TRƯỜNG ĐẠI HỌC BÁCH KHOA ĐÀ NẴNG KHOA HOÁ
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PHÂN TÍCH POLYME
(POLYMER ANALYSIS)
TS. ĐoànTh ị Thu Loan
Polymer analysis
(cid:252)Is a branch of polymer science dealing with analysis and characterisation of
polymers.
(cid:252)The complication of macromolecular chains, the dispersion in molecular
weight, tacticity, crystallinity, orientation, composition of polymers etc. and
complex morphological systems
analysis of polymer „
the small organic materials
(cid:222)
Focus on viscoelasticproperties, dynamic mechanical testing.
(cid:222)
Methods of polymer analysis
Chemical, Molecular and Structural Characterisation Surface Characterisation Mechanical and Physical Properties
-Surface roughness, -Chemical composition, -Interface characetrisation
•-AFM, SEM •-FT-IR •-Pull-out test
•Instronmechanical tester •Vickerhardness tester •DMA •Melt flow indexer •Torsions Rheometer
•
-Molecular weight determination, -Microstructuralcharacterisation and compositional analysis, -Crystallinity, -Investigation of polymer morphology, particle size, -Contact angle and wettability measurements -Tensile, flexural, impact, compression, hardness tests, -Rheologicaland viscoelastic properties, stiffness and modulus, surface tension, permeation and diffusion in polymers, adhesion tests, density
Instruments •FT-IR •IR-microscope •GPC ( size exclusion chromatography SEC) •-Viscosimetry •-X-ray (WAXS and SAXS) •-EM, SEM, TEM, AFM •-Dynamic and static methods for contact angle measurements.
Methods of polymer analysis
Thermal Behaviour Miscellaneous (hontap) Electrical and Optical Properties
Conductivity, electric -Melting point, glass transition Purity and molecular
current in solution, temperature, free rotation temperature, weight of small
light emitting and -Degradation and stability behaviour of molecules, water content
electromagnetic polymers in organic solvents,
surface tension properties
•Thermogravimetricanalyser (TGA)
measurement, pH
•TGA-FTIR coupled technique
•
•Differential scanning calorimetry(DSC)
•GC •pH meter •HPLC •Karl-Fischer titration
•Modulated differential scanning
Instruments Inolabconductivity meter
•Dynamic thermomechanicalanalyser
calorimetry(ADSC)
(DMTA) •Dielectric relaxation
Purpose of polymer analysis
-For quality control
-For predicting service performance
-To generate design data
-To investigate failures
Essential to identify the purpose of testing, because the requirements for each of the purposes are different.
-Precision Balance of these attributes,
-Reproducibility according to the purpose of
-Rapidity the test -Complexity -Automated test -Nondestructive test -Cost
Quality Control Tests
(cid:252)Nondestructive methods are advantageous and indeed essential when
100% of the output is being tested.
(cid:252)The tests should be simple and
inexpensive, and automation will
probably aid the rapidity of testing.
(cid:252)Tests related to product performance are preferred.
Tests Predicting Product Performance
(cid:252)The most important factor is that the tests
relate to service conditions
and to aspects of product performance.
(cid:252)should not be too complex, although rapidity and cheapness are less
important than was the case with quality control.
(cid:252)Nondestructive tests are not always appropriate when predicting product
performance, as it may be necessary to establish the point at which failure
occurs.
Tests for Producing Design Data
(cid:252)Usually test pieces are of a simple shape and a specified size , whereas
the product may be of a different geometry and size
(cid:252)Data must be presented in a form that enables the designer to allow for
changes in geometry, time scale, etc.. which implies
detailed and
comprehensive understanding of material behavior
(cid:252)It follows that data of this type are expensive to produce and that results
are unlikely to be obtained with great rapidity.
(cid:252)However, automation may be advantageous, particularly in the case of
tests running for a long time (creep tests)
Tests for Investigating Failures
(cid:252)Some understanding of the various mechanisms of failure is necessary before
suitable tests can be chosen.
(cid:252) Tests need not be complex but must be relevant
Ex: a simple measurement of product thickness may establish thatthere has
been a departure from the specified design thickness.
(cid:252)The absolute accuracy of the test may not be important, but it is essential that
it be capable of discriminating between the good and the bad product.
What are our expectations of polymer materials?
•Excellent Characteristics:
Mechanical and Physical Properties
Thermal Behaviour
Electrical and Optical Properties •Safe to use
Surface and interface Characteristics •Light weight
•Reliable, durable
•Low cost
•Less adverse environmental impact
•Good resistance to environmental attacks
Mechanical Testing
of Polymers
Types of MechnicalTests
(h)
(i)
Flexural test (d) (e) (f) Tensile test (a) Impact test (h) (i)
Compression test (b) Shear (g)
Tensile test
Scope:
(cid:252)Measure the force required to break a specimen and the extent to which the
specimen stretches or elongates to that breaking point.
(cid:252)Produce a stress-strain diagram, which is used to determine tensile modulus.
(cid:252)The data is often used to specify a material, to design parts towithstand
application force and as a quality control check of materials.
(cid:252)Since the physical properties of many materials (especially thermoplastics) can
(cid:222) vary depending on ambient temperature test materials at temperatures that
simulate the intended end use environment.
Tensile test
Specimen Size:
(cid:252)The most common specimen for ISO 527 is the ISO 3167 Type 1A
multipurpose specimen.
(cid:252)ASTM D882 uses strips cut from thin sheet or film.
*The multipurpose test specimen:
+150 mm long,
b
W
+The centersection: 10 mm wide *4 mm thick *80 mm long.
l
d
A tensile dog bone specimen
For the composite samples
Longitudinal test
Transverse test
Tensile test
Test Procedure:
(cid:252)Specimens are placed in the
grips and pulled until failure.
(cid:252)For ASTM D638, the test
speed is determined by the
material specification.
(cid:252)For ISO 527 the test speed
is typically 5 or 50mm/min for
measuring strength and
elongation
+and 1mm/min for measuring
modulus.
(cid:252) An extensometer is used to
Tensile2.wmv
determine elongation and
tensile modulus.
Stress –Strain Behavior
Characteristics of stress-strain behavior:
•
(cid:252) Modulus of elasticity (stiffness, elastic
modulus, Young’s modulus) is the slope of s
y
F
, s s e r t
s s the stress-strain curve in the elastic region
S
y)is the stress applied to a
(cid:252) Yield strength (s
material that just causes permanent
2%0
F
E deformation e e
y Strain, e
(cid:252) Tensile strength (TS) is defined at the
= d /l
fracture point and can be lower than the
yield strength
(cid:252) Ultimate tensile strength is the stress that
corresponds to the maximum load
(cid:252) Elongation at break (% e ) –the increase in
length of a specimen under tension before
P= Applied load A = Original cross-sectional area it breaks (Strain).
Stress-train behavior of polymers
Stress –Strain Behavior
Stress –Strain Behavior
(cid:252)Moduliof elasticity for polymers are ~ 10MPa-4GPa (compare to metals ~ 50 -
400 GPa)
(cid:252)Tensile strengths are ~ 10 -100MPa (compare to metals, hundreds of MPato
several GPa)
(cid:252)Elongation can be up to 1000 % in some cases (< 100% for metals)
(cid:252)Polymers are also very sensitive to the rate of deformation (strain rate).
Decreasing rate of deformation has the same effect as increasingT.
TENSILE RESPONSE: ELASTOMER CASE
Deformation of Amorphous Polymers
Deformation of Semicrystallineand crosslinkedPolymers
Stress-strain curves
Flexural test
Scope:
(cid:252)Measures the force required to bend a
beam under 3 point loading conditions.
(cid:252)The data is often used to select materials
for parts that will support loads without
flexing.
(cid:252)Flexural modulus is used as an indication
of a material’s stiffness when flexed.
(cid:252)can test materials at temperatures that
simulate the intended end use environment.
Flexural test
(cid:252)A variety of specimen shapes can be used Specimen Size:
(cid:252)The most commonly used specimen size:
+ 3.2mm x 12.7mm x 125mm for ASTM D790
+10mm x 4mm x 80mm for ISO 178
Test Procedure: (cid:252) Most commonly the specimen lies on a span and the load is
applied to the centerby the loading nose producing three point
bending at a specified rate.
(cid:252)The parameters for this test are :
+The support span;
+The speed of the loading
+The maximum deflection for the test.
These parameters are based on the test specimen
thickness, and are defined differently by ASTM and ISO.
Flexural test
F
b
b
L
d
m : initial slope of the load vs. deflection curve
b
=
=s (cid:252)Flexural strength 3 2
Eb
3
(cid:252)Flexural modulus LF 2 hb 3 Lm 4 hb
Flexural test
For relatively thin samples fi two point loading
For thick samples fi 4 point loading
Izod Impact Testing (Notched Izod)
Scope:
(cid:252)Notched IzodImpact is a single point test that measures
a materials resistance to impact from a swinging
pendulum.
(cid:252) Izodimpact is defined as the kinetic energy needed to
initiate fracture and continue the fracture until the
specimen is broken.
(cid:252)Izodspecimens are notched to prevent deformation of
the specimen upon impact.
(cid:252)This test can be used as a quick and easy quality control
check to determine if a material meets specific impact
properties or to compare materials for general toughness.
Izod Impact Testing (Notched Izod)
Specimen Size:
(cid:252) 64 x 12.7 x 3.2 mm for ASTM D256
(cid:252)The preferred thickness is 6.4 mm because it is not as likely tobend or crush
(cid:252)The depth under the notch of the specimen is 10.2 mm
(cid:252)80 x 10 x 4 mm forISO 180
(cid:252)The depth under the notch of the specimen is 8mm
Izod Impact Testing (Notched Izod)
Test Procedure:
(cid:252)The specimen is clamped into the pendulum impact test
fixture with the notched side facing the striking edge of the
pendulum.
(cid:252)The pendulum is released and allowed to strike through
the specimen.
(cid:252)If breakage does not occur, a heavier hammer is used
izodimpact.wmv
until failure occurs.
(cid:252)Since many materials (especially thermoplastics) exhibit
lower impact strength at reduced temperatures (cid:222) to test
materials at temperatures that simulate the intended end
use environment
Reduced Temperature Test procedure:
(cid:252)The specimens are conditioned at the specified temperature in a freezer
until they reach equilibrium.
(cid:252)The specimens are quickly removed, one at a time, from the freezer and
impacted.
(cid:252)Neither ASTM nor ISO specify a conditioning time or elapsed timefrom
freezer to impact -typical values from other specifications are 6 hours of
conditioning and 5 seconds from freezer to impact.
Data
ASTM
(cid:252)Impact energy is expressed in J/m or ft-lb/in.
(cid:252)Impact strength is calculated by dividing impact energy in J (orft-lb) by the
thickness of the specimen.
(cid:252)The test result is typically the average of 5 specimens.
ISO
(cid:252)Impact strength is expressed in kJ/m2
(cid:252)Impact strength (a cU)is calculated by dividing impact energy in J by the
area under the notch.
=
a
3 10
cU
·
W bh
(cid:252)The test result is typically the average of 10 specimens.
The higher the resulting number, the tougher the material.
W: energy b = width of the sample h = thickness of the sample
Impact Testing
Compression test
Scope:
(cid:252)Compressive properties describe the behaviorof a
material when it is subjected to a compressive load.
(cid:252)Loading is at a relatively low and uniform rate.
(cid:252)Compressive strength and modulus are the two most
common values produced.
Specimen size: (cid:252)Blocks or cylinders
(cid:252)For ASTM D695:
+The typical blocks: 12.7 x 12.7 x 25.4mm
+The cylinders:12.7mm diameter and 25.4mm long
(cid:252)For ISO 604: the preferred specimens:
+50 x 10 x 4mm for modulus
+10 x 10 x 4mm for strength
Compression test
Test Procedure:
(cid:252)The specimen is placed between compressive plates
parallel to the surface.
(cid:252)The specimen is then compressed at a uniform rate.
(cid:252)The maximum load is recorded along with stress-strain
data.
(cid:252)An extensometer attached to the front of the fixture is
used to determine modulus.
maximum compressive load
Compressive strength =
minimum cross-sectional area
change in stress
Compressive modulus =
change in strain
Rockwell Hardness tester
Scope:
(cid:252) A hardness measurement based on the net increase in
depth of impression as a load is applied.
(cid:252)Hardness numbers have no units and are commonly
given in the R, L, M, E and K scales.
(cid:252)The higher the number in each of the scales, the harder
the material
fi (cid:252)The harder the material better resistance to plastic
deformation or cracking in compression, better wear
properties
Specimen size:
(cid:252)Standardspecimen of 6.4mm thickness
(cid:252) is moldedor cut from a sheet.
DurometerHardness -Shore Hardness
Scope:
(cid:252)Determine the relative hardness of soft materials,
usually plastic or rubber.
(cid:252)The test measures the penetration of a specified
indentorinto the material under specified conditions of
force and time.
(cid:252)The hardness value is often used to identify or
specify a particular hardness of elastomersor as a
quality control measure on lots of material.
DurometerHardness -Shore Hardness
Specimen size:
(cid:252)Generally 6.4mm (¼in) thick for ASTM D 2240.
Test Procedure:
(cid:252)The specimen is first placed on a hard flat surface.
(cid:252)The indentorfor the instrument is then pressed into the specimen making sure
that it is parallel to the surface.
(cid:252)The hardness is read within one second (or as specified by the customer) of firm
contact with the specimen.
Data:
(cid:252)The hardness numbers are derived from a scale.
(cid:252)Shore A and Shore D hardness scales are common, with the A scalebeing used
for softer and the D scale being used for harder materials.
Density and Specific Gravity ASTM D792, ISO 1183
Scope:
(cid:252) Density is the mass per unit volume of a material.
(cid:252) Specific gravity is a measure of the ratio of mass of a given volume of
material at 23°C to the same volume of deionizedwater.
(cid:252)Specific gravity and density are especially relevant because plastic is
sold on a cost per pound basis and a lower density or specific gravity
means more material per pound or varied part weight.
Test procedures:
(cid:252) For sheet, rod, tube and moldedarticles.
(cid:252)The specimen is weighed in air then weighed when immersed in distilled water at
23°C using a sinker and wire to hold the specimen completely submerged as
required.Density and Specific Gravity are calculated.
(cid:252)Any convenient size
+Specific gravity = a/[(a + w)-b]
a = mass of specimen in air.
b = mass of specimen and sinker (if used) in water.
W = mass of totally immersed sinker if used and partially immersed wire.
+Density, kg/m3= (specific gravity) x (997.6)
Bulk Density ASTM D1895B
(cid:252)Bulk density is defined as the weight per unit volume of material.
(cid:252)Bulk density is primarily used for powders or pellets.
(cid:252)The test can provide a gross measure of particle size and dispersion which can affect
material flow consistency and reflect packaging quantity.
(cid:252)A funnel is suspended above a measuring cylinder.
(cid:252)The funnel is filled with the sample and allowed to freely flow into the measuring
cylinder.
(cid:252)The excess material on top of the measuring cylinder is scraped off with a straight
edge.
(cid:252)The sample and the cylinder is then weighed and the weight / volume (Bulk Density) is
determined.
(cid:252)Apparent density value is recorded as g/cm3
Thermal Analysis
(cid:252)Thermal analysis (TA) is frequently used to describe analytical experimental
techniques which investigate the behaviourof a sample as a function of temperature.
TA refers to conventional TA techniques such as:
+Differential thermal analysis (DTA)
+Differential scanning calorimetry(DSC)
+Dynamic mechanical analysis (DMA)
+Thermogravimetry(TG/TGA)
Representative TA curves
Thermal Analysis
The advantages of TA over other analytical methods can be summarized as follows:
(i)the sample can be studied over a wide temperature range using various temperature
programmes
(ii)almost any physical form of sample (solid, liquid or gel) can beaccommodated using
a variety of sample vessels or attachments
(iii)a small amount of sample (0.1 µg-10 mg) is required
(iv)the atmosphere in the vicinity of the sample can be standardized
(v)the time required to complete an experiment ranges from several minutes to several
hours
(vi)TA instruments are reasonably priced
Differential thermal analysis (DTA)
Scope:
(cid:252)Measure the differential temperature between a sample and a reference pan
fi to determine the temperature of the transitions
Test procedures:
(cid:252)As the sample goes through the programmed temperature change, there is no
temperature difference until the sample undergoes an exothermic or endothermic
chemical reaction or change of physical state.
(cid:252)The thermal event (a temperature difference between the sample and the
D reference (D T)) will be recordedfi Tversus time or temperature plot
Differential thermal analysis (DTA)
Schematic of a DTA apparatus
A DTA curve
Tr
The subscripts represent: s-sample, r-reference, i-initial,f-final.
Differential Scanning Calorimeter(DSC)
Scope: DSC measures:
Tg = Glass Transition Temperature = The temperature (°C) at which an amorphous
polymer or an amorphous part of a crystalline polymer goes from a hard, brittle state to
a soft, rubbery state.
Tm = melting point = The temperature (°C) at which a crystalline polymer melts.
DHm = the amount of energy in (joules/gram) a sample absorbs while melting.
Tc = crystallization point = is the temperature at which a polymercrystallizes upon
heating.
DHc = the amount of energy (joules/gram) a sample releases while crystallizing.
The data can be used to identify materials, differentiate homopolymersfrom
copolymers or to characterize materials for their thermal performance.
Test Procedure:
(cid:252)A sample of 10 to 20 mg in an aluminum
sample pan is placed into the differential
scanning calorimeter.
(cid:252)The sample is heated at a controlled
rate (usually 10°/min)
(cid:252)a plot of heat flow versus temperature
is produced.
(cid:252)The resulting thermogram
is then
Dsc3.wmv
analyzed.
DSC
Some factors influence on DSC resultsc
Does the sample contain volatile components? 1.
g) by up to
(cid:252) 2 to 3% water/solvent can lower the glass transition temperature(T
100oC
(cid:252) Evaporation creates endothermic peaks in standard (non-hermetic) DSC pans and
can be suppressed with use of hermetic DSC pans.
2. At what temperature does the sample decompose?
(cid:252) Set the upper limit of the DSC experiment based on decompositiontemperature
(TGA). No meaningful DSC data can be obtained once decompositionresults in a
5% weight loss
(cid:252) Decomposition affect: the quality of the baseline due to both endothermic and
exothermic heat flow, the quality of the baseline for future experiments and can affect
the useful lifetime of the DSC cell due to corrosion.
Some factors influence on DSC results
3. How does thermal history (temperature and time) affect DSC results on the sample?
4. Identical materials can look totally different based on:
- Storage temperature and time.
- Cooling rate from a temperature above Tgor above the melting point.
- Heating rate.
- Different kinds of experiments may need to be performed in orderto measure the
current structure vs. comparing samples to see if the materials are the same.
5. How is the Influence of the atmosphere (air or inert gases (N2, argon,..))
Tgsensitivity
Use >10oC/min heating rates
Thermogravimetry(TG)
(cid:252)To characterize the decomposition and the thermal stability of materials.
(cid:252)To provide an indication of the composition of the sample, including volatiles and
inert filler
(cid:252)The change of mass as function of temperature (scanning mode) ortime
(isothermal mode)
(cid:252)To get information about the following processes:
vDecomposition
vDesorption
vAbsorption
vVaporization
vOxidation
vReduction
Tma.wmv
Block diagramofa thermobalance
Test procedure:
(cid:252)Set the inert (usually N2) and oxidative (air, O2) gas flow rates to provide the
appropriate environments for the test.
(cid:252)Place the test material in the specimen holder and raise the furnace.
(cid:252)Set the initial weight reading to 100%, then initiate the heating program.
(cid:252)The gas environment is preselectedfor :
veither a thermal decomposition (inert -nitrogen gas), an oxidative decomposition
(air or oxygen)
vor a thermal-oxidative combination.
vSample amount: 10 to 15 milligrams
TG curve
TG and DTG curves for the thermal decomposition of calcium oxalate (CaC2O4. H2O in argon at 20oC/min(3).
The three steps in Figure are: (1)The loss of H2O to form anhydrous oxalate (2)The loss of CO to form the carbonate ,and (3)The loss of CO to form CaO
120
25
100
As received_J3 NaOH_J3 NaOH/(APS+XB)_J3 NaOH/Y9669_J3
20
80
)
%
15
60
( t h g i e
W
D e v i a t i o n
40
10
20
5
0
0
-20
100
200
500
600
300
400
Temperature(°C)
TG and DTG curves of jute fibrewith different treatments
Dynamic Mechanical Analysis (DMA)
Scope:
(cid:252)Determines elastic modulus (or storage modulus, G'),
viscous modulus (or loss modulus, G'') and damping
coefficient (Tan D) as a function of temperature, frequency
or time.
(cid:252)Results are typically provided as a graphical plot of G',
G'', and Tan Dversus temperature.
(cid:252)Identifies transition regions in plastics, such as the glass
transition, and may be used for quality control or product
development.
(cid:252) Can recognize small transition regions that are beyond
the resolution of DSC (Differential Scanning Calorimetry).
Dynamic Mechanical Analysis (DMA)
Specimen size:
-Typically 56 x 13 x 3 mm, cut from the centersection of an ASTM Type I tensile bar,
or an ISO multipurpose test specimen.
Test Procedure:
(cid:252)The test specimen is clamped between the movable and stationary fixtures, and
then enclosed in the thermal chamber.
(cid:252)Frequency, amplitude, and a temperature range appropriate for the material being
tested are input.
(cid:252)The Analyzer applies torsionaloscillation to the test sample while slowly moving
through the specified temperature range.
Is DMA Thermal Analysis or Rheology
(cid:216) Definitions
(cid:216) Thermal Analysis is the measurement of some characteristic of a
substance as a function of temperature or time.
(cid:216) Rheology is the science of flow and deformation of matter.
(cid:216) DMA is the general name given to an instrument that mechanically deforms
a sample and measures the sample response. The deformation can be
applied sinusoidally, in a constant (or step) fashion, or under a fixed rate.
The response to the deformation can be monitored as a function of
temperature or time.
Dynamic Mechanical Testing
Deformation
l An oscillatory (sinusoidal) deformation (stress or strain) is applied to a sample.
Response
lThe material response (strain or stress) is measured.
Phase angle d
lThe phase angle d , or phase shift, between the deformation and response is measured.
Dynamic Mechanical Testing
Purely Elastic Response (HookeanSolid)
Purely Viscous Response (Newtonian Liquid)
d = 90
d = 0
Stress
Stress
Strain
Strain
Dynamic Mechanical Testing: ViscoelasticMaterial Response
Phase angle 0 < d < 90
Strain
Stress
DMA ViscoelasticParameters
G = Stress/Strain
G' = (stress/strain)cosd
The Modulus: Measure of materials overall resistance to deformation.
G" = (stress/strain)sind
The Elastic (Storage) Modulus: Measure of elasticity of material. The ability of the material to store energy.
The Viscous (loss) Modulus: The ability of the material to dissipate energy. Energy lost as heat.
Tan d = G"/G'
Tan Delta: Measure of material damping -such as vibration or sound damping.
Storage and Loss of a ViscoelasticMaterial
SUPER BALL
LOSS
X
TENNIS BALL
STORAGE
DMA ViscoelasticParameters: Damping, tan d
G*
G"
Dynamic measurement represented as a vector
Phase angle d
G'
lThe tangent of the phase angle is the ratio of the loss modulus to the storage modulus.
tan d = G"/G' l"TAN DELTA" (tan d ) is a measure of the damping ability of the material.
DMA 2980 : Schematic
BIFILAR-WOUND FURNACE
SAMPLE
CLAMPS
LOW MASS, HIGH STIFFNESS CLAMPING FIXTURES
AIR BEARING SLIDE
AIR BEARING
OPTICAL ENCODER
DRIVE MOTOR
UNIQUE PATENT-PENDING DESIGN
DMA : Dual Cantilever Mode
Sample
Movable clamp Stationary Clamp
DMA : Single Cantilever Mode
Sample
Stationary Clamp
Movable clamp
DMA : 3-Point Bend Mode
Sample
Stationary Fulcrum
Force
Moveable Clamp
DMA : Tension Mode
Stationary Clamp
Sample (film, fiber,orthin sheet)
Movable clamp
DMA : Shear Sandwich Mode
Sample
Movable Clamp
Stationary Clamp
DMA : Compression Mode
Movable Clamp
Sample
Stationary clamp
PSA: Glass Transition Measurement
INTERFACES IN COMPOSITES
• Questions that need to be answered:
–Are interfacial properties important at all?
–What is the role/effect of interfaces with respect to overall
mechanical properties of composites?
–How can we measure interfacial adhesion in composites?
–Can we develop analytical models that are useful for design
purposes?
–Is it possible to tailor interfacial adhesion?
EXAMPLES OF PRACTICAL RELEVANCE (VARIOUS FIELDS)
• Thin coatings on critical surfaces (reflective coatings on optical components, plating for corrosion protection, magnetic films for data storage…)
• Interfaces in composites (carbon-epoxy, glass-PP, SiC-SiC, PE-
PE…)
• Interaction of biological systems or media with engineering materials (tissue bonding of prostheses, dental implants, artificial hips, cell adhesion [cells remain alive only if they adhere to a substrate]…)
Wetting and adhesive strength
• Adequate wetting is a necessary (but not sufficient!) condition for
good adhesion between a liquid and a solid surface.
• The contact angle between a liquid droplet and a surface is an
indication of compatibility between these.
q
If q < 90°, the liquid ‘wets’the solid surface. If q = 0°, the liquid ‘spreads’on the surface (complete wetting). If q = 180°, the liquid ‘does not wet’the surface
• • •
In terms of surface energies:
•
Surface energies (g)
vapor
liquid
gLV q
gSV
gSL
solid
(S = Solid, V = Vapor, L = Liquid)
The equilibrium wetting or contact angle q is dictated by the Young equation, obtained by a balance of horizontal forces:
gSV = gLV cosq+ g SL
Thus, good wetting (q = 0 or small) arises when the surface energy of the solid is equal to or greater than the sum of the liquid surface energy and the solid-liquid interface surface energy.
gSV ≥ gLV + gSL
[Interface surface energies are difficult to measure (and may be influenced by chemical reactions) but are often smaller than thevalues for the phases in air]
The lower the contact angle, the greater the wettability:
Liquid is attracted to itself, not to solid
Liquid is attracted to solid, less to itself
Indirect measurement can be made by immersing the fiber into the liquid
of interest and measuring the force of immersion or emersion (= Wilhelmy
microbalance technique). A force balance permits the calculationof the
contact angle if the fiber perimeter and surface energy of the liquid are
known (see Bascom).
Mic robalanc e
Krüs s tensiomete r
Comp ute r
Fibr e
Liq uid
Glass containe r
Drive system
Capillary-rise method
Sessile drop method
Wilhelmymethod
Fiber-matrix interfacial adhesion
• Two general methodologies:
–Indirect (or macromechanical) testing -
focuses on the collective
behavior of fibers in a polymer matrix [interfacial strength is
interpreted via simplistic approximations; fast but questionable
data collection]
–Direct (or micromechanical) testing –probes interfacial behavior
of individual fibers interacting with a polymer matrix [more
fundamental information; variability within and between
techniques; issue of relevance to real-life composites (scaling-
up)]
Indirect (or macromechanical) testing
1.The transverse tensile test
2. The short-beam shear (or interlaminarshear
strength -ILSS) test
3. Asymetrical4-point (Iosipescu) bend test
CONCLUSION – They are simple to perform, but yield
ambiguous, inaccurate data.
(And other macroscopic tests… )
Direct (or micromechanical) testing
a) b)
Fibre
Indentor Microscope Objective
Matrix
Composite
c) F d) F Knife edge Fibre
Matrix Sustrate le le
Micromichanicaltests : (a)fragmentation, (b) microindentation, (c) pull-out and (d) microbondtest
Single fiber pull-out test
Load cell
Mesurement object
Greszczuk’smodel for pull-out
A small single fiber is embedded in a resin and the debondingload for the
pull-out of the fiber from the resin is measured and calculated for the
=
t
i
F lf 2 r p
interfacial shear strength (IFSS, t) using the following equation:
where F is the debondingload, r f the fiber radius, and ℓ the embedded length. This technique has been successfully studied in carbon and boronfibers in
an epoxy resin.
2. The single-fiber microcompression(or MIT) test
Tricky test, difficult to perform, fiber-matrix interfacial fracture is often
only partial due to slight off-axis moments, loading must be exactly
parallel to the fiber axis.
3. The single-fiber fragmentation test
Single fiber embedded in matrix
Fragmented fiber
Pre-conditions for successful test : (a) failure strain of the fiber is much
smaller than that of matrix; (b) Interfacial bonding must be fair to good.
Mapping NanomechanicalProperties by AFM Nanoindentation
A
B
C
D
Stiffness contrast
Glass fibre
Interp hase E pox y
Fmax
2.6
D
A
B
C
)
N
m
Loading
Unloading
dF dh
( e c r o f n o i t a t n e d n I
hc
hmax
23
0
Penetration depth(nm)
Cyclic Loading-AFM-TopographyatFailure
• APS
Virginfiber
Aftercyclic loading
Pulloutaps.000
Pulloutaps.001
Ra= 3.5 nm, Rmax= 151 nm Ra= 4.2 nm, Rmax= 48 nm
Scanning Electron Microscopy (SEM)
(cid:252) Examine surface irregularities or fracture areas in a part for plastics applications.
(cid:252) Measure the thickness (in cross section) of thin coatings.
(cid:252)Study surface topography and failure analysis
(cid:252)Test specimens are sputter coated with gold, then placed in a vacuum chamber for
viewing on the computer monitor at up to 10,000x magnification.
(cid:252) Polaroid photos are taken for a permanent record. Approximately 0.25" x 0.25"
Polaroid photos can be scanned into electronic documents.
Untreated jute NaOH-treated jute
NaOH/PAPS-jute
PP/jute composite without treatment
PP/jute composite with treatment
Fourier Transform Infrared Spectrometry (FTIR)
-ASTM E1252
-Identify of polymer
-Detect organic layers or fiberglass
-Detect surface coatings
-Also examine contaminants and some fillers within the polymers
-A small amount (few grams) of sample is needed.
Fourier Transform Infrared Spectrometry (FTIR)
Simplified optical layout of a typical FTIR spectrometer
-Three basic spectrometer components: -The sample is inserted into a detector
and the amount of Infrared Light absorbed
at each frequency is determined. +Radiation source +Interferometer (giaothoa k ế), +and detector
Fourier Transform Infrared Spectrometry (FTIR)
The most commonly used interferometer is a Michelson interferometer.
(cid:252)Consists of 3 active components: a moving mirror, a fixed mirror, and a beamsplitter
(cid:252)The two mirrors are perpendicular to each other.
(cid:252)The beamsplitteris often made by depositing a thin film of germanium onto a flat KBr
substrate
(cid:252)Radiation from the broadband IR source impinges on the beamsplitter
(cid:252) At the beamsplitter, half the IR beam is transmitted to the fixed mirror and the
remaining half is reflected to the moving mirror
(cid:252)After the divided beams are reflected from the two mirrors, theyare recombined at the
beamsplitter. Due to changes in the relative position of the moving mirror to the fixed
mirror, an interference pattern is generated.
(cid:252)The resulting beam then passes through the sample and is eventually focused on the
detector.
Infrared Region(IR)
FTIR
['gæmə]
['reidiou]
ultraviolet
electromagnetic spectrum
The energy of the wave (E):
=
=
E
hν
Wavenumber( ): =1 / l
• ch λ
n: frequency l :wavelength
The infrared region (14,000 cm-1 to 10 cm-1): near, mid and far-infrared region (cid:252)Mid-infrared region (4,000 cm-1 to 400 cm-1):
fi themost interest region
fi corresponds to changes in vibrational energies within molecules
(cid:252)The far infrared region (400 cm-1 to 10 cm-1): fi useful for molecules containing heavy atoms such as inorganic compounds
fi requires rather specialisedexperimental techniques.
FTIR
Molecular Vibrations
Stretching vibration
Asymmetrical stretching Symmetrical stretching
Out-of -plane bend
Bending vibration
In-plane bending Out-of-plane bending
Major vibrationalmodes for a nonlinear group, CH 2 (When a compound absorbs the energy of Infrared radiation)
FTIR
Single Bonds to Hydrogen