Axa Assurance Maroc - Insurer Innovation Award 2024
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.
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
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
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
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