Chapter 4c Mechanical Properties. Heat Distortion Temperature The maximum temperature at which a...
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Transcript of Chapter 4c Mechanical Properties. Heat Distortion Temperature The maximum temperature at which a...
Chapter 4c
Mechanical Properties
Heat Distortion Temperature• The maximum temperature at which a polymer can be used in rigid
material applications is called the softening or heat distortion temperature (HDT).
• A typical test (plastic sheeting) involves application of a static load, and heating at a rate of 2oC per min. The HDT is defined as the temperature at which the
• elongation becomes 2%.
• A: Rigid poly(vinyl chloride)
• 50 psi load.
• B: Low-density poly(ethylene)
• 50 psi load.
• C: Poly(styrene-co-acrylonitrile)
• 25 psi load.
• D: Cellulose acetate
• (Plasticized) 25 psi load.
Transient Testing: Resilience of Cured Elastomers
• Resilience tests reflect the ability of
• an elastomeric compound to store
• and return energy at a given• frequency and temperature.
• Change of rebound • resilience (h/ho) with • temperature T for: • 1. cis-poly(isoprene); • 2. poly(isobutylene); • 3. poly(chloroprene); • 4. poly(methyl methacrylate).
Polyethylene33%Vinyls16%Polypropylene15%PMMAABSNylonPolycarbonateSaturated PolyesterPEEKPolyurethaneSome are thermosets as well.PVC
Not Cross-Linked90% of market
ThermoplasticsWill reform when melted
EpoxyMelamine FormaldehydePhenolicPolyester (unsaturated)PolyimidePolyurethaneSome are thermoplastic as well.SiliconeUrea Formaldehyde
Cross-linked10% of market
Thermosets/ElastomersWill not reform
Polymer Family Tree
Types of Polymers
Tensile strengths
Polymers: ~ 10 - 100 MPa
Metals: 100’s - 1000’s MPa
Elongation
Polymers: up to 1000 % in some cases
Metals: < 100%
Moduli (Elastic or Young’s)
Polymers: ~ 10 MPa - 4 GPa
Metals: ~ 50 - 400 GPa
Ballpark Comparisons
Amorphous v Crystalline Polymers Thermo-mechanical properties
Thermal ExpansionIf a part is to be produced within a close dimensional tolerance, careful
consideration of thermal expansion/contraction must be made.
Parts are produced in the melt state, and solidify to amorphous or semi-crystalline states.
Changes in density must
be taken into account
when designing the mold.
Thermal Expansion
Stress Strain Studies
Initial slope is the Young’s Modulus (E’ or sometimes G)TS = tensile strengthy = yield strengthToughness = Energy required to break (area under curve)
/strain
Elongation = 100% x
Anatomy of a Stress Strain Graph
Compression and Shear vs. Tensile TestsStress-strain curves are very dependent on the test method. A modulus
determined under compression is generally higher than one derived from a tensile experiment, as shown below for polystyrene.
Tensile testing is most sensitive
to material flaws and microscopic
cracks.
Compression tests tend to
be characteristic of the polymer,
while tension tests are more
characteristic of sample flaws.
Note also that flexural and shear
test modes are commonly
employed.
Elongation by extension of neck
Chains in neck align along elongation direction: strengthening
Stress Strain Graphs
Beyond “B”, the yield strength, deformations are plastic
Thermosets = strong & brittleNot Ductile
Thermolastics = depends on T
Ductility & Elongation (EL)EL < 5% BrittleEL > 5% Ductile
Cold Drawing above the Tg
25
• Compare to responses of other polymers: --brittle response (aligned, cross linked & networked case) --plastic response (semi-crystalline case)
Stress-strain curves adapted from Fig. 15.1, Callister 6e. Inset figures along elastomer curve (green) adapted from Fig. 15.14, Callister 6e. (Fig. 15.14 is from Z.D. Jastrzebski, The Nature and Properties of Engineering Materials, 3rd ed., John Wiley and Sons, 1987.)
TENSILE RESPONSE:initial: amorphous chains are kinked, heavily cross-linked.final: chainsare straight,
stillcross-linked
02040600246( )MPa8xxxelastomer plastic failure brittle failureDeformation !is reversible
Elastomer Molecules
Model of long elastomer molecules, with low degree of cross‑linking: (a) unstretched, and (b) under tensile stress.
High entropy Low entropy
Low energy High energy
13
0.280.61Magnesium,AluminumPlatinumSilver, GoldTantalumZinc, TiSteel, NiMolybdenumGraphiteSi crystalGlass-sodaConcreteSi nitrideAl oxidePCWood( grain)AFRE( fibers)*CFRE*GFRE*Glass fibers onlyCarbon fibers onlyAramid fibers onlyEpoxy only0.40.8246102040608010020060080010001200400TinCu alloysTungsten<100><111>Si carbideDiamondPTFEHDPELDPEPPPolyesterPSPETCFRE( fibers)*GFRE( fibers)*GFRE(|| fibers)*AFRE(|| fibers)*CFRE(|| fibers)*
MetalsAlloys
GraphiteCeramicsSemicond
PolymersComposites
/fibers
E(GPa)
Eceramics> Emetals>> Epolymers
109 Pa
Based on data in Table B2,Callister 6e.Composite data based onreinforced epoxy with 60 vol%of alignedcarbon (CFRE),aramid (AFRE), orglass (GFRE)fibers.
YOUNG’S MODULI: COMPARISON
• Hooke's Law: = E
• Poisson's ratio, :
metals: ~ 0.33 ceramics: ~0.25 polymers: ~0.40
Lε1-ν
FFsimpletensiontest
Linear-elastic1Eε
Units:E: [GPa] or [psi]: dimensionless
Linear Elasticity: Possion Effect
€
=−width strain
axial strain= −
Δw /w
Δl /l= −ε Lε
Why does have minus sign?
Poisson Ratio
€
=−Δw /w
Δl /l= −1
• Poisson Ratio has a range –1 1/2
Look at extremes• No change in aspect ratio:
€
Δw /w = Δl /l
• Volume (V = AL) remains constant: ΔV =0.
Hence, ΔV = (L ΔA+A ΔL) = 0. So,
In terms of width, A = w2, then ΔA/A = 2 w Δw/w2 = 2Δw/w = –ΔL/L.
Hence, €
ΔA /A = −ΔL /L
€
=−Δw /w
Δl /l= −
(−1
2Δl /l )
Δl /l=1/2 Incompressible solid.
Water (almost).
Poisson Ratio: materials specific
Metals: Ir W Ni Cu Al Ag Au 0.26 0.29 0.31 0.34 0.34 0.38
0.42generic value ~
1/3Solid Argon: 0.25
Covalent Solids: Si Ge Al2O3 TiC 0.27 0.28 0.23 0.19 generic
value ~ 1/4
Ionic Solids: MgO 0.19
Silica Glass: 0.20
Polymers: Network (Bakelite) 0.49 Chain (PE) 0.40
Elastomer: Hard Rubber (Ebonite) 0.39 (Natural) 0.49
Tensile stress is applied along cylindrical brass rod (10 mm diameter). Poisson ratio is = 0.34 and E = 97 GPa.
• Determine load needed for 2.5x10–3 mm change in diameter if the deformation is entirely elastic?
FFsimpletensiontest
Example: Poisson Effect
Width strain: (note reduction in diameter)x= Δd/d = –(2.5x10–3 mm)/(10 mm) = –2.5x10–4
Axial strain: Given Poisson ratioz= –x/ = –(–2.5x10–4)/0.34 = +7.35x10–4
Axial Stress: z = Ez = (97x103 MPa)(7.35x10–4) = 71.3 MPa.
Required Load: F = zA0 = (71.3 MPa)(5 mm)2 = 5600 N.
Negtive poisson’s ratio• foams
Lakes, R. S., "No contractile obligations", Nature, 1992, 358, 713-714.
CompressionRadialn = -1.24Axialn = 0
Anisotropic Materials
1) Compaction of UHMWPE powder2) Sintering3) Extrusion
• Mechanical properties are sensitive to temperature
FIGURE 10.9 Effect of temperature on the stress-strain curve for cellulose acetate, a thermoplastic. Note the large drop in strength and increase in ductility with a relatively small increase in temperature. Source: After T.S. Carswell and H.K. Nason. Manufacturing Processes for Engineering Materials, 5th ed. Kalpakjian • Schmid Prentice Hall, 2008.
Poly(methyl methacrylate)
Str
ess
Strain
Polymers
Metals
Ceramics
•Lower elastic modulus, yield and ultimate properties
•Greater post-yield deformability
•Greater failure strain
Polymers: Thermal Properties
• In the liquid/melt state enough thermal energy for random motion (Brownian motion) of chains
• Motions decrease as the melt is cooled
• Motion ceases at “glass transition temperature”
• Polymer hard and glassy below Tg, rubbery above Tg
Polymers: Thermal Properties
linear amorphous
log
(Mo
du
lus)
Temperature
semicrystalline
crosslinked
TmTg
Polymers: Thermal PropertiesS
tres
s
Strain
decreasing temperature or increasing crystallinity
• Properties depend on amount of cross-linking
Figure 8.13 M. P. Groover, “Fundamentals of Modern Manufacturing 3/e” John Wiley, 2007
Increasing cross-linking