Curve fit to the stress-strain response:

 T  K  T

 

n

“true” stress (F/A) “true” strain: ln(L/Lo) hardening exponent: n = 0.15 (some steels) to n = 0.5 (some coppers)

  • An increase in y due to plastic deformation.

large hardening small hardening

y

y 1

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Variability in Material Properties

  • Elastic modulus is material property
  • Critical properties depend largely on sample flaws

(defects, etc.). Large sample to sample variability.

  • Statistics

– Mean – Standard Deviation

฀ s  

n

xi  x

 

2

n 1          

1 2

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  • Design uncertainties mean we do not push the limit.
  • Factor of safety, N

N

y working

  

Often N is between 1.2 and 4

  • Example: Calculate a diameter, d, to ensure that yield does

not occur in the 1045 carbon steel rod below. Use a factor of safety of 5.

Design or Safety Factors

฀ 220,000N  d2 / 4

 

N

y working

  

1045 plain carbon steel:  y = 310 MPa TS = 565 MPa F = 220,000N

d L o d = 0.067 m = 6.7 cm

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What are the limits of “safe” deformation?

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Design stress: σd = N*σc where σc = maximum anticipated stress, N is the “design factor” > 1. Want to make sure that σd < σy Safe or working stress: σw = σy/N where N is “factor of safety” > 1. For practical engineering design, the yield strength is usually the important parameter