Chapter 6: Mechanical Properties

Slides:



Advertisements
Similar presentations
Mechanical Properties of Metals
Advertisements

2E4: SOLIDS & STRUCTURES Lecture 9
ISE316 Chapter 3 --Mechanics of materials
Dr. HABEEB HATTAB HABEEB Office: BN-Block, Level-3, Room Ext. No.: 7292 Lecturer: Dr. HABEEB ALANI.
Elasticity by Ibrhim AlMohimeed
Week 4 MECHANICAL PROPERTIES AND TESTS
MECHANICAL PROPERTIES
Normal Strain and Stress
Chapter 3 Mechanical Properties of Materials
MECHANICAL PROPERTIES OF MATERIALS
Chapter 7 Mechanical Properties of Solids.
Chapter 6: Mechanical Properties
ENGR-45_Lec-15_Metal_MechProp-2.ppt 1 Bruce Mayer, PE Engineering-45: Materials of Engineering Bruce Mayer, PE Licensed Electrical.
Materials Engineering – Day 2
CHAPTER 7: MECHANICAL PROPERTIES
EXPERIMENT # 3 Instructor: M.Yaqub
CHAPTER 6: MECHANICAL PROPERTIES
Chapter 7:機械性質(Mechanical Properties)
Chapter 6: Behavior Of Material Under Mechanical Loads = Mechanical Properties. Stress and strain: What are they and why are they used instead of load.
Tensile Test The most common static test is the uniaxial tensile test, which provides information about a variety of properties. As a load is applied to.
Lecture 26: Mechanical Properties I: Metals & Ceramics
ENGR 225 Section
Lecture # 6 Mechanical Properties of Metals Intended learning Outcomes: After the end of this lecture the student should be able to: Define stress –strain.
Mechanical Properties of Metals
Special Assignment  Add figures/graphics to all slides  Use bullets instead of short sentences  For the 15’ presentations use fonts 18 or bigger; however,
Chapter 6: Mechanical Properties
Mechanical Properties
CHAPTER 6: MECHANICAL PROPERTIES
Mechanical Properties
ME260 Mechanical Engineering Design II Instructor notes.
Objectives Students will be able to label a stress-strain diagram correctly indicating. Ultimate stress, yield stress and proportional limit. Students.
FYI: All three types of stress are measured in newtons / meter2 but all have different effects on solids. Materials Solids are often placed under stress.
Mechanical Properties
Class #1.2 Civil Engineering Materials – CIVE 2110
ENGR-45_Lec-14_Metal_MechProp-1.ppt 1 Bruce Mayer, PE Engineering-45: Materials of Engineering Bruce Mayer, PE Registered Electrical.
 Stress has units: N/m 2 or lb f /in 2 Engineering Stress Shear stress,  : Area, A F t F t F s F F F s  = F s A o Tensile stress,  : original area.
CONCEPTS OF FORCE-STRESS and DEFORMATION- STRAIN.
CHAPTER 7: MECHANICAL PROPERTIES
4 Mechanical Properties of Biomaterials CHAPTER 4.1 Introduction
Poisson's ratio, n • Poisson's ratio, n: Units:
Chapter 2 Properties of Metals.
Mechanical Properties of Materials
Mechanical Behavior: Part I Dr. Aaron L. Adams, Assistant Professor
Haseeb Ullah Khan Jatoi Department of Chemical Engineering UET Lahore.
STRUCTURES Young’s Modulus. Tests There are 4 tests that you can do to a material There are 4 tests that you can do to a material 1 tensile This is where.
Chapter ISSUES TO ADDRESS... Stress and strain: What are they and why are they used instead of load and deformation? Elastic behavior: When loads.
Mechanical & Aerospace Engineering West Virginia University Elastic Properties of Materials, Tensile Test Xingbo Liu.
SIMPLE STRESS & STRAIN ► EN NO GUIDED BY EN NO PROF. V.R.SHARMA GEC PALANPUR APPLIED MECHANICS DEPARTMENT.
Chapter ISSUES TO ADDRESS... Stress and strain: What are they and why are they used instead of load and deformation? Elastic behavior: When loads.
Chapter 7: Mechanical Properties
Chapter 4. Mechanical Testing: Tension Test and Other Basic Tests
Chapter 6: Mechanical Properties
CHAPTER 6: MECHANICAL PROPERTIES
CHAPTER 6: MECHANICAL PROPERTIES
Special Assignment Add figures/graphics to all slides
Mechanical properties of Materials
Introduction We select materials for many components and applications by matching the properties of the material to the service condition required of the.
MECHANICAL PROPERTIES OF MATERIALS
MEKANIKA MATERIAL (BAHAN)
Poisons Ratio Poisons ratio = . w0 w Usually poisons ratio ranges from
ME260 Mechanical Engineering Design II
Introduction to Materials Science and Engineering
Mechanical Properties of Metals
Mechanical Properties: 1
CHAPTER 6: MECHANICAL PROPERTIES
Elastic & Plastic behavior of Materials
PDT 153 Materials Structure And Properties
Simple Stresses & Strain
Mechanical Properties Of Metals - I
Mechanical Property 기계적 성질
Presentation transcript:

Chapter 6: Mechanical Properties ISSUES TO ADDRESS... • Stress and strain: What are they and why are they used instead of load and deformation? • Elastic behavior: When loads are small, how much deformation occurs? What materials deform least? • Plastic behavior: At what point does permanent deformation occur? What materials are most resistant to permanent deformation? • Toughness and ductility: What are they and how do we measure them?

Elastic Deformation d F F d 1. Initial 2. Small load 3. Unload bonds stretch 3. Unload return to initial F Linear- elastic Elastic means reversible! Non-Linear- elastic d

Plastic Deformation (Metals) 1. Initial 2. Small load 3. Unload planes still sheared F d elastic + plastic bonds stretch & planes shear plastic F d linear elastic plastic Plastic means permanent!

Engineering Stress s = F A F t s = A m N or in lb • Tensile stress, s: original area before loading s = F t A o 2 f m N or in lb Area, Ao • Shear stress, t: Area, Ao F t s = A o  Stress has units: N/m2 or lbf /in2

Common States of Stress • Simple tension: cable A o = cross sectional area (when unloaded) F o s = F A s Ski lift (photo courtesy P.M. Anderson) • Torsion (a form of shear): drive shaft M A o 2R F s c o t = F s A Note: t = M/AcR here.

OTHER COMMON STRESS STATES (i) • Simple compression: A o Balanced Rock, Arches National Park (photo courtesy P.M. Anderson) Canyon Bridge, Los Alamos, NM o s = F A Note: compressive structure member (s < 0 here). (photo courtesy P.M. Anderson)

OTHER COMMON STRESS STATES (ii) • Bi-axial tension: • Hydrostatic compression: Fish under water Pressurized tank (photo courtesy P.M. Anderson) (photo courtesy P.M. Anderson) s z > 0 q s < 0 h

Engineering Strain L w e = d L - d e = w q g = Dx/y = tan • Tensile strain: d /2 L o w • Lateral strain: e = d L o - d e L = w o d L /2 • Shear strain: q 90º 90º - q y x g = Dx/y = tan Strain is always dimensionless. Adapted from Fig. 6.1(a) and (c), Callister & Rethwisch 8e.

Stress-Strain Testing • Typical tensile test machine • Typical tensile specimen Adapted from Fig. 6.2, Callister & Rethwisch 8e. gauge length specimen extensometer Adapted from Fig. 6.3, Callister & Rethwisch 8e. (Fig. 6.3 is taken from H.W. Hayden, W.G. Moffatt, and J. Wulff, The Structure and Properties of Materials, Vol. III, Mechanical Behavior, p. 2, John Wiley and Sons, New York, 1965.)

Linear Elastic Properties • Modulus of Elasticity, E: (also known as Young's modulus) • Hooke's Law: s = E e s Linear- elastic E e F simple tension test

Poisson's ratio, n eL e -n e n = - • Poisson's ratio, n: Units: metals: n ~ 0.33 ceramics: n ~ 0.25 polymers: n ~ 0.40 Units: E: [GPa] or [psi] n: dimensionless  > 0.50 density increases  < 0.50 density decreases (voids form)

Mechanical Properties Slope of stress strain plot (which is proportional to the elastic modulus) depends on bond strength of metal Adapted from Fig. 6.7, Callister & Rethwisch 8e.

Other Elastic Properties simple torsion test M t G g • Elastic Shear modulus, G: t = G g • Elastic Bulk modulus, K: pressure test: Init. vol =Vo. Vol chg. = DV P P = - K D V o • Special relations for isotropic materials: 2(1 + n) E G = 3(1 - 2n) K

Young’s Moduli: Comparison Graphite Ceramics Semicond Metals Alloys Composites /fibers Polymers 0.2 8 0.6 1 Magnesium, Aluminum Platinum Silver, Gold Tantalum Zinc, Ti Steel, Ni Molybdenum G raphite Si crystal Glass - soda Concrete Si nitride Al oxide PC Wood( grain) AFRE( fibers) * CFRE GFRE* Glass fibers only Carbon fibers only A ramid fibers only Epoxy only 0.4 0.8 2 4 6 10 00 1200 Tin Cu alloys Tungsten <100> <111> Si carbide Diamond PTF E HDP LDPE PP Polyester PS PET C FRE( fibers) FRE( fibers)* FRE(|| fibers)* E(GPa) Based on data in Table B.2, Callister & Rethwisch 8e. Composite data based on reinforced epoxy with 60 vol% of aligned carbon (CFRE), aramid (AFRE), or glass (GFRE) fibers. 109 Pa

Useful Linear Elastic Relationships • Simple tension: • Simple torsion: a = 2 ML o  r 4 G M = moment = angle of twist 2ro Lo d = FL o E A d L = - n Fw o E A F A o d /2 L Lo w • Material, geometric, and loading parameters all contribute to deflection. • Larger elastic moduli minimize elastic deflection.

Plastic (Permanent) Deformation (at lower temperatures, i.e. T < Tmelt/3) • Simple tension test: Elastic+Plastic at larger stress engineering stress, s Elastic initially permanent (plastic) after load is removed ep plastic strain engineering strain, e Adapted from Fig. 6.10(a), Callister & Rethwisch 8e.

Yield Strength, sy y = yield strength sy • Stress at which noticeable plastic deformation has occurred. when ep = 0.002 tensile stress, s engineering strain, e sy ep = 0.002 y = yield strength Note: for 2 inch sample  = 0.002 = z/z  z = 0.004 in Adapted from Fig. 6.10(a), Callister & Rethwisch 8e.

Yield Strength : Comparison Graphite/ Ceramics/ Semicond Metals/ Alloys Composites/ fibers Polymers Yield strength, s y (MPa) PVC Hard to measure , since in tension, fracture usually occurs before yield. Nylon 6,6 LDPE 70 20 40 60 50 100 10 30 200 300 400 500 600 700 1000 2000 Tin (pure) Al (6061) a ag Cu (71500) hr Ta (pure) Ti Steel (1020) cd (4140) qt (5Al-2.5Sn) W Mo (pure) cw Hard to measure, in ceramic matrix and epoxy matrix composites, since in tension, fracture usually occurs before yield. H DPE PP humid dry PC PET ¨ Room temperature values Based on data in Table B.4, Callister & Rethwisch 8e. a = annealed hr = hot rolled ag = aged cd = cold drawn cw = cold worked qt = quenched & tempered

VMSE: Virtual Tensile Testing

Tensile Strength, TS TS engineering stress strain engineering strain • Maximum stress on engineering stress-strain curve. y strain Typical response of a metal F = fracture or ultimate strength Neck – acts as stress concentrator engineering TS stress engineering strain Adapted from Fig. 6.11, Callister & Rethwisch 8e. • Metals: occurs when noticeable necking starts. • Polymers: occurs when polymer backbone chains are aligned and about to break.

Tensile Strength: Comparison Si crystal <100> Graphite/ Ceramics/ Semicond Metals/ Alloys Composites/ fibers Polymers Tensile strength, TS (MPa) PVC Nylon 6,6 10 100 200 300 1000 Al (6061) a ag Cu (71500) hr Ta (pure) Ti Steel (1020) (4140) qt (5Al-2.5Sn) W cw L DPE PP PC PET 20 30 40 2000 3000 5000 Graphite Al oxide Concrete Diamond Glass-soda Si nitride H wood ( fiber) wood(|| fiber) 1 GFRE (|| fiber) ( fiber) C FRE A FRE( fiber) E-glass fib Aramid fib Room temperature values Based on data in Table B.4, Callister & Rethwisch 8e. a = annealed hr = hot rolled ag = aged cd = cold drawn cw = cold worked qt = quenched & tempered AFRE, GFRE, & CFRE = aramid, glass, & carbon fiber-reinforced epoxy composites, with 60 vol% fibers.

Ductility x 100 L EL % - = • Plastic tensile strain at failure: Lf Ao Adapted from Fig. 6.13, Callister & Rethwisch 8e. Engineering tensile strain, e E ngineering tensile stress, s smaller %EL larger %EL Lf Ao Af Lo • Another ductility measure: 100 x A RA % o f - =

Toughness • Energy to break a unit volume of material • Approximate by the area under the stress-strain curve. very small toughness (unreinforced polymers) Engineering tensile strain, e E ngineering tensile stress, s small toughness (ceramics) large toughness (metals) Adapted from Fig. 6.13, Callister & Rethwisch 8e. Brittle fracture: elastic energy Ductile fracture: elastic + plastic energy

Resilience, Ur 2 1 U e s @ Ability of a material to store energy Energy stored best in elastic region If we assume a linear stress-strain curve this simplifies to y r 2 1 U e s @ Adapted from Fig. 6.15, Callister & Rethwisch 8e.

Elastic Strain Recovery syi D syo Elastic strain recovery 2. Unload Stress 1. Load 3. Reapply load Strain Adapted from Fig. 6.17, Callister & Rethwisch 8e.

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 of 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 diamond

Hardness: Measurement 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

Hardness: Measurement Table 6.5

True Stress & Strain Note: S.A. changes when sample stretched True strain Adapted from Fig. 6.16, Callister & Rethwisch 8e.

( ) Hardening s e s s • An increase in sy due to plastic deformation. large hardening s y 1 s y small hardening e • Curve fit to the stress-strain response: s T = K e ( ) n “true” stress (F/A) “true” strain: ln(L/Lo) hardening exponent: n = 0.15 (some steels) to n = 0.5 (some coppers)

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 All samples have same value Because of large variability must have safety margin in engineering specifications where n is the number of data points

Design or Safety Factors • Design uncertainties mean we do not push the limit. • Factor of safety, N 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. 1045 plain carbon steel: s y = 310 MPa TS = 565 MPa F = 220,000N d L o 5 d = 0.067 m = 6.7 cm

Summary • Stress and strain: These are size-independent measures of load and displacement, respectively. • Elastic behavior: This reversible behavior often shows a linear relation between stress and strain. To minimize deformation, select a material with a large elastic modulus (E or G). • Plastic behavior: This permanent deformation behavior occurs when the tensile (or compressive) uniaxial stress reaches sy. • Toughness: The energy needed to break a unit volume of material. • Ductility: The plastic strain at failure.

ANNOUNCEMENTS Reading: Core Problems: Self-help Problems: