slides on composites

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1 MSE 280: Introduction to Engineering Materials I dd Reading: Callister Ch. 15 Composites Issues to address… What are composites? Classification of composites. Why composites? MSE280 © 2007, 2008 Moonsub Shim 1 Mechanical properties of composites. • Applications. Composites: definition & examples - Multiphase materials with chemically different phases and distinct interfaces. - Properties of the resultant combination of materials are - Properties of the resultant combination of materials are superior to the properties of the individual components. - Advantages: High-strength/light-weight, low cost, environmentally resistant… - Natural composites: -Wood: strong & flexible cellulose fibers in stiffer lignin (surrounds the fibers). B t bt ft ll ( ti) ithi h d b t b ittl tit MSE280 © 2007, 2008 Moonsub Shim 2 -Bone: strong but soft collagen (protein) within hard but brittle apatite (mineral). -Certain types of rocks can also be considered as composites. -Synthetic composites: fiberglass, concrete, carbon-carbon composites….

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1

MSE 280: Introduction to Engineering Materials

I ddReading: Callister Ch. 15

CompositesIssues to address… • What are composites?• Classification of composites.• Why composites?

MSE280© 2007, 2008 Moonsub Shim1

• Mechanical properties of composites.• Applications.

Composites: definition & examples- Multiphase materials with chemically different phases and distinct interfaces.

- Properties of the resultant combination of materials are- Properties of the resultant combination of materials are superior to the properties of the individual components.

- Advantages: High-strength/light-weight, low cost, environmentally resistant…

- Natural composites:-Wood: strong & flexible cellulose fibers in stiffer lignin (surrounds the fibers).B t b t ft ll ( t i ) ithi h d b t b ittl tit

MSE280© 2007, 2008 Moonsub Shim2

-Bone: strong but soft collagen (protein) within hard but brittle apatite (mineral).-Certain types of rocks can also be considered as composites.

-Synthetic composites: fiberglass, concrete, carbon-carbon composites….

2

Bicycle forksBraided and

High Strength

unidirectional S-2 Glass and carbon fibers are used to produce forks with different stiffness

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High StrengthWeight ReductionDesign FlexibilityCost Performance

From http://matse101.mse.uiuc.edu/

Lightweight - low density

Pole-vaultingg t e g t o de s ty

Buckling resistance - stiffness Strong - yield strength Minimal twisting Cost

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Glass fiber web/epoxy Glass fiber ringsLongitudinal carbon fibers/epoxy

From http://matse101.mse.uiuc.edu/

3

Boeing 757-200Rudder (graphite) Fixed trailing edge

panels graphiteFlap support fairings Fwd segment (graphite/Kevlar

Aft flaps Outboard (graphite) Inboard (graphite/fiberglass)

Fixed trailing edge panels Graphite/Kevlar + non-woven

Fixed trailing edge panels upper (graphite /fiberglass), lower (graphite /Kevlar + non-woven Kevlar mat)

Elevators (graphite)

Auxiliary power inlet

graphiteEnvironmental control system ducts (Kevlar)

Engine strut fairings (Kevlar/fiberglass)

Ailerons (graphite)

Tip fairings (fiberglass)

panels graphite /Kevlar + non-woven Kevlar mat)

Fwd segment (graphite/Kevlar + non-woven Kevlar mat Aft segment (graphite/fiberglass)

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Wing leading edge lower panel Kevlar/fiberglass

Kevlar matSpoilers (graphite)

Cowl components (graphite)

Body main landing gear doors (graphite) Trunnion fairings and wing landing gear doors (graphite/Kevlar) Brakes( structural carbon)

Wing to body fairings (graphite/Kevlar/Fiberglass and Graphite/Kevlar + non-woven Kevlar mat

Nose landing gear doors (graphite)

From http://matse101.mse.uiuc.edu/

Terminology• Matrix:

– softer, more flexible and continuous part that surrounds the other phase.– transfer stress to other phases– protect phases from environment

• Reinforcement (dispersed phase):– stiffer, high strength part (particles or fibers are the most common).– enhances matrix properties

C fibers: very stiff very strongC matrix:

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fibers lie in plane

view onto plane

C matrix: less stiff less strong

4

Composite characteristicsDepends on:

- properties of the matrixconcentration size shapeproperties of the matrix

material.

- properties of reinforcement material.

- ratio of matrix to reinforcement. distribution

orientation

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- matrix-reinforcement bonding/adhesion.

- mode of fabrication.

Classification of Composites• Matrix-based:

– Metal Matrix Composites (MMC)Metal Matrix Composites (MMC) – Ceramic Matrix Composites (CMC)– Polymer Matrix Composites (PMC)

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5

• CMCs: Increased toughness • PMCs: Increased E/ρ

E(GPa)10 210 3

PMCs

ceramicsparticle-reinf

Force

COMPOSITE BENEFITS

10-46061 Al1

G=3E/8K=E

Density, ρ [Mg/m 3].1 .3 1 3 10 30

.01.1

110

10metal/ metal alloys

polymers

fiber -reinf

un-reinf

Bend d isplacement

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• MMCs:Increasedcreepresistance

20 30 50 10 0 20010-10

10-8

10-66061 Al

6061 Al w/SiC whiskers σ(MPa)

εss (s -1 )Adapted from T.G. Nieh, "Creep rupture of a silicon-carbide reinforced aluminum composite", Metall. Trans. A Vol. 15(1), pp. 139-146, 1984. Used with permission.

From Callister resources CD

Reinforcement-based

dparticle>100nm

dparticle< 100nm

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6

Particle-reinforced Fiber -reinforced Structural• Examples:

-Spheroidite matrix: particles: Adapted from Fig.

COMPOSITE SURVEY: Particle-I

p steel ferrite ( α)

(ductile)cementite(Fe 3C) (brittle)

-WC/Co cemented carbide

matrix: cobalt (ductile)

particles: WC (brittle, hard)

60 μm

Vm:

10.10, Callister 6e. (Fig. 10.10 is copyright United States Steel Corporation, 1971.)

Adapted from Fig. 16.4, Callister 6e. (Fig. 16.4 is courtesy Carboloy Systems, Department, General Electric Company )

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hard)

-Automobile tires

matrix: rubber (compliant)

particles: C (stiffer)

Vm: 10-15vol%! 600 μm

0.75 μm

Electric Company.)

Adapted from Fig. 16.5, Callister 6e. (Fig. 16.5 is courtesy Goodyear Tire and Rubber Company.)

From Callister resources CD

• Elastic modulus, Ec, of composites:two approaches

Fiber -reinforced StructuralParticle-reinforced

COMPOSITE SURVEY: Particle-II

-- two approaches.

Data: Cu matrix w/tungsten particles

15020 025030 0350

E(GPa)

lower limit:1

Ec= Vm

Em+

VpEp

c m m

upper limit:E = V E + VpEp

“rule of mixtures”

Adapted from Fig. 16.3, Callister 6e. (Fig. 16.3 is from R.H. Krock, ASTM Proc, Vol. 63, 1963.)

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• Application to other properties:-- Electrical conductivity, σe: Replace E by σe.-- Thermal conductivity, k: Replace E by k.

0 20 40 60 80 10 0 vol% tungsten(Cu) (W)

From Callister resources CD

Analogy to resistors in series vs. parallel…

7

Fiber-reinforced composites

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Continuous & aligned

Discontinuous & aligned

Discontinuous & random

Fiber-reinforced compositesThe Fiber Phase

Smaller diameter fiber is stronger than bulk in most materials ( i ll b i l ) Wh ?(especially brittle ones). Why? Flaws!

Whiskers:• very thin single crystals that have extremely large aspect ratios.• high degree of crystallinity and virtually flaw free – exceptionally high strength.• usually extremely expensive.• some whisker materials: graphite, SiC, silicon nitride, aluminum oxide.Fibers:

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Fibers:• polycrystalline or amorphous.• typically: polymers or ceramics (polymer aramids, glass, carbon, boron, SiC…Fine Wires:• relatively large diameter, often metal wires.• e.g. steel, molybdenum, tungsten…

8

Fiber-reinforced compositesThe Matrix Phase• can be metal polymers or ceramics• can be metal, polymers, or ceramics.

• typically metals and polymer because some ductility is often desired.

• main functions of the matrix:

-Hold fibers together.

-Transmit and distribute external stress to the fibers.

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-Protect fibers from surface damage: abrasions, chemical reactions…

• in CMCs, reinforcements are usually added to improve fracture toughness .

Fiber-reinforced composites

1. Molecular entanglement (interdiffusion):• Entanglement of molecules at the interface.

The Fiber-Matrix Interface

Entanglement of molecules at the interface.• Especially important in fibers that are pre-

coated with polymers.• Molecular conformation/structural and

chemical aspects.2. Electrostatic attraction

• Depends on surface charge density.• e.g. glass fibers, polymers with chargeable

groups.3. Covalent bonding

• Usually the strongest fiber matrix

+ + + + + + + - - - - - - -

- - - - - - -+

-

+

-

+

-

+

-

+

-

+

-

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• Usually the strongest fiber-matrix interaction.

• The most important in many composites.4. Mechanical adhesion

• Interlocking of 2 rough surfaces• e.g. thermosetting resins

AB

AB

AB

9

Fiber-reinforced compositesProperties depend on LENGTH and ORIENTATION of the fibers (as well as isolated properties of each of the components)!

*Critical fiber length

c

fc

dl

τσ2

*

==fσ Fiber tensile strength

=d Fiber diameter

=cτ Smaller of:• fiber-matrix bond strength• matrix shear yield strength.

Possible failure modes:

Continuous when fiber length >> lcDiscontinuous when fiber length < 15 lc

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1) fiber breaking.2) matrix breaking.3) fiber pullout (interface between fiber and matrix fails)

Fiber-reinforced composites

σ(x)σ(x)

Short fibersLong fibers

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Poorer fiber efficiency Better fiber efficiency

10

Aligned fibers

Elastic Modulus

Continuous when fiber length >> lcDiscontinuous when fiber length < 15 lc

Not so detrimental since:1) Not all fibers fail at the same time2) Matrix still intact

E

0o

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0o 90o

σ

max min

Aligned Continuous fibersFiber-reinforcedParticle-reinforced Structural

COMPOSITE SURVEY: Fiber-I

• Examples:

fracture surface

matrix: α (Mo) (ductile)

--Metal: γ'(Ni3Al)-α(Mo)by eutectic solidification.

--Glass w/SiC fibersformed by glass slurryEglass = 76GPa; ESiC = 400GPa.

(a)

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From W. Funk and E. Blank, “Creep deformation of Ni3Al-Mo in-situ composites", Metall. Trans. A Vol. 19(4), pp. 987-998, 1988. Used with permission.

surface

fibers: γ’ (Ni3Al) (brittle)

2μm From F.L. Matthews and R.L. Rawlings, Composite Materials; Engineering and Science, Reprint ed., CRC Press, Boca Raton, FL, 2000. (a) Fig. 4.22, p. 145 (photo by J. Davies); (b) Fig. 11.20, p. 349 (micrograph by H.S. Kim, P.S. Rodgers, and R.D. Rawlings). Used with permission of CRCPress, Boca Raton, FL.

(b)

From Callister resources CD

11

Continuous-aligned fibersConsider a composite with fibers having square rod geometry with stress in the longitudinal direction…

fiber

L

B

B

Matrix

b

l

σ σ

When l >> l (typically l > 15 l ) we can simplify to:

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b

When l >> lc (typically l > 15 lc), we can simplify to:

σ σB

l thenl

Ll

Ll

L matrixfibercomposite Δ=

Δ=

Δ

since ,lLΔ

≡ε matrixfibercomposite εεε ==

ISOSTRAIN

Continuous-aligned fibersWhat about elastic modulus? σ σ

B

l

Total force on the composite is simply the sum of

Longitudinal loading

b

fibermatrixcomposite FFF +=Total force on the composite is simply the sum of forces on matrix and fibers:

sinceAF

=σ or , we have: AF σ= ffmmcc AAA σσσ +=

Recall stress-strain relation: εσ E= Sub-in for stresses…

AEAE

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fffmmmccc AEAEAE εεε +=

Imposing isostrain condition ,mfc εεε ==cc

fff

cc

mmmc A

AEA

AEEεε

εε

+=rearrange

c

ff

c

mmc A

AE

AAEE +=

“Area fractions”Prefer volume fractions….

12

Continuous-aligned fibers

σ σB

l

Total area = Bb

Af = number of fibers x area of each fiber = Nb2

Longitudinal loading

bThen we have:

BNb

AA

c

f = Also,

BNb

AA

AAor

AAA

c

f

c

m

fcm

−=−=

−=

11For volume fractions:

lNbV

BblV

f

c2=

=

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Then:c

f

c

ff A

AB

NbBbl

lNbVV

v ====2

same as “area fraction”

c

mm A

Av =Similarly, ffmmcl EvEvE +=Longitudinal elastic modulus(upper bound for Ec)

Continuous-aligned fibers

σ σB

l

?fFWhat about the load on the matrix and the fibers?

Longitudinal loading

b?=m

f

F AF σ=

mm

ff

mm

ff

m

f

vv

AA

FF

σσ

σσ

==

With εσ E=

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mmm

fff

m

f

vEvE

FF

εε

=Isostrain conditions

mm

ff

m

f

vEvE

FF

=

13

Continuous-aligned fibersσ

B

lTransverse loading

Stress, rather than strain, is the same in this case:

b

σ

B

mfc σσσ == ISOSTRESS condition

The total elongation will be the sum of elongation of the components:

mfc LLL Δ+Δ=Δ

mfcc L

LLL

LL Δ

=ε Where Lc = length of the composite along the direction of stress = BStrain =

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ccc LLL along the direction of stress B

Again, to express in terms of volume fractions:

BNb

LL

NbL

c

f

f

=

=

Same as what we derived for volume fraction

fv=Rearrange

f

fc v

LL = Similarly,

m

mc v

LL =

Continuous-aligned fibers

B

lTransverse loading

mfcc L

LLL

LL Δ

b

σ

B

m

mm

f

ff

mm

m

ff

f

LLv

LL

vvL

LvL

L Δ+

Δ=

Δ+

Δ=

//

ccc LLL

fε mε

ffmmc vv εεε +=Lower bound for E

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From stress-strain relation;Eσε =

f

ff

m

mm

c

c

Ev

Ev

Eσσσ

+=

Applying isostress condition and rearranging gives mffm

fmct EvEv

EEE

+=

Lower bound for Ec(transverse modulus)

14

Continuous-aligned fibers

B

lMany properties follow these upper and lower bound relations for continuous-aligned fiber composities.

b

BIn general:

ffmmupperccl vv χχχχ +==

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mffm

fmlowercct vv χχ

χχχχ

+==

Continuous-aligned fibers: example1. Calculate the longitudinal and transverse modulus and

thermal conductivity for polyester reinforced with 60% volume fraction of glass fiber (E-glass).volume fraction of glass fiber (E glass).

2. Calculate longitudinal specific stiffness.

3. Calculate the percentage of the load on the fibers for longitudinal loading.

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E(GPa) K(W/mK) Specific gravity

Polyester 6.3 0.17 1.46

E-glass 72.4 0.97 2.58

15

Continuous-aligned fibers: example Mixed Fibers

• A two-fiber composite (continuous aligned) i d f th f ll i tis composed of the following components.

E(GPa) Vol. fraction

Kevlar fiber 131 30%

E-glass fiber 72.5 20%

Epoxy matrix 2.41 50%

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• Calculate the longitudinal elastic modulus.

Continuous-aligned fibers

B

l

Tensile strengthTensile strengthLongitudinal: *'*

ffl vv σσσ +=

Similar to elastic modulus

bffmmcl vv σσσ +This is assuming that the fiber fails prior to the matrix.

='mσ Stress in the matrix at failure

=*fσ Tensile strength of the reinforcement fiber

Transverse: more complex due to many factors that affect it(e.g. matrix & fiber properties, fiber-matrix bond strength,

presence of voids etc…)

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In general, stronger along longitudinal direction

16

Discontinuous & aligned fibersDiscontinuous when fiber length < 15 lc

If l > lc

mmc

ffcd vl

lv '**

21 σσσ +⎟

⎠⎞

⎜⎝⎛ −= Similar to continuous case,

except for the length factor.

If l < l

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mmfc

cd vvd

l '*' στσ +=

=cτ Smaller of:• fiber-matrix bond strength• matrix shear yield strength.

If l < lc

Discontinuous, random 2D fibers• Example: Carbon-Carbon

--process: fiber/pitch, then

C fibers: very stiff very strong

Discontinuous & random fibers

burn out at up to 2500C.--uses: disk brakes, gas

turbine exhaust flaps, nosecones. fibers lie

in plane

view onto plane

y gC matrix: less stiff less strong

(b)

(a)

Ec = EmVm + KEf Vf

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From Callister resources CD

efficiency factor (depends on vf and Ef/Em):--aligned 1D: K = 1 (anisotropic)--random 2D: K = 3/8 (2D isotropy)--random 3D: K = 1/5 (3D isotropy)

17

Polymer matrix composites• Glass fiber-reinforced

polymer (GFRP) it fib lcomposites: fiberglass

– Some reasons for using glass as fibers:

• Easy to draw fibers from molten state.

• Strength.• Readily available/economic.• Chemical inertness (e.g.

non-corrosive).

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)– Applications: automotive &

marine bodies, storage containers, industrial flooring…

Polymer matrix composites• Carbon fiber-reinforced polymer (CFRP)

composites:composites:– Some reason for using C-fibers:

• Highest specific modulus and specific strength of all reinforcing fiber materials.

• Retain high modulus and TS at elevated T (chemical oxidation may be a problem).

• At or near RT, very inert.• Can engineer specific mechanical and physical properties

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• Can engineer specific mechanical and physical properties.– Some applications: fishing rods, golf clubs, bicycles,

military and commercial aircraft structural components…

18

Polymer matrix composites• Aramid (e.g. Kevlar) fiber-reinforced polymer composites:

– High strength, high modulus.Much better strength to weight than metals– Much better strength-to-weight than metals.

– Stable to relatively high T (high mechanical properties maintained from ~ - 200 to 200oC).

– Relatively inert chemically (except strong acids).– Uses: bullet-proof vests, tires, ropes, missile cases, parts for automotive

brake, clutch lining and gaskets…

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Carbon-carbon composites• Carbon fiber reinforced carbon matrix

composites.p– High modulus & TS (retained to T > 2000oC).– Resistant to creep.– Large fracture toughness.– Small thermal expansion coefficient.– High thermal conductivity.– Uses: rocket motors, friction material for aircraft and

hi h f t bil b k t f

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high-performance automobile brakes, components for turbine engines…

– Very expensive mainly due to relatively complex processing.

19

Carbon nanotube composite

Carbon matrixMaterial Young’s Modulus

Aluminum 72 GPa

1μm

Aluminum alloys

72 GPa

Steel 200 GPa

Tungsten 400 GPa

Carbon Nanotube

>1000 GPa

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Ajayan et al.

Nanotube bundles

Processing of fiber-reinforced composites

Pultrusion

Prepreg production process

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Processing of fiber-reinforced composites

Filament winding

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Design exampleF

Requirements - at F = 890N, deflection < 0.33mm

- Circumferential winding with θ = 15o

A) Which fiber(s), if embedded in epoxy matrix, meet the these criteria?

B) D id th t t ff ti fib

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B) Decide on the most cost-effective fiber.

21

Concepts to remember…• Matrix & reinforcement.• What composite characteristics depend on.

Cl ifi ti t i b d MMC CMC PMC• Classification: matrix-based – MMC, CMC, PMC; reinforcement-based.

• Particle reinforced composites: upper and lower bound for E (rule of mixtures).

• Fiber-reinforced composites– Continuous-aligned, discontinuous-aligned &

discontinuous-random cases.C i i l l h

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– Critical length.– Longitudinal & transverse properties.– Isostrain & isostress cases.

• Structural composites.