Chapter 6: Mechanical Properties

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1 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? Chapter 6-1

2 Elastic Deformation 1. Initial 2. Small load 3. Unload bonds stretch d Elastic means reversible! F F Linearelastic d return to initial Non-Linearelastic Chapter 6-2

3 Plastic Deformation (Metals) 1. Initial 2. Small load 3. Unload bonds stretch planes & planes still shear sheared d elastic + plastic d plastic F F Plastic means permanent! linear elastic d plastic linear elastic d Chapter 6-3

4 Tensile stress, s: Engineering Stress F t Shear stress, t: F t F Area, A o Area, A o F s s = F t lb f = 2 A o in original area before loading F t or N 2 m t = F s A o F s F Stress has units: N/m 2 or lb f /in 2 F t Chapter 6-4

5 Common States of Stress Simple tension: cable F A o = cross sectional area (when unloaded) s = F A A c M o 2R s M F Torsion (a form of shear): drive shaft s F s A o t = F s A o Note: t = M/A c R here. Ski lift (photo courtesy P.M. Anderson) Chapter 6-5

6 OTHER COMMON STRESS STATES (i) Simple compression: A o Canyon Bridge, Los Alamos, NM (photo courtesy P.M. Anderson) Balanced Rock, Arches National Park (photo courtesy P.M. Anderson) s = F A o Note: compressive structure member (s < 0 here). Chapter 6-6

7 OTHER COMMON STRESS STATES (ii) Bi-axial tension: Hydrostatic compression: Pressurized tank (photo courtesy P.M. Anderson) s q > 0 Fish under water (photo courtesy P.M. Anderson) s z > 0 s < 0 h Chapter 6-7

8 Tensile strain: e = d L o Engineering Strain w o d /2 L o Lateral strain: - d e L = L w o Shear strain: q x d L /2 g = x/y = tan q y 90º 90º - q Strain is always dimensionless. Adapted from Fig. 6.1(a) and (c), Callister & Rethwisch 8e. Chapter 6-8

9 Typical tensile test machine Stress-Strain Testing Typical tensile specimen extensometer specimen Adapted from Fig. 6.2, Callister & Rethwisch 8e. gauge length 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.) Chapter 6-9

10 Linear Elastic Properties Modulus of Elasticity, E: (also known as Young's modulus) Hooke's Law: s = E e s F E Linearelastic e F simple tension test Chapter 6-10

11 Poisson's ratio, n Poisson's ratio, n: e L e n = - L e e metals: n ~ 0.33 ceramics: n ~ 0.25 polymers: n ~ n Units: E: [GPa] or [psi] n: dimensionless n > 0.50 density increases n < 0.50 density decreases (voids form) Chapter 6-11

12 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. Chapter 6-12

13 Elastic Shear modulus, G: t = G g Other Elastic Properties t G g M simple torsion test Elastic Bulk modulus, K: P = - K V V o Special relations for isotropic materials: G = E 2(1 + n) K = P K E 3(1-2n) V V o P M P P pressure test: Init. vol =V o. Vol chg. = V Chapter 6-13

14 Young s Moduli: Comparison E(GPa) 10 9 Pa Metals Alloys Tungsten Molybdenum Steel, Ni Tantalum Platinum Cu alloys Zinc, Ti Silver, Gold Aluminum Magnesium, Tin Graphite Ceramics Semicond Diamond Si carbide Al oxide Si nitride <111> Si crystal <100> Glass - soda Concrete G raphite Polymers Composites /fibers Polyester PET PS PC PP HDP E PTF E LDPE Carbon fibers only C FRE( fibers)* A ramid fibers only A FRE( fibers)* Glass fibers only G FRE( fibers)* GFRE* CFRE * G FRE( fibers)* C FRE( fibers) * AFRE( fibers) * Epoxy only Wood( grain) 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. Chapter 6-14

15 Simple tension: A o Useful Linear Elastic Relationships d = FL o E A o F d L = - n Fw o E A o d /2 Simple torsion: a = 2 ML o 4 r o G M = moment a = angle of twist w o L o L o d L /2 2r o Material, geometric, and loading parameters all contribute to deflection. Larger elastic moduli minimize elastic deflection. Chapter 6-15

16 Plastic (Permanent) Deformation (at lower temperatures, i.e. T < T melt /3) Simple tension test: engineering stress, s Elastic+Plastic at larger stress Elastic initially permanent (plastic) after load is removed e p engineering strain, e plastic strain Adapted from Fig. 6.10(a), Callister & Rethwisch 8e. Chapter 6-16

17 Yield Strength, s y Stress at which noticeable plastic deformation has occurred. when e p = s y tensile stress, s s y = yield strength Note: for 2 inch sample e = = z/z z = in e p = engineering strain, e Adapted from Fig. 6.10(a), Callister & Rethwisch 8e. Chapter 6-17

18 since in tension, fracture usually occurs before yield. Hard to measure, in ceramic matrix and epoxy matrix composites, since in tension, fracture usually occurs before yield Yield Strength : Comparison Metals/ Alloys Steel (4140) qt Graphite/ Ceramics/ Semicond Polymers Composites/ fibers Yield strength, s y (MPa) Ti (5Al-2.5Sn) W (pure) a Cu (71500) Mo (pure) cw Steel (4140) a Steel (1020) cd Al (6061) ag Steel (1020) hr Ti (pure) Ta (pure) a Cu (71500) hr Al (6061) a Hard to measure, PC Nylon 6,6 PET humid PVC PP H DPE dry 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 Tin (pure) LDPE Chapter 6-18

19 VMSE: Virtual Tensile Testing Chapter 6-19

20 engineering stress Tensile Strength, TS Maximum stress on engineering stress-strain curve. TS s y Adapted from Fig. 6.11, Callister & Rethwisch 8e. F = fracture or ultimate strength Typical response of a metal strain engineering strain Neck acts as stress concentrator Metals: occurs when noticeable necking starts. Polymers: occurs when polymer backbone chains are aligned and about to break. Chapter 6-20

21 Tensile strength, TS (MPa) Tensile Strength: Comparison Metals/ Alloys Steel (4140) qt W (pure) Ti (5Al-2.5Sn) Steel (4140) a a Cu (71500) Cu (71500) hr cw Steel (1020) Al (6061) Ti (pure) ag a Ta (pure) Al (6061) a Graphite/ Ceramics/ Semicond Diamond Si nitride Al oxide Si crystal <100> Glass-soda Concrete Graphite Polymers Nylon 6,6 PC PET PVC PP L DPE H DPE Composites/ fibers C fibers Aramid fib E-glass fib A FRE ( fiber) GFRE ( fiber) C FRE ( fiber) wood( fiber) GFRE ( fiber) C FRE ( fiber) A FRE( fiber) wood ( fiber) 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. Chapter 6-21

22 Ductility Plastic tensile strain at failure: E ngineering tensile stress, s Adapted from Fig. 6.13, Callister & Rethwisch 8e. smaller %EL larger %EL % EL = L o L f - L o A o L o A f x 100 L f Engineering tensile strain, e Another ductility measure: A A % RA = f x 100 A o - o Chapter 6-22

23 Toughness Energy to break a unit volume of material Approximate by the area under the stress-strain curve. E ngineering tensile stress, s Adapted from Fig. 6.13, Callister & Rethwisch 8e. small toughness (ceramics) large toughness (metals) very small toughness (unreinforced polymers) Engineering tensile strain, e Brittle fracture: elastic energy Ductile fracture: elastic + plastic energy Chapter 6-23

24 Resilience, U r Ability of a material to store energy Energy stored best in elastic region U = e r 0 y sde If we assume a linear stress-strain curve this simplifies to U 1 2 s y e y Adapted from Fig. 6.15, Callister & Rethwisch 8e. Chapter 6-24

25 Stress Elastic Strain Recovery s yi D s yo 2. Unload 1. Load 3. Reapply load Strain Adapted from Fig. 6.17, Callister & Rethwisch 8e. Elastic strain recovery Chapter 6-25

26 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. most plastics brasses Al alloys easy to machine steels file hard cutting tools nitrided steels diamond increasing hardness Chapter 6-26

27 Rockwell Hardness: Measurement No major sample damage Each scale runs to 130 but only useful in range 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 Chapter 6-27

28 Hardness: Measurement Table 6.5 Chapter 6-28

29 True Stress & Strain Note: S.A. changes when sample stretched True stress True strain st = F A i e = ln T i o s e T T = s 1+ e = ln 1+ e Adapted from Fig. 6.16, Callister & Rethwisch 8e. Chapter 6-29

30 Hardening An increase in s y due to plastic deformation. s s y 1 s y 0 large hardening small hardening Curve fit to the stress-strain response: s T = K e n T hardening exponent: n = 0.15 (some steels) to n = 0.5 (some coppers) true stress (F/A) true strain: ln(l/l o ) e Chapter 6-30

31 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 x = n x n n n Standard Deviation s = x i - x 2 n -1 where n is the number of data points 1 2 Chapter 6-31

32 Design or Safety Factors Design uncertainties mean we do not push the limit. Factor of safety, N s working = s y 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. s 220,000N d 2 / 4 working 5 = s y N d = m = 6.7 cm 1045 plain carbon steel: s y = 310 MPa TS = 565 MPa F = 220,000N d Chapter 6-32 L o

33 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 s y. Toughness: The energy needed to break a unit volume of material. Ductility: The plastic strain at failure. Chapter 6-33

34 ANNOUNCEMENTS Reading: Core Problems: Self-help Problems: Chapter 6-34