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10/12/2010 1 Structure and Properties of Materials Eighth Lecture Mechanical Properties and Behavior October 12, 2010 ENGR 230 Structure and Properties of Materials Nahid Abdel Salam 2 It is the response of materials to external forces Mechanical properties are expressed in terms of quantities that are functions of stress or strain or both stress and strain.

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Page 1: Lecture_8

10/12/2010

1

Structure and Properties of Materials

Eighth Lecture

Mechanical Properties and Behavior

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

2

It is the response of materials

to external forces

Mechanical properties

are expressed in terms of

quantities that are functions of

stress or strain or both stress

and strain.

Page 2: Lecture_8

10/12/2010

2

Introduction

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

3

The mechanical behavior of materials

is described by their mechanical

properties, which are measured with

idealized, simple tests;

These tests are designed to present

different types of loading conditions;

The properties of a materials

reported in various handbooks are

the results of these tests;

Introduction (cont.)

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

4

The material’s composition,

nature of bonding, crystal

structure, defects, and grain

size have a profound influence

on the strength and ductility

of metallic materials.

Page 3: Lecture_8

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October 12, 2010 ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

5

There are three factors involved in

defining the manner in which the

load is applied:

kind of stress induced;

rate at which the load is applied;

number of times the load is

applied

Types of Loading (stress induced)

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

6

TorsionTension

Compression Bending Shear

Page 4: Lecture_8

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Three groups of the rate of loading

Rate of loading

over a short time

(Static test)

very rapidly

(Dynamic test,

impact)

long-time (Creep

test)

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

7

Number of Times of Loading

Number of times the load is applied

Single application

Repeated application (Fatigue test)

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

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Page 5: Lecture_8

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A typical stress-strain diagram for a

ductile metal undergoing tension

October 12, 2010 ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam9

Definitions (V.I)

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

10

You are requested to know precisely the

definitions of the following:

stress, strain, strength, modulus of

elasticity E, shear modulus G,

yield strength, elastic limit,

proportional limit, ultimate tensile

strength UTS, Poisson’s ratio,

stiffness, toughness, ductility.

Page 6: Lecture_8

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Elastic Properties, E and Stiffness

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

11

The modulus of elasticity, Young’s

modulus E = σ / ε in elastic zone

In metallic materials, this modulus is

closely related to the binding forces;

For ceramics, the Young’s modulus

depends on the level of porosity;

Young’s modulus of a composite

depends upon the stiffness and amounts

of the individual components.

Stiffness

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

12

Young’s modulus is a measure of

the Stiffness of a component;

A stiff component, with a high

modulus of elasticity, will show

much smaller changes in

dimensions if the applied stress is

relatively small and, therefore,

causes only elastic deformation.

Page 7: Lecture_8

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Poisson’s Ratio

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

13

μ = εlateral / εlongitudinal

In elastic region μ = 0.25-0.4

In plastic region μ = 0.5

Ductility

Gage Length

Measure of Ductility

Elongation % = (L-Lo)/Lo %

Reduction in Area % = (A-Ao)/Ao%

• Higher elongation indicates higher

ductility.

• The smallest cross section can be

measured at or after fracture.

October 12, 2010

ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam14

Page 8: Lecture_8

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Toughness

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

15

Modulus of Toughness:

The amount of work per

unit volume of a material

required to carry the

material to failure under

static loading. It equals

the area under stress

strain curve up to

fracture.

Macroscopic deformation of metal

sample under tensile test

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

16

Page 9: Lecture_8

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9

Effect of temperature and Strain rate

October 12, 2010ENGR 230

Structure and Properties of Materials

Nahid Abdel Salam

17