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Amorphous polymer Morphology
The bulk state, sometimes called the condensed or
solid state, includes both amorphous and crystalline
polymers
Morphology : is a term used to describe the form or
structure of the polymer chains of thermoplastic
materials when they are in their frozen or solid state.
• For thermoplastic resins, there are two basic morphologies:
AMORPHOUS and SEMI-CRYSTALLINE
• Amorphous polymers appear random and jumbled when allowed to
cool in a relaxed state. They appear very similarly to their molten
state, only the molecules are closer together.
• They can be described as being similar to a large pot of spaghetti
noodles.
Amorphous materials are like cooked ramen noodles in
that there is a random arrangement of the molecules and
there are no crystals present to prevent the chains from
flowing
 It is important to remember that both materials have random,
unordered arrangement when molten.
 amorphous polymers exhibit different physical and
mechanical behavior depending on temperature and structure.
 At low temperatures, glassy, hard, and brittle. As the
temperature is raised, they go through the glass–rubber
transition.
 Above Tg, cross-linked amorphous polymers exhibit rubber
elasticity. An example is styrene–butadiene rubber (SBR)
 An amorphous polymer does not exhibit a crystalline X-
ray diffraction pattern, and it does not have a first-order
melting transition.
Example :
• Polyvinyl Chloride (PVC)
• General Purpose Polystyrene (GPPS)
• Polycarbonate (PC)
• Polymethylmethacrylate (PMMA or
Acrylic)
• Acrylonitrile Butadiene Styrene (ABS
a terpolymer)
 Older literature referred to the amorphous state as a
liquid state.
 However, polystyrene or poly(methyl methacrylate) at
room temperature are glassy.
 Today, amorphous polymers in the glassy state are better
called amorphous solids.
 >Tg, if the polymer is amorphous and linear, it will flow,
albeit the viscosity may be very high.
 For most materials, we are concerned with the melting
point and boiling point.
Glass Transition Temperature (Tg)
 The glass transition temperature (Tg) is defined as the
temperature at which the polymer softens because of the onset
of long-range coordinated molecular motion.
 For thermoplastic materials, we are concerned with:
o Glass Transition Temperature
o Melting Temperature
 In amorphous materials, it is the temperature at which
material behaves more rubber-like than glass-like.
 Above Tg:
 The material stretches further when pulled (more ductile)
 The material absorbs more impact energy without fracturing
when struck
 When the material does fail, it fails in a ductile manner as
opposed to a brittle manner
The sample experienced a brittle
failure The material broke like glass
The sample broke in a ductile manner.
The material yielded (stretched) before
failure. The material behaved more
like a rubber
example:
Polyethylene and Polypropylene both have low
Tg’s. They are way below room temperature. That is why
milk jugs and yogurt containers are flexible when you take
them out of the refrigerator.
Amorphous materials don’t truly have a Tm. They just
continue to soften more until they behave more like a liquid.
The molecules absorb enough energy and move far
enough apart (increase the free volume) that the material
can flow.
Amorphous polymer
Melt Temperature (Tm)
 When we refer to the melt temperature for amorphous materials, it
is usually the temperature at which we can process it.
 For S/C materials, the Tm is the temperature at which the crystals
melt.
 If the polymer is crystalline Tm>Tg
ideal temperature for
growing crystals
is approximately 2/3
of the way between the Tg
and the Tm.
 Not in all cases, but in
many, the degradation temperature for S/C materials is not
much higher than the melt temperature.
Melting vs. Glass Transition Temp.
What factors affect Tm and Tg?
Factors
affecting
Tm
Molecular chemistry
and structure: -
Molecular chemistry and
structure will influence the
ability of the polymer chain
molecules to make
rearrangements and,
therefore, will also affect the
Tm
Chemical bonds: -
The presence of double
bonds and aromatic
groups in the polymer
backbone lowers chain
flexibility and causes an
increase in Tm.
Size and type of side
groups: - size and type of side
groups influence chain rotational
freedom and flexibility; Bulky or
large side groups tend to restrict
molecular rotation and raise Tm.
The presence of polar
groups:- leads to significant
intermolecular bonding forces and
relatively high Tm.
Degree of branching:- The
introduction of side
branches introduces
defects into the crystalline
material and lowers the
melting temperature.
Factors
Affecting
Tg
Molecular Weight – In straight chain
polymers, increase in MW leads to
decrease in chain end concentration
resulting in decreases free volume at end
group region – and increase in Tg
Molecular Structure - Insertion of bulky,
inflexible side group increases Tg of
material due to decrease in mobility,
Chemical cross-linking - Increase in cross-
linking decreases mobility leads to
decrease in free volume and increase in Tg
Polar groups - Presence of polar groups
increases intermolecular forces; inter chain
attraction and cohesion leading to
decrease in free volume resulting in
increase in Tg.
• The mechanical properties of polymers are
sensitive to temperature changes
Figure 1 Modulus versus temperature for an
amorphous thermoplastic
Figure 2. Modulus versus temperature for crystalline
thermoplastics
Figure 3. Modulus versus temperature for thermosetting
resins
Figure 4 Modulus versus temperature for a reinforced
crystalline thermoplastic
crystalline state
• Both amorphous and crystalline areas in can exist in
the same polymer.
• Areas in polymer where chains packed in regular
way.
• X-ray scattering and electron microscopy have shown
that the crystallites are made up of lamellae which,in
turn, are built-up of folded polymer chains
Schematic representation of
(a) fold plane showing regular chain folding,
(b) ideal stacking of lamellar crystals,
(c) interlamellar amorphous model
(d) fringed micelle model of randomly distributed crystallites
(Plastic Technology Handbook)
crystalline state
• The crystalline state is defined as one that diffracts X-
rays and exhibits the first-order transition known as
melting.
A first-order transition normally has a discontinuity in the volume–
temperature dependence
crystalline
region
amorphous
region
crystalline state
 Polymers crystallized in the bulk, however, are never
totally crystalline, a consequence of their long-chain
nature and subsequent entanglements.
 Crystallinity occurs when linear polymer chains are
structurally oriented in a uniform three dimensional
matrix.
 Three factors that influence the degree of crystallinity
are:
i) Chain length
ii) Chain branching
iii) Interchain bonding
iv) the rate of cooling during solidification
Melting temperature observing
 Non regularity of structure first decreases the melting
temperature and finally prevents crystallinity.
 crystalline materials have sharp X-ray pattern
characteristic at Tm
 Ideally, the melting temperature constitutes a first order
phase change, should give a discontinuity in the volume,
with a connected sharp melting point.
 Due to polymer imperfections or very small size of the
crystallites in bulk most polymers melt over a range of
several degrees
Specific volume–temperature relations for linear polyethylene
• Open circles, specimen
cooled relatively rapidly
from the melt to room
temperature;
• solid circles, specimen
crystallized at 130°C for
40 days, then cooled to
room temperature
The melting temperature is usually taken as the
temperature at which the last trace of crystallinity
disappears.
melting temperature can be determined thermally.
using the differential scanning calorimeter (DSC)
gives the heat of fusion as well as the melting
temperature
methods for determining the percent
crystallinity
 most crystallizing polymers are semi-crystalline; that is,
a certain fraction of the material is amorphous, while the
remainder is crystalline
 The reason why polymers fail to attain 100% crystallinity
is kinetic, resulting from the inability of the polymer
chains to completely disentangle and line up properly in
a finite period of cooling or annealing.
1. Determination of the heat of fusion of the whole sample
by calorimetric methods such as DSC
Difference in heat out put of the two
heaters vs temperature
the latent heat of melting is the area of
this peak
the temperature at the top of the peak to
be the polymer's melting temperature, Tm.
DSC of a commercial isotactic polypropylene sample
 DSC measure the heat flow in to or from a sample as is
either heated or cooled
heat of fusion ∆Hf is the area under the peak
The percent crystallinity is then determined using the
following equation:
% crystallinity =
Δ𝐻𝑚 − Δ𝐻𝑐
Δ𝐻𝑚𝑜 ∗ 100%
Δ𝐻𝑚 is The heats of melting
ΔHc is The heats of crystallization
ΔHmo is a reference value and represents the heat of melting if
the polymer were 100% crystalline
are determined by
integrating the areas (J/g)
under the peaks
}
Example
Polyethylene terephthalate (PET) is widely utilized for the production of
food and beverage containers. The reference heat of melting for PET is
140.1 J/g and the result generated from DSC instrument show that the
amount of heat for Cold crystallization at 101 0C is 1.65 J/g where the
polymer undergoes some small amount of crystallization while heating
in the DSC melting at 247 0 C is 46.5 J/g where the existing crystalline
component is destroyed, determine the percentage of crystallinity?
Soln
% crystallinity =
Δ𝐻𝑚 − Δ𝐻𝑐
Δ𝐻𝑚𝑜 ∗ 100%
=
46.5 −1.65
140.1
∗ 100%
= 32%
2. Determination of the density of the crystalline portion via
X-ray analysis of the crystal structure, and determining
the theoretical density of a 100% crystalline material.
s- density of a specimen for which the present crystallinity
is to be determined.
a- density of the completely amorphous polymer.
c- density of the completely crystalline polymer.
Semi-Crystalline polymer
summery
METHODS OF DETERMINING CRYSTAL
STRUCTURE
 There are four basic methods in wide use for the study of
polymer crystallinity: X-ray diffraction, electron
diffraction, infrared absorption, and Raman spectra
X-Ray Methods
 When a beam of x-rays
impinges on a solid
material, a portion of this
beam will be scattered in
all directions by the
electrons associated with
each atom or ion that lies
within the beam’s path.
Fig Diffraction of x-rays by planes of atoms (A–A’ and B–B’).
 if the path length difference between 1-P-1’ and 2-Q-2’is
equal to a whole number, n, of wavelengths.
 That is, the condition for diffraction is nλ = 𝑆𝑄 + 𝑄𝑇
crystalline substances must to act as a three-dimensional diffraction
grating for X-rays
Bragg equation :
By considering crystals as reflection gratings.
λ the X-ray wavelength
θ the angle between the X-ray beam and these atomic planes
n the order of diffraction
X-Ray Methods
 d and λ are of the order of 1 Å. Such an analysis from a
single crystal produces a series of spots.
 However, not every crystalline substance can be
obtained in the form of macroscopic crystals.
 This led to the Debye–Scherrer method of analysis for
powdered crystalline solids or polycrystalline specimens.
 The crystals are oriented at random so the spots become
cones of diffracted beams.
 can be recorded either as circles on a flat photographic
plate or as arcs on a strip of film encircling the specimen
The angle RSX is 2θ, where θ is the angle of incidence
on a set of crystal plane
X-Ray Methods
X-Ray Methods
Diffraction spot or line depends on
the scattering power of the individual atoms( the
number of electrons in the atom)
the arrangement of the atoms with regard to the
crystal planes
the angle of reflection
the number of crystallographically equivalent sets
of planes contributing
the amplitude of the thermal vibrations of the
atoms.
 intensities of the spots or arcs and their positions are
required to calculate the crystal lattice
Electron Diffraction of Single Crystals
 Electron microscopy provides information about the very
small, including a view of the actual crystal cell size and
shape.
 Electron diffraction studies utilize single crystals.
 Since the polymer chains in single crystals are most often
oriented perpendicular to their large flat surface,
diffraction patterns perpendicular to the 001 plane are
common.
 Tilting of the sample yields diffraction from other planes.
The interpretation of the spots obtained utilizes Bragg’s
law in a manner identical to that of X-rays.
Electron Diffraction of Single Crystals
Required:
Evacuated diffraction tube that contains an electron
gun accelerating anode to provide a known energy to
the electrons in the beam
crystalline targets and screen
Infrared Absorption
The information that infrared absorption spectra yield about
crystallinity:
1. Infrared spectra of semicrystalline polymers
include“crystallization sensitive bands.” The intensities
of these bands vary with the degree of crystallinity and
have been used as a measure of the crystallinity.
2. By measuring the polarized infrared spectra of oriented
semicrystalline polymers, information about both the
molecular and crystal structure can be obtained. Both
uniaxially and biaxially oriented samples can be studied.
3. The regular arrangement of polymer molecules in a
crystalline region can be treated theoretically, utilizing
the symmetry properties of the chain or crystal
Raman Spectra
1. Since the selection rules for Raman and infrared spectra are
different, Raman spectra yield information complementary to
the infrared spectra.
example, the S—S linkages in vulcanized rubber and the C=C
bonds yield strong Raman spectra but are very weak or
unobservable in infrared spectra.
2. Since the Raman spectrum is a scattering phenomenon,
whereas the infrared methods depend on transmission, small
bulk, powdered, or turbid samples can be employed.
3. the Raman spectra provide information equivalent to very low-
frequency measurements, even lower than 10 cm-1. Such low
frequency studies provide information on lattice vibrations.
Polymer Single Crystals
 crystallization is an allayment of molecular chain and
folding of chain to get order region
polymer single crystal formation
1) From precipitate (from dilute solutions, they form
lamellar-shaped single crystals)
2) From melt
Polymer Single Crystals
1) From precipitate
 Ideas about polymer crystallinity start by preparing
single crystals of polyethylene.
 These were made by precipitation from extremely dilute
solutions of hot xylene.
 These crystals tended to be diamond-shaped and of the
order of 100 to 200 Å thick
2. CRYSTALLIZATION FROM THE MELT
usually super cool to greater or lesser extents
crystallization temperature may be 10 to 20°C lower
than the melting temperature
Supercooling arises from the extra free energy required
to align chain segments
the most obvious of the observed structures are the
spherulites
spherulites are really spherical in shape only during
the initial stages of crystallization
Spherulites of low-density polyethylene
Spherulites of low-density polyethylene
Later spherulites interrupt on their neighbors
then pervade the entire mass of the material
The evolution of the spherulite
KINETICS OF CRYSTALLIZATION
 During crystallization from the bulk, polymers form
lamellae,
 which in turn are organized into spherulites or their
predecessor structures
 volume changes on melting; usually increasing
The rate of crystallization increases as the temperature
is decreased.
This follows from the fact that the driving force
increases as the sample is supercooled
KINETICS OF CRYSTALLIZATION
 Crystallization rates may also be observed
microscopically :
 by measuring the growth of the spherulites as a function
of time
 The isothermal radial(at 125°C) growth of the spherulites
is usually observed to be linear
KINETICS OF CRYSTALLIZATION
 The increase in rate of crystallization as the temperature
is lowered is controlled by the increase in the driving
force
 temperature is lowered still
further, molecular motion
becomes sluggish as the glass
transition is approached, and
the crystallization rate
decreases again.
linear growth rate versus crystallization temperature for poly(ethylene terephthalate) .Tf =
265°C, and Tg = 67°C, at which points the rates of crystallization are theoretically zero.
KINETICS OF CRYSTALLIZATION
 Below Tg, the rate of crystallization effectively becomes
zero.
rule-of-thumb
 for determining a good temperature to crystallize a
polymer
 if the melting temperature(Tf) is known. where Tf is in
absolute temperature. At (8/9) Tf the polymer is
supposed to crystallize readily.
Free energy of polymer crystallization
 The classic melting temperature is usually taken
where the last trace of crystallinity disappears, point
A in Figure b.
∆Gf The free energy of fusion
∆Hf the molar enthalpy
∆Sf entropy of fusion
 At the melting temperature, ∆Gf equals zero, and
 smaller entropy or a larger enthalpy term raises Tf.
 the relative changes in ∆Hf and ∆Sf in going from the
amorphous state to the crystalline state determine the
melting temperature of the polymer
Free energy of polymer crystallization
Properties
Amorphous vs. S/C
 Chemical Resistance
 Optical Properties
 Impact Resistance
 Viscosity
 Weather Resistance
 Shrinkage
Chemical Resistance
 Plastic materials are used in virtually and contact with a
wide variety of chemical substances that they need to
resist
As a general rule S/C materials are more resistant to
chemical attack than amorphous materials.
It is more difficult for the chemical media to
penetrate the dense crystalline structure to damage
the polymer chains.
Polyethylene is used to store everything from
detergent to mineral spirits to gasoline.
 But Polypropylene is only slightly less chemically
resistant than Polyethylene.
 Of the amorphous materials PVC is probably the best in
chemical resistance, mainly due to the large chlorine
atom that helps to protect the main polymer chain.
 Polycarbonate, Acrylic, Polystyrene and the other
styrenics are all very susceptible to chemical attack,
especially to mineral spirits and solvents like lacquer and
paint thinners, alcohol, and gasoline.
Optical Properties
Amorphous materials have a much higher clarity
than S/C materials. and can be translucent/optical
quality.
If the crystallinity is disrupted by adding a copolymer
or other additive or by quenching the material so
quickly the crystals don’t have enough time to form,
the material may appear somewhat clear.
Amorphous Acrylic more commonly known as
Plexiglas and Polycarbonate used in safety glasses
and optical lenses are far superior in terms of optical
properties
Impact Resistance
 The material structure determines the impact resistance,
but as a general rule, S/C materials are more brittle
than Amorphous.
 The chain portions that are folded up in the crystal
restrict the polymer chains as they try to move past one
another when a force is applied making the S/C materials
more brittle.
 Polycarbonate is used in safety glasses, but General
Purpose Polystyrene (GPPS) is very brittle – both are
amorphous, but have different polymer structures.
 On the S/C side, Polyethylene is very ductile at room
temperature because it is above its Tg, but Nylon and
Polyester are brittle at room temperature.
Viscosity
 S/C materials by their very nature flow more easily than
Amorphous materials.
 The same mechanism that allows the material to fold up
into dense crystals allows the polymer chains to slide
past one another easily in the melted state.
Weather Resistance
 The most damaging aspect of weathering is generally
considered to be Ultraviolet light.
 The UV light breaks down the chains of the polymers
making them more brittle, causing colors to fade or
yellow, and causing additives in the polymers to migrate
to the surface (chalking).
 Amorphous polymers have better chemical resistance to
weathering effects than S/C polymers.
 The crystals in the S/C polymers diffract the light so the
UV rays spend more time within the polymer structure
and do more damage.
 The clear amorphous polymers allow the damaging
radiation to pass through doing less damage.
Shrinkage
 Because they fold up into crystal structures, S/C
materials have higher shrinkage rates when compared to
Amorphous materials.
 In injection molding most amorphous materials will
shrink between 0.003-0.007 in/in (0.3-0.7%)
 S/C materials shrink differently depending upon the
level of crystallinity that they achieve.
 Some will shrink over 0.025 in/in depending on
processing variables, part thickness, and additives.
Broad soflening range
thermal agitation of the molecules breaks down the weak
secondary bonds.
The rate at which this occurs throughout the formless
structure varies producing broad temperature range for
softening
Sharp melting point
the regular close-packed structure results in most of the
secondary bonds being broken down at the same time.
Crystalline vs Amorphous Thermoplastics
Crystalline (actually usually semi-crystalline):
Atomic bonds regular and repeated
Have a defined melting point Tm
Can contain some degree of amorphous polymer
Usually translucent to opaque
Amorphous
 Extensive chain branching
 All thermosets are amorphous
 Exhibit glass transition temperatures Tg
 Below Tg, polymer acts stiff and rigid
 Above Tg, polymer acts soft and rubbery
 Melt or liquefy over extended temperature range near Tg.
 Don’t have distinct Tm like crystalline polymers.
 Thermosetting polymers do not melt but degrade above Tg
Examples o amorphous and crystalline
thermoplastics
Amorphous
• Polyvinyl Chloride (PVC)
• Polystyrene (PS)
• Polycarbonate (PC)
• Acrylic (PMMA)
• Acrylonitrile-butadiene-
styrene (ABS)
• Polyphenylene (PPO)
Crystalline
• Polyethylene (PE)
• Polypropylene (PP)
• Polyamide (PA)
• Acetal (POM)
• Polyester (PEW, PBTF’)
• Fluorocarbons (PTFE,
• PFA, FEP and ETFE)

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CHAPTER FOUR final.pdf

  • 1.
  • 2. Amorphous polymer Morphology The bulk state, sometimes called the condensed or solid state, includes both amorphous and crystalline polymers Morphology : is a term used to describe the form or structure of the polymer chains of thermoplastic materials when they are in their frozen or solid state. • For thermoplastic resins, there are two basic morphologies: AMORPHOUS and SEMI-CRYSTALLINE • Amorphous polymers appear random and jumbled when allowed to cool in a relaxed state. They appear very similarly to their molten state, only the molecules are closer together. • They can be described as being similar to a large pot of spaghetti noodles.
  • 3. Amorphous materials are like cooked ramen noodles in that there is a random arrangement of the molecules and there are no crystals present to prevent the chains from flowing
  • 4.  It is important to remember that both materials have random, unordered arrangement when molten.  amorphous polymers exhibit different physical and mechanical behavior depending on temperature and structure.  At low temperatures, glassy, hard, and brittle. As the temperature is raised, they go through the glass–rubber transition.  Above Tg, cross-linked amorphous polymers exhibit rubber elasticity. An example is styrene–butadiene rubber (SBR)  An amorphous polymer does not exhibit a crystalline X- ray diffraction pattern, and it does not have a first-order melting transition.
  • 5. Example : • Polyvinyl Chloride (PVC) • General Purpose Polystyrene (GPPS) • Polycarbonate (PC) • Polymethylmethacrylate (PMMA or Acrylic) • Acrylonitrile Butadiene Styrene (ABS a terpolymer)
  • 6.  Older literature referred to the amorphous state as a liquid state.  However, polystyrene or poly(methyl methacrylate) at room temperature are glassy.  Today, amorphous polymers in the glassy state are better called amorphous solids.  >Tg, if the polymer is amorphous and linear, it will flow, albeit the viscosity may be very high.  For most materials, we are concerned with the melting point and boiling point.
  • 7. Glass Transition Temperature (Tg)  The glass transition temperature (Tg) is defined as the temperature at which the polymer softens because of the onset of long-range coordinated molecular motion.  For thermoplastic materials, we are concerned with: o Glass Transition Temperature o Melting Temperature  In amorphous materials, it is the temperature at which material behaves more rubber-like than glass-like.  Above Tg:  The material stretches further when pulled (more ductile)  The material absorbs more impact energy without fracturing when struck  When the material does fail, it fails in a ductile manner as opposed to a brittle manner
  • 8. The sample experienced a brittle failure The material broke like glass The sample broke in a ductile manner. The material yielded (stretched) before failure. The material behaved more like a rubber
  • 9. example: Polyethylene and Polypropylene both have low Tg’s. They are way below room temperature. That is why milk jugs and yogurt containers are flexible when you take them out of the refrigerator. Amorphous materials don’t truly have a Tm. They just continue to soften more until they behave more like a liquid. The molecules absorb enough energy and move far enough apart (increase the free volume) that the material can flow.
  • 11. Melt Temperature (Tm)  When we refer to the melt temperature for amorphous materials, it is usually the temperature at which we can process it.  For S/C materials, the Tm is the temperature at which the crystals melt.  If the polymer is crystalline Tm>Tg ideal temperature for growing crystals is approximately 2/3 of the way between the Tg and the Tm.  Not in all cases, but in many, the degradation temperature for S/C materials is not much higher than the melt temperature.
  • 12. Melting vs. Glass Transition Temp. What factors affect Tm and Tg?
  • 13. Factors affecting Tm Molecular chemistry and structure: - Molecular chemistry and structure will influence the ability of the polymer chain molecules to make rearrangements and, therefore, will also affect the Tm Chemical bonds: - The presence of double bonds and aromatic groups in the polymer backbone lowers chain flexibility and causes an increase in Tm. Size and type of side groups: - size and type of side groups influence chain rotational freedom and flexibility; Bulky or large side groups tend to restrict molecular rotation and raise Tm. The presence of polar groups:- leads to significant intermolecular bonding forces and relatively high Tm. Degree of branching:- The introduction of side branches introduces defects into the crystalline material and lowers the melting temperature.
  • 14. Factors Affecting Tg Molecular Weight – In straight chain polymers, increase in MW leads to decrease in chain end concentration resulting in decreases free volume at end group region – and increase in Tg Molecular Structure - Insertion of bulky, inflexible side group increases Tg of material due to decrease in mobility, Chemical cross-linking - Increase in cross- linking decreases mobility leads to decrease in free volume and increase in Tg Polar groups - Presence of polar groups increases intermolecular forces; inter chain attraction and cohesion leading to decrease in free volume resulting in increase in Tg.
  • 15. • The mechanical properties of polymers are sensitive to temperature changes Figure 1 Modulus versus temperature for an amorphous thermoplastic
  • 16. Figure 2. Modulus versus temperature for crystalline thermoplastics
  • 17. Figure 3. Modulus versus temperature for thermosetting resins
  • 18. Figure 4 Modulus versus temperature for a reinforced crystalline thermoplastic
  • 19. crystalline state • Both amorphous and crystalline areas in can exist in the same polymer. • Areas in polymer where chains packed in regular way. • X-ray scattering and electron microscopy have shown that the crystallites are made up of lamellae which,in turn, are built-up of folded polymer chains Schematic representation of (a) fold plane showing regular chain folding, (b) ideal stacking of lamellar crystals, (c) interlamellar amorphous model (d) fringed micelle model of randomly distributed crystallites (Plastic Technology Handbook)
  • 20. crystalline state • The crystalline state is defined as one that diffracts X- rays and exhibits the first-order transition known as melting. A first-order transition normally has a discontinuity in the volume– temperature dependence crystalline region amorphous region
  • 21. crystalline state  Polymers crystallized in the bulk, however, are never totally crystalline, a consequence of their long-chain nature and subsequent entanglements.  Crystallinity occurs when linear polymer chains are structurally oriented in a uniform three dimensional matrix.  Three factors that influence the degree of crystallinity are: i) Chain length ii) Chain branching iii) Interchain bonding iv) the rate of cooling during solidification
  • 22. Melting temperature observing  Non regularity of structure first decreases the melting temperature and finally prevents crystallinity.  crystalline materials have sharp X-ray pattern characteristic at Tm  Ideally, the melting temperature constitutes a first order phase change, should give a discontinuity in the volume, with a connected sharp melting point.  Due to polymer imperfections or very small size of the crystallites in bulk most polymers melt over a range of several degrees
  • 23. Specific volume–temperature relations for linear polyethylene • Open circles, specimen cooled relatively rapidly from the melt to room temperature; • solid circles, specimen crystallized at 130°C for 40 days, then cooled to room temperature
  • 24. The melting temperature is usually taken as the temperature at which the last trace of crystallinity disappears. melting temperature can be determined thermally. using the differential scanning calorimeter (DSC) gives the heat of fusion as well as the melting temperature
  • 25. methods for determining the percent crystallinity  most crystallizing polymers are semi-crystalline; that is, a certain fraction of the material is amorphous, while the remainder is crystalline  The reason why polymers fail to attain 100% crystallinity is kinetic, resulting from the inability of the polymer chains to completely disentangle and line up properly in a finite period of cooling or annealing. 1. Determination of the heat of fusion of the whole sample by calorimetric methods such as DSC
  • 26. Difference in heat out put of the two heaters vs temperature the latent heat of melting is the area of this peak the temperature at the top of the peak to be the polymer's melting temperature, Tm.
  • 27. DSC of a commercial isotactic polypropylene sample  DSC measure the heat flow in to or from a sample as is either heated or cooled heat of fusion ∆Hf is the area under the peak
  • 28. The percent crystallinity is then determined using the following equation: % crystallinity = Δ𝐻𝑚 − Δ𝐻𝑐 Δ𝐻𝑚𝑜 ∗ 100% Δ𝐻𝑚 is The heats of melting ΔHc is The heats of crystallization ΔHmo is a reference value and represents the heat of melting if the polymer were 100% crystalline are determined by integrating the areas (J/g) under the peaks }
  • 29. Example Polyethylene terephthalate (PET) is widely utilized for the production of food and beverage containers. The reference heat of melting for PET is 140.1 J/g and the result generated from DSC instrument show that the amount of heat for Cold crystallization at 101 0C is 1.65 J/g where the polymer undergoes some small amount of crystallization while heating in the DSC melting at 247 0 C is 46.5 J/g where the existing crystalline component is destroyed, determine the percentage of crystallinity? Soln % crystallinity = Δ𝐻𝑚 − Δ𝐻𝑐 Δ𝐻𝑚𝑜 ∗ 100% = 46.5 −1.65 140.1 ∗ 100% = 32%
  • 30.
  • 31. 2. Determination of the density of the crystalline portion via X-ray analysis of the crystal structure, and determining the theoretical density of a 100% crystalline material.
  • 32. s- density of a specimen for which the present crystallinity is to be determined. a- density of the completely amorphous polymer. c- density of the completely crystalline polymer.
  • 34. METHODS OF DETERMINING CRYSTAL STRUCTURE  There are four basic methods in wide use for the study of polymer crystallinity: X-ray diffraction, electron diffraction, infrared absorption, and Raman spectra X-Ray Methods  When a beam of x-rays impinges on a solid material, a portion of this beam will be scattered in all directions by the electrons associated with each atom or ion that lies within the beam’s path.
  • 35. Fig Diffraction of x-rays by planes of atoms (A–A’ and B–B’).  if the path length difference between 1-P-1’ and 2-Q-2’is equal to a whole number, n, of wavelengths.  That is, the condition for diffraction is nλ = 𝑆𝑄 + 𝑄𝑇
  • 36. crystalline substances must to act as a three-dimensional diffraction grating for X-rays Bragg equation : By considering crystals as reflection gratings. λ the X-ray wavelength θ the angle between the X-ray beam and these atomic planes n the order of diffraction
  • 37. X-Ray Methods  d and λ are of the order of 1 Å. Such an analysis from a single crystal produces a series of spots.  However, not every crystalline substance can be obtained in the form of macroscopic crystals.  This led to the Debye–Scherrer method of analysis for powdered crystalline solids or polycrystalline specimens.  The crystals are oriented at random so the spots become cones of diffracted beams.  can be recorded either as circles on a flat photographic plate or as arcs on a strip of film encircling the specimen
  • 38. The angle RSX is 2θ, where θ is the angle of incidence on a set of crystal plane X-Ray Methods
  • 39. X-Ray Methods Diffraction spot or line depends on the scattering power of the individual atoms( the number of electrons in the atom) the arrangement of the atoms with regard to the crystal planes the angle of reflection the number of crystallographically equivalent sets of planes contributing the amplitude of the thermal vibrations of the atoms.  intensities of the spots or arcs and their positions are required to calculate the crystal lattice
  • 40. Electron Diffraction of Single Crystals  Electron microscopy provides information about the very small, including a view of the actual crystal cell size and shape.  Electron diffraction studies utilize single crystals.  Since the polymer chains in single crystals are most often oriented perpendicular to their large flat surface, diffraction patterns perpendicular to the 001 plane are common.  Tilting of the sample yields diffraction from other planes. The interpretation of the spots obtained utilizes Bragg’s law in a manner identical to that of X-rays.
  • 41. Electron Diffraction of Single Crystals Required: Evacuated diffraction tube that contains an electron gun accelerating anode to provide a known energy to the electrons in the beam crystalline targets and screen
  • 42. Infrared Absorption The information that infrared absorption spectra yield about crystallinity: 1. Infrared spectra of semicrystalline polymers include“crystallization sensitive bands.” The intensities of these bands vary with the degree of crystallinity and have been used as a measure of the crystallinity. 2. By measuring the polarized infrared spectra of oriented semicrystalline polymers, information about both the molecular and crystal structure can be obtained. Both uniaxially and biaxially oriented samples can be studied. 3. The regular arrangement of polymer molecules in a crystalline region can be treated theoretically, utilizing the symmetry properties of the chain or crystal
  • 43. Raman Spectra 1. Since the selection rules for Raman and infrared spectra are different, Raman spectra yield information complementary to the infrared spectra. example, the S—S linkages in vulcanized rubber and the C=C bonds yield strong Raman spectra but are very weak or unobservable in infrared spectra. 2. Since the Raman spectrum is a scattering phenomenon, whereas the infrared methods depend on transmission, small bulk, powdered, or turbid samples can be employed. 3. the Raman spectra provide information equivalent to very low- frequency measurements, even lower than 10 cm-1. Such low frequency studies provide information on lattice vibrations.
  • 44. Polymer Single Crystals  crystallization is an allayment of molecular chain and folding of chain to get order region polymer single crystal formation 1) From precipitate (from dilute solutions, they form lamellar-shaped single crystals) 2) From melt
  • 45. Polymer Single Crystals 1) From precipitate  Ideas about polymer crystallinity start by preparing single crystals of polyethylene.  These were made by precipitation from extremely dilute solutions of hot xylene.  These crystals tended to be diamond-shaped and of the order of 100 to 200 Å thick
  • 46. 2. CRYSTALLIZATION FROM THE MELT usually super cool to greater or lesser extents crystallization temperature may be 10 to 20°C lower than the melting temperature Supercooling arises from the extra free energy required to align chain segments the most obvious of the observed structures are the spherulites spherulites are really spherical in shape only during the initial stages of crystallization
  • 48. Spherulites of low-density polyethylene Later spherulites interrupt on their neighbors then pervade the entire mass of the material
  • 49. The evolution of the spherulite
  • 50. KINETICS OF CRYSTALLIZATION  During crystallization from the bulk, polymers form lamellae,  which in turn are organized into spherulites or their predecessor structures  volume changes on melting; usually increasing
  • 51. The rate of crystallization increases as the temperature is decreased. This follows from the fact that the driving force increases as the sample is supercooled
  • 52. KINETICS OF CRYSTALLIZATION  Crystallization rates may also be observed microscopically :  by measuring the growth of the spherulites as a function of time  The isothermal radial(at 125°C) growth of the spherulites is usually observed to be linear
  • 53. KINETICS OF CRYSTALLIZATION  The increase in rate of crystallization as the temperature is lowered is controlled by the increase in the driving force  temperature is lowered still further, molecular motion becomes sluggish as the glass transition is approached, and the crystallization rate decreases again. linear growth rate versus crystallization temperature for poly(ethylene terephthalate) .Tf = 265°C, and Tg = 67°C, at which points the rates of crystallization are theoretically zero.
  • 54. KINETICS OF CRYSTALLIZATION  Below Tg, the rate of crystallization effectively becomes zero. rule-of-thumb  for determining a good temperature to crystallize a polymer  if the melting temperature(Tf) is known. where Tf is in absolute temperature. At (8/9) Tf the polymer is supposed to crystallize readily.
  • 55. Free energy of polymer crystallization  The classic melting temperature is usually taken where the last trace of crystallinity disappears, point A in Figure b.
  • 56. ∆Gf The free energy of fusion ∆Hf the molar enthalpy ∆Sf entropy of fusion  At the melting temperature, ∆Gf equals zero, and  smaller entropy or a larger enthalpy term raises Tf.  the relative changes in ∆Hf and ∆Sf in going from the amorphous state to the crystalline state determine the melting temperature of the polymer Free energy of polymer crystallization
  • 57. Properties Amorphous vs. S/C  Chemical Resistance  Optical Properties  Impact Resistance  Viscosity  Weather Resistance  Shrinkage
  • 58. Chemical Resistance  Plastic materials are used in virtually and contact with a wide variety of chemical substances that they need to resist As a general rule S/C materials are more resistant to chemical attack than amorphous materials. It is more difficult for the chemical media to penetrate the dense crystalline structure to damage the polymer chains. Polyethylene is used to store everything from detergent to mineral spirits to gasoline.
  • 59.  But Polypropylene is only slightly less chemically resistant than Polyethylene.  Of the amorphous materials PVC is probably the best in chemical resistance, mainly due to the large chlorine atom that helps to protect the main polymer chain.  Polycarbonate, Acrylic, Polystyrene and the other styrenics are all very susceptible to chemical attack, especially to mineral spirits and solvents like lacquer and paint thinners, alcohol, and gasoline.
  • 60. Optical Properties Amorphous materials have a much higher clarity than S/C materials. and can be translucent/optical quality. If the crystallinity is disrupted by adding a copolymer or other additive or by quenching the material so quickly the crystals don’t have enough time to form, the material may appear somewhat clear. Amorphous Acrylic more commonly known as Plexiglas and Polycarbonate used in safety glasses and optical lenses are far superior in terms of optical properties
  • 61. Impact Resistance  The material structure determines the impact resistance, but as a general rule, S/C materials are more brittle than Amorphous.  The chain portions that are folded up in the crystal restrict the polymer chains as they try to move past one another when a force is applied making the S/C materials more brittle.  Polycarbonate is used in safety glasses, but General Purpose Polystyrene (GPPS) is very brittle – both are amorphous, but have different polymer structures.  On the S/C side, Polyethylene is very ductile at room temperature because it is above its Tg, but Nylon and Polyester are brittle at room temperature.
  • 62. Viscosity  S/C materials by their very nature flow more easily than Amorphous materials.  The same mechanism that allows the material to fold up into dense crystals allows the polymer chains to slide past one another easily in the melted state.
  • 63. Weather Resistance  The most damaging aspect of weathering is generally considered to be Ultraviolet light.  The UV light breaks down the chains of the polymers making them more brittle, causing colors to fade or yellow, and causing additives in the polymers to migrate to the surface (chalking).
  • 64.  Amorphous polymers have better chemical resistance to weathering effects than S/C polymers.  The crystals in the S/C polymers diffract the light so the UV rays spend more time within the polymer structure and do more damage.  The clear amorphous polymers allow the damaging radiation to pass through doing less damage.
  • 65. Shrinkage  Because they fold up into crystal structures, S/C materials have higher shrinkage rates when compared to Amorphous materials.  In injection molding most amorphous materials will shrink between 0.003-0.007 in/in (0.3-0.7%)  S/C materials shrink differently depending upon the level of crystallinity that they achieve.  Some will shrink over 0.025 in/in depending on processing variables, part thickness, and additives.
  • 66. Broad soflening range thermal agitation of the molecules breaks down the weak secondary bonds. The rate at which this occurs throughout the formless structure varies producing broad temperature range for softening Sharp melting point the regular close-packed structure results in most of the secondary bonds being broken down at the same time.
  • 67. Crystalline vs Amorphous Thermoplastics Crystalline (actually usually semi-crystalline): Atomic bonds regular and repeated Have a defined melting point Tm Can contain some degree of amorphous polymer Usually translucent to opaque
  • 68. Amorphous  Extensive chain branching  All thermosets are amorphous  Exhibit glass transition temperatures Tg  Below Tg, polymer acts stiff and rigid  Above Tg, polymer acts soft and rubbery  Melt or liquefy over extended temperature range near Tg.  Don’t have distinct Tm like crystalline polymers.  Thermosetting polymers do not melt but degrade above Tg
  • 69.
  • 70. Examples o amorphous and crystalline thermoplastics Amorphous • Polyvinyl Chloride (PVC) • Polystyrene (PS) • Polycarbonate (PC) • Acrylic (PMMA) • Acrylonitrile-butadiene- styrene (ABS) • Polyphenylene (PPO) Crystalline • Polyethylene (PE) • Polypropylene (PP) • Polyamide (PA) • Acetal (POM) • Polyester (PEW, PBTF’) • Fluorocarbons (PTFE, • PFA, FEP and ETFE)