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Materials Science Regina Zibuck [email protected] Please note This presentation was given at a 2012-2013 workshop. Be sure to refer to the 2013-2014 event rules for any changes.
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Page 1: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Materials Science

Regina Zibuck

[email protected]

Please note – This presentation was given at a 2012-2013

workshop. Be sure to refer to the 2013-2014 event rules

for any changes.

Page 2: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Disclaimer

• I am not the event supervisor

• I do not know what the event supervisor will cover

• I am not a Materials Chemist

• I am an Organic Chemist

Page 3: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Properties of Materials (Materials Chemistry)

• Evaluating the intermolecular forces of materials

– Crystal structure

• Ionic, covalent, crystalline, semi-crystalline, amorphous

• Cubic – FCC, BCC, HCP, simple cubic

– Surface chemistry

• Surface tension

• Contact angle

• Thickness of a molecule or film

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Properties of Materials (Materials Chemistry)

• Evaluating the mechanical performance of materials

– Visual

– Stiffness

– Yield strength

– Surface area/volume ratio

– Creep rate

– Viscosity

Page 5: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Resources

• soinc.org

• AP Chem textbook, chapters on bonding, liquids and solids

• Materials Science textbook

• http://www.uwstout.edu/chemistry/scienceolympiad.cfm

• The internet, search key words

Page 6: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

6

Types of Materials • Metals:

– Strong, ductile

– High thermal & electrical conductivity

– Opaque, reflective.

• Polymers/plastics: Covalent bonding sharing of e’s

– Soft, ductile, low strength, low density

– Thermal & electrical insulators

– Optically translucent or transparent.

• Ceramics: ionic bonding (refractory) – compounds of metallic & non-metallic elements (oxides, carbides, nitrides, sulfides)

– Brittle, glassy, elastic

– Non-conducting (insulators)

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7

1. Pick Application Determine required Properties

Processing: changes structure and overall shape ex: casting, sintering, vapor deposition, doping forming, joining, annealing.

Properties: mechanical, electrical, thermal, magnetic, optical, deteriorative.

Material: structure, composition.

2. Properties Identify candidate Material(s)

3. Material Identify required Processing

The Materials Selection Process

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8

ELECTRICAL • Electrical Resistivity of Copper:

• Adding “impurity” atoms to Cu increases resistivity.

• Deforming Cu increases resistivity.

Adapted from Fig. 18.8, Callister & Rethwisch 8e. (Fig. 18.8 adapted from: J.O. Linde, Ann Physik 5, 219 (1932); and C.A. Wert and R.M. Thomson, Physics of Solids, 2nd edition, McGraw-Hill Company, New York, 1970.)

T (ºC) -200 -100 0

1

2

3

4

5

6

Res

isti

vity

, r

(10

-8 O

hm

-m)

0

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9

THERMAL • Space Shuttle Tiles:

-- Silica fiber insulation offers low heat conduction.

• Thermal Conductivity

of Copper: -- It decreases when you add zinc!

Adapted from Fig. 19.4W, Callister 6e. (Courtesy of Lockheed Aerospace Ceramics Systems, Sunnyvale, CA) (Note: "W" denotes fig. is on CD-ROM.)

Adapted from Fig. 19.4, Callister & Rethwisch 8e. (Fig. 19.4 is adapted from Metals Handbook: Properties and Selection: Nonferrous alloys and Pure Metals, Vol. 2, 9th ed., H. Baker, (Managing Editor), American Society for Metals, 1979, p. 315.)

Composition (wt% Zinc) Th

erm

al C

on

du

ctiv

ity

(W

/m-K

)

400

300

200

100

0 0 10 20 30 40

100 mm

Adapted from chapter-opening photograph, Chapter 17, Callister & Rethwisch 3e. (Courtesy of Lockheed Missiles and Space Company, Inc.)

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10

MAGNETIC • Magnetic Permeability

vs. Composition:

-- Adding 3 atomic % Si makes Fe a better recording medium!

Adapted from C.R. Barrett, W.D. Nix, and A.S. Tetelman, The Principles of Engineering Materials, Fig. 1-7(a), p. 9, 1973. Electronically reproduced by permission of Pearson Education, Inc., Upper Saddle River, New Jersey.

Fig. 20.23, Callister & Rethwisch 8e.

• Magnetic Storage:

-- Recording medium is magnetized by recording head.

Magnetic Field M

agn

etiz

atio

n

Fe+3%Si

Fe

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11

• Transmittance:

-- Aluminum oxide may be transparent, translucent, or opaque depending on the material structure.

Adapted from Fig. 1.2, Callister & Rethwisch 8e. (Specimen preparation, P.A. Lessing; photo by S. Tanner.)

single crystal polycrystal: low porosity

polycrystal: high porosity

OPTICAL

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12

DETERIORATIVE • Stress & Saltwater...

-- causes cracks!

Adapted from chapter-opening photograph, Chapter 16, Callister & Rethwisch 3e. (from Marine Corrosion, Causes, and Prevention, John Wiley and Sons, Inc., 1975.) 4 mm -- material:

7150-T651 Al "alloy" (Zn,Cu,Mg,Zr)

Adapted from Fig. 11.26, Callister & Rethwisch 8e. (Provided courtesy of G.H. Narayanan and A.G. Miller, Boeing Commercial Airplane Company.)

• Heat treatment: slows crack speed in salt water!

Adapted from Fig. 11.20(b), R.W. Hertzberg, "Deformation and Fracture Mechanics of Engineering Materials" (4th ed.), p. 505, John Wiley and Sons, 1996. (Original source: Markus O. Speidel, Brown Boveri Co.)

“held at 160ºC for 1 hr before testing”

increasing load crac

k sp

ee

d (

m/s

) “as-is”

10 -10

10 -8

Alloy 7178 tested in saturated aqueous NaCl solution at 23ºC

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13

• Occurs between + and - ions.

• Requires electron transfer.

• Large difference in electronegativity required.

• Example: NaCl

Ionic Bonding

Na (metal)

unstable

Cl (nonmetal)

unstable

electron

+ - Coulombic

Attraction

Na (cation)

stable

Cl (anion)

stable

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14

Ionic Bonding • Energy – minimum energy most stable

– Energy balance of attractive and repulsive terms

Attractive energy EA

Net energy EN

Repulsive energy ER

Interatomic separation r

r A

n r B

EN = EA + ER = + -

Adapted from Fig. 2.8(b), Callister & Rethwisch 8e.

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15

C: has 4 valence e-, needs 4 more

H: has 1 valence e-, needs 1 more

Electronegativities are comparable.

Adapted from Fig. 2.10, Callister & Rethwisch 8e.

Covalent Bonding • similar electronegativity - share electrons

• bonds determined by valence – s & p orbitals dominate bonding

• Example: CH4

shared electrons from carbon atom

shared electrons from hydrogen atoms

H

H

H

H

C

CH 4

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16

• atoms pack in periodic, 3D arrays

Crystalline materials...

-metals -many ceramics

-some polymers

• atoms have no periodic packing

Noncrystalline materials...

-complex structures

-rapid cooling

crystalline SiO2

noncrystalline SiO2 "Amorphous" = Noncrystalline Adapted from Fig. 3.23(b), Callister & Rethwisch 8e.

Adapted from Fig. 3.23(a), Callister & Rethwisch 8e.

Materials and Packing

Si Oxygen

• typical of:

• occurs for:

Page 17: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

17

Metallic Crystal Structures

• How can we stack metal atoms to minimize empty space?

2-dimensions

vs.

Now stack these 2-D layers to make 3-D structures

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18

• Tend to be densely packed.

• Reasons for dense packing:

- Typically, only one element is present, so all atomic radii are the same. - Metallic bonding is not directional. - Nearest neighbor distances tend to be small in order to lower bond energy. - Electron cloud shields cores from each other

• Have the simplest crystal structures.

We will examine three such structures...

Metallic Crystal Structures

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19

• Rare due to low packing density (only Po has this structure) • Close-packed directions are cube edges.

• Coordination # = 6 (# nearest neighbors)

Simple Cubic Structure (SC)

(Courtesy P.M. Anderson)

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20

• APF for a simple cubic structure = 0.52

APF =

a 3

4

3 p (0.5a) 3

1

atoms

unit cell

atom

volume

unit cell

volume

Atomic Packing Factor (APF)

APF = Volume of atoms in unit cell*

Volume of unit cell

*assume hard spheres

Adapted from Fig. 3.24, Callister & Rethwisch 8e.

close-packed directions

a

R=0.5a

contains 8 x 1/8 = 1 atom/unit cell

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21

• Coordination # = 8

Adapted from Fig. 3.2, Callister & Rethwisch 8e.

• Atoms touch each other along cube diagonals.

--Note: All atoms are identical; the center atom is shaded differently only for ease of viewing.

Body Centered Cubic Structure (BCC)

ex: Cr, W, Fe (), Tantalum, Molybdenum

2 atoms/unit cell: 1 center + 8 corners x 1/8 (Courtesy P.M. Anderson)

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22

Atomic Packing Factor: BCC

a

APF =

4

3 p ( 3 a/4 ) 3

2

atoms

unit cell atom

volume

a 3

unit cell

volume

length = 4R =

Close-packed directions:

3 a

• APF for a body-centered cubic structure = 0.68

a R Adapted from

Fig. 3.2(a), Callister & Rethwisch 8e.

a 2

a 3

Page 23: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

23

• Coordination # = 12

Adapted from Fig. 3.1, Callister & Rethwisch 8e.

• Atoms touch each other along face diagonals.

--Note: All atoms are identical; the face-centered atoms are shaded differently only for ease of viewing.

Face Centered Cubic Structure (FCC)

ex: Al, Cu, Au, Pb, Ni, Pt, Ag

4 atoms/unit cell: 6 face x 1/2 + 8 corners x 1/8 (Courtesy P.M. Anderson)

Page 24: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

24

• APF for a face-centered cubic structure = 0.74

Atomic Packing Factor: FCC

maximum achievable APF

APF =

4

3 p ( 2 a/4 ) 3

4

atoms

unit cell atom

volume

a 3

unit cell

volume

Close-packed directions:

length = 4R = 2 a

Unit cell contains:

6 x 1/2 + 8 x 1/8

= 4 atoms/unit cell a

2 a

Adapted from Fig. 3.1(a), Callister & Rethwisch 8e.

Page 25: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

25

A sites

B B

B

B B

B B

C sites

C C

C A

B

B sites

• ABCABC... Stacking Sequence • 2D Projection

• FCC Unit Cell

FCC Stacking Sequence

B B

B

B B

B B

B sites

C C

C A

C C

C A

A

B C

Page 26: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

26

• Coordination # = 12

• ABAB... Stacking Sequence

• APF = 0.74

• 3D Projection • 2D Projection

Adapted from Fig. 3.3(a), Callister & Rethwisch 8e.

Hexagonal Close-Packed Structure (HCP)

6 atoms/unit cell

ex: Cd, Mg, Ti, Zn

• c/a = 1.633

c

a

A sites

B sites

A sites Bottom layer

Middle layer

Top layer

Page 27: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

27

Theoretical Density, r

where n = number of atoms/unit cell A = atomic weight VC = Volume of unit cell = a3 for cubic NA = Avogadro’s number = 6.022 x 1023 atoms/mol

Density = r =

VC NA

n A r =

Cell Unit of Volume Total

Cell Unit in Atoms of Mass

Page 28: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

28

• Ex: Cr (BCC)

A = 52.00 g/mol

R = 0.125 nm

n = 2 atoms/unit cell

rtheoretical

a = 4R/ 3 = 0.2887 nm

ractual

a R

r = a3

52.00 2

atoms

unit cell mol

g

unit cell

volume atoms

mol

6.022 x 1023

Theoretical Density, r

= 7.18 g/cm3

= 7.19 g/cm3

Adapted from Fig. 3.2(a), Callister & Rethwisch 8e.

Page 29: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

29

Densities of Material Classes r

metals > r ceramics > r

polymers

Why?

Data from Table B.1, Callister & Rethwisch, 8e.

r (

g/c

m )

3

Graphite/ Ceramics/ Semicond

Metals/ Alloys

Composites/ fibers

Polymers

1

2

2 0

30 B ased on data in Table B1, Callister

*GFRE, CFRE, & AFRE are Glass, Carbon, & Aramid Fiber-Reinforced Epoxy composites (values based on

60% volume fraction of aligned fibers in an epoxy matrix). 10

3

4

5

0.3

0.4 0.5

Magnesium

Aluminum

Steels

Titanium

Cu,Ni

Tin, Zinc

Silver, Mo

Tantalum Gold, W Platinum

G raphite

Silicon

Glass - soda Concrete

Si nitride Diamond Al oxide

Zirconia

H DPE, PS PP, LDPE

PC

PTFE

PET PVC Silicone

Wood

AFRE *

CFRE *

GFRE*

Glass fibers

Carbon fibers

A ramid fibers

Metals have... • close-packing (metallic bonding) • often large atomic masses

Ceramics have... • less dense packing • often lighter elements

Polymers have... • low packing density (often amorphous) • lighter elements (C,H,O)

Composites have... • intermediate values

In general

Page 30: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Surface Chemistry

• Surface tension

• Contact angle

• Thickness of a molecule

Page 31: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Surface Tension

• A molecule in the interior of a liquid is attracted by the molecules surrounding it

Page 32: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)
Page 33: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Surface Tension

• Try to float a tack on water

• Add a drop of soap

Page 34: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Contact Angle

• The contact angle is the angle measured where a liquid interface meets a solid surface.

Page 35: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)
Page 36: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Material Performance and Characterization

• Visual

• Stiffness

• Yield strength

• Surface area/volume ratio

• Creep rate

• Viscosity

Page 37: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

37

Microscopic Examination

• Crystallites (grains) and grain boundaries. Vary considerably in size. Can be quite large.

– ex: Large single crystal of quartz or diamond or Si

– ex: Aluminum light post or garbage can - see the individual grains

• Crystallites (grains) can be quite small (mm or less) – necessary to observe with a microscope.

Page 38: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

38

• Useful up to 2000X magnification. • Polishing removes surface features (e.g., scratches) • Etching changes reflectance, depending on crystal orientation.

Micrograph of brass (a Cu-Zn alloy)

0.75mm

Optical Microscopy

Adapted from Fig. 4.13(b) and (c), Callister & Rethwisch 8e. (Fig. 4.13(c) is courtesy of J.E. Burke, General Electric Co.)

crystallographic planes

Page 39: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

39

Grain boundaries...

• are imperfections, • are more susceptible to etching, • may be revealed as dark lines, • change in crystal orientation across boundary.

Adapted from Fig. 4.14(a) and (b), Callister & Rethwisch 8e. (Fig. 4.14(b) is courtesy of L.C. Smith and C. Brady, the National Bureau of Standards, Washington, DC [now the National Institute of Standards and Technology, Gaithersburg, MD].)

Optical Microscopy

ASTM grain size number

N = 2 n -1

number of grains/in2 at 100x magnification

Fe-Cr alloy

(b)

grain boundary

surface groove

polished surface

(a)

Page 40: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

Unetched Steel 200 X

Etched Steel 200 X

Unetched Brass 200 X

Etched Brass 200 X

Page 41: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

41

Optical Microscopy

• Polarized light

– metallographic scopes often use polarized light to increase contrast

– Also used for transparent samples such as polymers

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42

Microscopy Optical resolution ca. 10-7 m = 0.1 mm = 100 nm

For higher resolution need higher frequency

– X-Rays? Difficult to focus.

– Electrons

• wavelengths ca. 3 pm (0.003 nm) – (Magnification - 1,000,000X)

• Atomic resolution possible

• Electron beam focused by magnetic lenses.

Page 43: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

43

• Atoms can be arranged and imaged!

Carbon monoxide molecules arranged on

a platinum (111) surface.

Photos produced from the work of C.P. Lutz, Zeppenfeld, and D.M. Eigler. Reprinted with permission from International Business Machines Corporation, copyright 1995.

Iron atoms arranged on a copper (111) surface. These Kanji characters

represent the word “atom”.

Scanning Tunneling Microscopy (STM)

Page 44: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

44

X-Ray Diffraction

• Diffraction gratings must have spacings comparable to the wavelength of diffracted radiation.

• Can’t resolve spacings

• Spacing is the distance between parallel planes of atoms.

Page 45: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

45

X-Rays to Determine Crystal Structure

X-ray intensity (from detector)

q

q c

d = n

2 sin q c

Measurement of critical angle, qc, allows computation of planar spacing, d.

• Incoming X-rays diffract from crystal planes.

Adapted from Fig. 3.20, Callister & Rethwisch 8e.

reflections must be in phase for a detectable signal

spacing between planes

d

q

q extra distance travelled by wave “2”

Page 46: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

46

Elastic means reversible!

Elastic Deformation 2. Small load

F

d

bonds stretch

1. Initial 3. Unload

return to initial

F

d

Linear- elastic

Non-Linear- elastic

Page 47: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

47

Plastic means permanent!

Plastic Deformation (Metals)

F

d

linear elastic

linear elastic

d plastic

1. Initial 2. Small load 3. Unload

planes

still

sheared

F

d elastic + plastic

bonds

stretch

& planes

shear

d plastic

Page 48: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

48

Stress has units: N/m2 or lbf /in2

Engineering Stress • Shear stress, t:

Area, Ao

F t

F t

F s

F

F

F s

t = F s

A o

• Tensile stress, s:

original area before loading

s = F t

A o 2 f

2 m

N or

in

lb =

Area, Ao

F t

F t

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49

• Simple tension: cable

Note: t = M/AcR here.

Common States of Stress

o

s = F

A

o

t = F s

A

s s

M

M A o

2R

F s A c

• Torsion (a form of shear): drive shaft Ski lift (photo courtesy

P.M. Anderson)

A o = cross sectional

area (when unloaded)

F F

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50

(photo courtesy P.M. Anderson) Canyon Bridge, Los Alamos, NM

o

s = F

A

• Simple compression:

Note: compressive structure member (s < 0 here). (photo courtesy P.M. Anderson)

OTHER COMMON STRESS STATES

A o

Balanced Rock, Arches National Park

Page 51: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

51

• Tensile strain: • Lateral strain:

Strain is always dimensionless.

Engineering Strain

• Shear strain:

q

90º

90º - q y

x q g = x/y = tan

e = d

L o

Adapted from Fig. 6.1(a) and (c), Callister & Rethwisch 8e.

d /2

L o w o

- d e L = L

w o

d L /2

Page 52: Types of Materials Sci workshop.pdf–ex: Large single crystal of quartz or diamond or Si –ex: Aluminum light post or garbage can - see the individual grains •Crystallites (grains)

52

Stress-Strain Testing • Typical tensile test machine

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.)

specimen extensometer

• Typical tensile specimen

Adapted from Fig. 6.2, Callister & Rethwisch 8e.

gauge length

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53

Linear Elastic Properties

• Modulus of Elasticity, E: (also known as Young's modulus) Stress is proportional to strain; the ratio is constant Always the same for a given material As you apply load to a material, the strain increases constantly (or proportionately) with stress.

Hooke's Law:

s = E e s

Linear-

elastic

E

e

F

F simple tension test

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Young’s Modulus

• http://www.matter.org.uk/schools/content/youngmodulus/default.htm

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Example: In a tension test you apply a gradually increasing load to a sample. You can determine the amount of strain (e that occurs in a sample at any given stress level (s.

s (ksi) e (in/in x 0.001) 0 0 3 1 6 2 9 3 12 4

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S

tre

ss ,s

(ksi)

Strain ,e (in/in x 0.001)

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Knowing E for a given material and : E = s/e

1.) We can find how much stress is in the

material if we know the strain:

s = Ee

2.) We can find how much strain is in the material if we know the stress:

e= s E

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• If the tension test continues, the stress will reach a level called the Proportional Limit ( sPL ). If the stress is increased above sPL , the strain will increase at a higher rate.

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S

tre

ss (

s),

ksi

Strain (e), in/in

sPL

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60

Metals Alloys

Graphite Ceramics Semicond

Polymers Composites

/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.

Young’s Moduli: Comparison

109 Pa

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

2 0

4 0

6 0 8 0

10 0

2 00

6 00 8 00

10 00 1200

4 00

Tin

Cu alloys

Tungsten

<100>

<111>

Si carbide

Diamond

PTF E

HDP E

LDPE

PP

Polyester

PS PET

C FRE( fibers) *

G FRE( fibers)*

G FRE(|| fibers)*

A FRE(|| fibers)*

C FRE(|| fibers)*

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61

• Stress at which noticeable plastic deformation has occurred.

when ep = 0.002

Yield Strength, sy

sy = yield strength

Note: for 2 inch sample

e = 0.002 = z/z

z = 0.004 in

Adapted from Fig. 6.10(a), Callister & Rethwisch 8e.

tensile stress, s

engineering strain, e

sy

ep = 0.002

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62

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

Yield Strength : Comparison Graphite/ Ceramics/ Semicond

Metals/ Alloys

Composites/ fibers

Polymers

Yiel

d s

tren

gth

,

s y

(MPa

)

PVC

Har

d t

o m

easu

re

,

sin

ce in

ten

sio

n, f

ract

ure

usu

ally

occ

urs

bef

ore

yie

ld.

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

Al (6061) ag

Cu (71500) hr Ta (pure) Ti (pure) a Steel (1020) hr

Steel (1020) cd Steel (4140) a

Steel (4140) qt

Ti (5Al-2.5Sn) a W (pure)

Mo (pure) Cu (71500) cw

Har

d t

o m

easu

re,

in c

eram

ic m

atri

x an

d e

po

xy m

atri

x co

mp

osi

tes,

sin

ce

in t

ensi

on

, fra

ctu

re u

sual

ly o

ccu

rs b

efo

re y

ield

.

H DPE PP

humid

dry

PC

PET

¨

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Surface Area/Volume Ratio

• The amount of surface area per unit volume of an object

• For a given shape, SA:V is inversely proportional to size

• Material with a large surface area to volume ratio reacts at a much faster rate than monolithic materials

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Surface Area/Volume Ratio

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65

Creep Sample deformation at a constant stress (s) vs. time

Adapted from

Fig. 8.28, Callister &

Rethwisch 8e.

Primary Creep: slope (creep rate)

decreases with time.

Secondary Creep: steady-state

i.e., constant slope (e/t).

Tertiary Creep: slope (creep rate)

increases with time, i.e. acceleration of rate.

s s,e

0 t

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66

• Occurs at elevated temperature, T > 0.4 Tm (in K)

Adapted from Fig. 8.29,

Callister & Rethwisch 8e.

Creep: Temperature Dependence

elastic

primary secondary

tertiary

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67

Secondary Creep • Strain rate is constant at a given T, s

-- strain hardening is balanced by recovery

stress exponent (material parameter)

strain rate

activation energy for creep

(material parameter)

applied stress material const.

• Strain rate

increases

with increasing

T, s

10

2 0

4 0

10 0

2 0 0

10 -2 10 -1 1 Steady state creep rate (%/1000hr) e

s

Str

ess (

MP

a) 427ºC

538ºC

649ºC

Adapted from

Fig. 8.31, Callister 7e.

(Fig. 8.31 is from Metals

Handbook: Properties

and Selection:

Stainless Steels, Tool

Materials, and Special

Purpose Metals, Vol. 3,

9th ed., D. Benjamin

(Senior Ed.), American

Society for Metals,

1980, p. 131.)

-s=e

RT

QK cn

s exp2

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Creep Failure • Failure: along grain boundaries.

applied

stress

g.b. cavities

From V.J. Colangelo and F.A. Heiser, Analysis of

Metallurgical Failures (2nd ed.), Fig. 4.32, p. 87, John

Wiley and Sons, Inc., 1987. (Orig. source: Pergamon

Press, Inc.)

68

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Viscosity

• Resistance offered by a fluid due to the attraction of the molecules to each other

• Measure the time required for a constant volume of liquid to drain from a pipet

• http://chemmovies.unl.edu/chemistry/smallscale/SS070.html


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