miscibility and biodegradation studies of poly(lactic...
TRANSCRIPT
Miscibility and Biodegradation Studies of Poly(lactic acid) Blends
By
Ranjani DEVI (BSc, PGD Chem)
A Thesis Submitted in Partial Fulfillment of the
Requirements for the Degree of
Master of Science
School of Biological, Chemical and Environmental Sciences
Faculty of Science and Technology
The University of the South Pacific
2008
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This thesis is dedicated with heartfelt thanks to my parents Roop and Chandra Deo
for their encouragement, constant support and blessings to me through-out my research.
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ABSTRACT
Poly(lactic acid) (PLA) was blended with poly(vinyl butyral) (PVB), poly(vinyl
formal) (PVF), poly(styrene-co-acrylonitrile) (SAN) and ethylcellulose (EC) through
solution casting method using chloroform as the common solvent. The films obtained were
characterized for miscibility using Fourier Transform Infrared spectroscopy (FTIR),
Differential Scanning Calorimetry (DSC), microscopy and tensile testing.
FTIR analysis showed that there was no appreciable change in the spectra with
respect to blend composition. The spectra of the blends showed characteristic absorption
frequencies of the individual component polymers indicating that no intermolecular
interaction between the polymers occurred. However, PLA/PVB blends with less than 30
wt% PLA and PLA/PVF blends with less than 50 wt% PLA showed possibility of some
interaction occurring.
The DSC results showed that the glass transition temperature (Tg) of PLA and the
second polymer component in the binary blends remained more or less constant over the
entire composition range investigated. The existence of two Tgs in the blends indicated that
PLA/PVB, PLA/PVF, PLA/SAN and PLA/EC are immiscible polymer pairs. There was no
observable depression in the melting point of PLA in any of the blends. The degree of
crystallinity (Xc) of PLA phase remained constant with increasing PVB, PVF, SAN or EC
content in the blends.
Microscopy studies were in good agreement with FTIR and DSC results. They
showed phase separation in the blends. The illuminated regions signified the crystalline
phase of PLA while the dark regions identified the amorphous phase of PVB, PVF, SAN and
EC in the blends.
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Tensile strength and percent elongation decreased on blending in all the PLA blends
studied in this investigation.
Pure PLA showed higher rate of biodegradation than the blends. Degradation rate in
garden and rubbish dump soil in the natural environment was higher than in the same soils in
the controlled environment.
All the techniques used to determine miscibility indicated that PLA did not exhibit
any favorable thermodynamic or any intermolecular interaction with any of the polymers
employed in this research.
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ACKNOWLEDGEMENTS
I wish to thank my sponsors, NzAid and University of the South Pacific for providing me
with Graduate Assistant Scholarship for the duration of my research. I also wish to extend
my genuine gratitude to the University Research Committee and the Division of Chemical
Science for providing financial support to enable me to successfully carry out part of my
research work in Royal Melbourne Institute of Technology (RMIT), Australia.
My sincere thanks to my supervisor, Dr. Jagjit Khurma, for his steady guidance, assistance
and consistent encouragement to me throughout my research.
I also wish to express my heartfelt appreciation to my co- supervisor Prof. Robert Shanks at
RMIT for his supervision, his eagerness to assist, advice and most importantly his warm
hospitality during my stay in Melbourne.
I thank both the Chemical and Biological Science technical staff for their co-operation and
assistance throughout my research.
I am grateful to Mr and Mrs Bijend Prasad as well as Mr and Mrs Subhash Goundar for
providing me with accommodation and hospitality during my stay in Melbourne.
My humble appreciation to Dr. Kifle Kahsai for his valuable advice and encouragement,
which motivated me, believe in myself and aim higher.
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To my true friends, Kavita, Ranjeeta, Mohammed Shereez, Francis Mani, Shibani and
Yogita, who stood by me and encouraged me on when the going got tough. Thank you for
your faith and confidence in me.
Finally, no words can be sufficient enough to give due thanks to my dear parents and brother
for being the rock in my life.
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TABLE OF CONTENTS
Page
Declaration of Originality 3
Abstract 4
Acknowledgements 6
Table of Contents 8
Acronyms 12
Structures of Some Polymers 15
CHAPTER ONE
INTRODUCTION 18
1.1 Poly(lactic acid) and Its Blends 22
CHAPTER TWO
2.1 Literature Review 28
CHAPTER THREE
3.1 Materials 42
3.2 Study of the Blends
3.2.1 Preparation of the Films 42
3.2.2 Visual Observations 43
3.2.3 Fourier Transform Infrared Spectroscopy 43
3.2.4 Differential Scanning Calorimetry 44
3.2.5 Mechanical Analysis 44
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3.2.6 Optical Microscopy 44
3.2.7 Degradation of PLA and its Blends in Various Media 45
A. Biodegradation by Specific Microorganisms 45
I. Isolation of Microorganisms from Garden
and Rubbish Dump Soil 46
II. Characterization of Isolated Microorganisms 46
III. Preparation of Microbial Medium 46
i) Mineral Salts Solution 46
ii) Bacterial Trace-elements Solutions 47
iii) Medium Sterilization 47
IV. Sample Preparation and Disinfection 47
V. Culture Inoculation and Incubation 48
VI. Weight-Loss Determination 48
B. Degradation in the Natural Environment 49
I. Degradation in Garden Soil 49
II. Degradation in Rubbish Dump Soil 49
C. Degradation in Controlled Environment 49
I. Degradation in Garden Soil under Controlled
Conditions 49
II. Degradation in Rubbish Dump Soil under Controlled
Conditions 50
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CHAPTER FOUR
RESULTS
4.1 Visual Observations 51
4.2 Physical Appearance after Degradation 51
4.3 Fourier Transform Infrared Spectroscopy 51
4.3.1 Spectra of Homopolymers 51
4.3.2 Spectra of Blends 64
4.3.2.1 Poly(lactic acid)/Poly(vinyl butyral) 64
4.3.2.2 Poly(lactic acid)/Poly(vinyl formal) 64
4.3.2.3 Poly(lactic acid)/Poly(styrene-co-acrylonitrile) 65
4.3.2.4 Poly(lactic acid)/Ethyl Cellulose 65
4.4 Differential Scanning Calorimetry 88
4.4.1 Thermal Analysis of Homopolymers 88
4.4.2 Thermal Analysis of the Blends 90
4.4.3 Percentage Crystallinity 90
4.5 Mechanical Analysis of Homopolymers and their Blends 103
4.6 Microscopy 107
4.7 Degradation of PLA and its Blends in Various Media 121
4.7.1 Biodegradation by Microorganisms 121
4.7.2 Degradation in the Natural Environment 122
4.7.3 Degradation in Controlled Environment 127
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CHAPTER FIVE
DISCUSSION
SECTION A 133
5.1 Miscibility Studies 134
5.1.1 Poly(lactic acid) 134
5.1.2 Poly(lactic acid)/Poly(vinyl butyral) blends 137
5.1.3 Poly(lactic acid)/Poly(vinyl formal) blends 140
5.1.4 Poly(lactic acid)/Poly(styrene-co-acrylonitrile) blends 143
5.1.5 Poly(lactic acid)/Ethyl Cellulose blends 145
SECTION B 147
5.2 Degradation Studies of PLA and its Blends 147
5.2.1 Biodegradation 148
5.2.2 Degradation in the Natural Environment 149
5.2.3 Degradation in Controlled Environment 151
CHAPTER SIX
CONCLUSION 153
CHAPTER SEVEN
REFERENCE 156
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ACRONYMS
AFM Atomic Force Microscopy
ASTM American Society for Testing Materials
CB carbon black
DCM dichloromethane
DMTA Dynamic Mechanical Thermal Analysis
DOM dioctyl maleate
DSC Differential Scanning Calorimetry
DTA Differential Thermal Analysis
EC Ethyl Cellulose
ESCA Electron Spectroscopy for Chemical Analysis
FTIR Fourier Transform Infrared
GPC Gel Permeation Chromatography
H Enthalpy of fusion
IPS interpenetrated spherulites
IR Infrared
ISO/CEN International Standards Organization/European Committee for
Standardization
LA lactic acid
MA maleic anhydride
MDI Methylenediphenyl diisocyanate
MW molecular weight
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NaCl sodium chloride
NMR Nuclear Magnetic Resonance
o-CL oligo- -caprolactone
PBS Poly(butylene succinate)
P(BS-co-BC) Poly(butylene succinate-co-butylene carbonate)
PCL Poly( - caprolactone)
P(CL/L-LA) Poly( -caprolactone-L-lactide)
PEG Poly(ethylene glycol)
PEO Poly(ethylene oxide)
PEO-PPO-PEO Poly(ethylene oxide)-poly(propylene oxide)-poly(ethylene oxide)
PEVAc Poly(ethylene-co-vinyl acetate)
PIP Poly(cis-1,4-isoprene)
PLA Poly(lactic acid)
PLAGA Poly(lactic acid-co-glycolic acid)
PLA/EC PLA polymer and EC polymer blended together
PLA/PVB PLA polymer and PVB polymer blended together
PLA/PVF PLA polymer and PVF polymer blended together
PLA/SAN PLA polymer and SAN polymer blended together
PSA Poly(sebacic anhydride)
PVB Poly(vinyl butyral)
PVA Poly(vinyl alcohol)
PVAc Poly(vinyl acetate)
P(VAc-co-VA) Poly(vinyl acetate-co-vinyl alcohol)
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PVF Poly(vinyl formal)
SAN Poly(styrene-co-acrylonitrile)
SAXS Small Angle X-ray Scattering
SBF simulated body fluid
SEC Size Exclusion Chromatography
SEM Scanning Electron Microscopy
Tc Crystallization temperature
Tg Glass transition temperature
Tm Melting temperature
TEM Transmission Electron Microscopy
TGA Thermogravimetric Analysis
TMA Thermomechanical Analysis
UV Ultra Violet
WAXD Wide Angle X-ray Diffraction
WAXS Wide Angle X-ray Scattering
Xc percentage crystallinity
XPS X-ray Photoelectron Spectroscopy
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STRUCTURES OF SOME POLYMERS
Polymer Structure
Poly( - caprolactone)
(CH2)5 CO
O
n
Poly(ethylene oxide) O
CH2CH2
OCH2
CH2O
CH2
n
Poly(ethylene glycol) CH2
OCH2
n
CH2CH2
OH OH
Poly(isobutylene)
CH2 C
CH3
CH3
n
Poly(methylmethacrylate)
CCH2
C
CH3
OCH3
O
n
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Polymer Structure
Poly(phenylene oxide) CH3
CH3
O
n
Poly(propylene)CH2 CH
CH3
n
Poly(styrene)
CC
H H
H n
Poly(urethane)
C
O
O NH (CH2)n(CH2)n NH C
O
O
Poly(vinyl acetate) CHO
CH2
C
CH3
On
Poly(vinyl alcohol)
C CH OH
HH
n
16
Poly(vinyl chloride)
C CH
HH
n
Cl
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CHAPTER ONE
INTRODUCTION
Today, the polymer industry is one of the dominant and most progressive economic
forces. It is worth noting that the production of plastics is nearly two and a half times larger
than that of steel (Utracki, 1998). Plastics have become a vital part of our lives and are
affecting our lifestyles in various ways. They are continuously replacing traditional materials
such as metals, wood and ceramics (Andrady, 2003). The early growth of the plastics
industry was much slower than that of the synthetic-fiber and synthetic-rubber industries.
However, the growth of plastics industry has been very rapid since about 1940 (Seymour,
1971). In the past fifty years, polymers have totally changed human life. The plastic industry
has worked on synthesizing and formulating durable materials that are more adapted to their
specific uses. The increasing preference for plastics due to their versatile properties such as
non-reactive nature, high strength at a low cost has also prompted a corresponding interest in
discovering polymers with enhanced properties.
Wide varieties of materials have been obtained and commercialized using
copolymerization techniques such as graft and block copolymerization. However, developing
chemically new polymers is expensive. Polymer blending is a relatively low-cost technique
that has come into focus to yield polymer blends with superior properties. This involves
mixing two or more polymers to form a blend with preferred chemical and physical
properties. Polymer blends are physical mixtures of different polymers, not covalently
bonded at molecular level. Blending of polymers is an important area in polymer science and
it has undergone a rapid development in the recent years. Polymer blends constitute over
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30% of polymer consumption today with the annual growth rate of 9% (Nicholson, 1997).
Poly(phenylene oxide) and nylon blends are extensively used nowadays in manufacture of
fenders of automobiles. Poly(vinyl chloride) and poly(urethane) blends are being employed
in floor coverings, wire and cable insulation and packaging. Many hoses, rolls, footwear,
automotive accessories etc are made from poly(vinyl chloride) and nitrile rubber blends.
Poly(propylene) and poly(isobutylene) blends are used in manufacture of tarpaulins and
photographic films. Blends from poly(methylmethacrylate) and poly(methylacrylate) are
widely used to produce automobile parts, electrical devices, construction units, clear drink
containers, sports goods etc (Utracki, 1998).
There are several methods of blending, namely solution-mixing, melt-mixing and
reactive blending. In solution-mixing, two polymers which have been dissolved in a common
solvent are mixed together in required compositions. Evaporation of the solvent yields a
blend film. In melt-mixing, two polymers in powdered or pellet form are mixed together and
then melted mainly by using an extruder or a hot-press. Reactive-blending is where chemical
reactions are promoted between the two polymers in a molten state by introducing a reactive
third component with appropriate functional groups or a catalyst.
The blending of polymers is an area of importance as the material properties of the
polymer system may be readily altered. The principal reason for blending is developing
materials with a full set of desired properties, improving specific properties such as tensile
strength, rigidity, ductility, chemical resistance, barrier properties, abrasion resistance,
flammability, gloss etc. From the economic aspect, blending of an expensive polymer with a
low-cost polymer is cost effective. Blending requires a wide spectrum of information from
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the thermodynamic principles of miscibility and compatibilization to interphasial
characteristics, morphology, rheology and performance (Stevens, 1975).
Miscibility of a polymer system is determined by its free energy of mixing, Gmix.
Free energy of mixing depends on Hmix and Smix as shown by the equation
Gmix = Hmix - Smix
where Hmix is the enthalpy of mixing and Smix is the entropy of mixing.
For a polymer system to be completely miscible, Gmix should be negative and the
second derivative of free energy, 2 Gmix/ 2 should be positive where is the volume
fraction (Askadskii, 1996).
Miscibility of a polymer system can be defined as the capability of the two polymers
in the blend system mixing at any concentration without separation of the phases due to
favorable thermodynamic interactions and adhesion between the two polymers. The degree
of miscibility between two polymers depends on a number of factors such as crystallinity and
molecular weights of the polymers, blending technique, temperature at which blending is
carried out, thermodynamics of the blend system and kinetics (Miles et al., 1992). Miscibility
in the polymer blends results from strong interactions between the segments of the two
polymers. These specific interactions are hydrogen bonding, ion-dipole, dipole-dipole,
charge transfer and -bonding (Jiang et al., 1999).
The following techniques have been employed over the years in determining whether
a polymer binary system is miscible or immiscible:
Visual Observations – miscible blends appear transparent. If one polymer component
in the blend is crystalline, the film appears opaque but becomes transparent above
melting point. Immiscible blends normally appear opaque.
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Fourier Transform Infrared Spectroscopy (FTIR) - this is one of the most widely used
methods. FTIR analysis is used to determine the nature of interactions in the polymer
blends. Incompatible polymers do not show any shift in the absorption frequencies.
The spectrum of the blend exhibits absorption bands characteristic of individual
polymers used in the polymer blend. If a polymer system is miscible, the absorption
frequencies band shift indicating intermolecular interactions between specific
chemical groups of the component polymers.
Thermal Analysis – the most common technique used in thermal analysis is
Differential Scanning Calorimetry (DSC). This method is employed to determine
melting temperature (Tm), glass transition temperature (Tg), crystallization
temperature (Tc), enthalpy of fusion and amount of crystallinity in polymers. All
polymers exhibit unique Tg and it is the most popular way of determining miscibility.
Miscible systems show presence of a single intermediate Tg, depression in Tm and the
amount of crystallinity affected in the composites. Thermogravimetric Analysis
(TGA), Thermomechanical Analysis (TMA) and Dynamic Mechanical Thermal
Analysis (DMTA) are other techniques used in thermal analysis.
Mechanical Analysis – Young’s modulus, tensile strength and percent elongation can
also be used to determine miscibility. Improved mechanical properties in a polymer
blend indicate adhesion in the component polymers.
Microscopy – optical polarized microscopy used to view the different phases in the
blend. It is used to determine if the polymer phases are crystalline or amorphous. The
size and shape of spherulites present in a crystalline polymer can be viewed.
Immiscible polymer system is known to show phase separation while a miscible
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system shows homogeneity. Scanning Electron Microscopy (SEM) and Transmission
Electron Microscopy (TEM) are more sophisticated methods which require expert
operations.
Other techniques employed in miscibility studies are Nuclear Magnetic Resonance
(NMR) and X-Ray Scattering. These methods are very sophisticated and involve
skilled expertise.
1.1 Poly(lactic acid) and Its Blends
Advanced technology in petrochemical polymers has brought many benefits to mankind
and together with the non-degradable materials came the environment problem of their
disposal. The environmental impact of persistent plastic wastes is increasing and raising
global concern. Plastics account for around 18 percent of the volume of municipal solid
waste. Plastics waste is generated on land as well as the sea. As litter, plastics also present
problems. Plastic litter is hazardous to birds, fish and other animals that die from ingesting it
or becoming entangled in it. Litter on highways, beach and streets is definitely a sore-sight
and malignant to natural environment beauty (Stevens, 2001). Plastic disposal is regarded as
a serious environment problem that needs immediate and appropriate solution (Pranamuda et
al., 1999). Recently, the continuously growing concern of the public for the problem has
stimulated research interest in biodegradable polymers as alternatives to conventional non-
degradable polymers such as poly(ethylene) and poly(styrene)
Polymers made from natural resources are of twofold interest; consumption of crop
surplus and replacement of plastics derived from conventional petroleum polymers. Several
biodegradable polymers are now commercially available although, at present, their prices are
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much higher compared to the synthetic non-biodegradable polymers. Poly(lactic acid) (PLA)
is one such polymer being considered for use in a variety of industrial fields. PLA can be
utilized for both ecological and biomedical applications (Garlotta, 2001).
PLA belongs to the family of aliphatic polyesters and can be made from renewable
resources such as corn, whey, barley, sweet sorghum and sugarcane (Rafael, 2003). It is a
thermoplastic, of high strength and high modulus. It has very good physical, chemical and
mechanical properties. This completely biodegradable polymer can be used for making films,
containers for packaging and medical devices (Datta et al., 1995).
PLA is a semi-crystalline polymer. Its properties such as melting point, mechanical
strength and crystallinity, are determined by its polymer structure. The glass transition
temperature (Tg) of PLA lies between 50oC to 80oC while the melting temperature (Tm)
ranges from 1300C to 1800C. The extent of crystallinity and therefore, the melting point can
be easily varied depending on annealing and polymerization conditions. Amorphous and
crystalline PLA is soluble in chlorinated solvents such as dichloromethane (DCM) and
chloroform (CHCl3) (Hartmann, 1998).
Due to its high cost, PLA has been used mainly for specific purposes. However,
introduction of modern technologies, the production cost of PLA has come down (Drumright,
2001). Brittleness of PLA at room temperature is a major defect for many applications. In
order to modify various properties, studies on PLA blends with other polymers have been
carried out. It is known that PLA is able to form miscible blends with various polymers such
as poly(ethylene oxide) (Seth et al., 1997), poly(vinyl acetate) (Gajria., 1996), poly(ethylene
glycol) (Lai et al., 2003). As a result of this, use of PLA for food packaging, and other
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applications is increasing. This is still a very active research area in polymer blends and it is
expected many new blends with interesting properties will result from these efforts.
PLA is produced by polymerization of lactic acid (LA). The existence of both the
hydroxyl and carboxyl groups in lactic acid enables it to be converted into polyesters
directly. In general there are three methods to produce high molecular mass PLA of about
100,000 Dalton. These are:
direct condensation-polymerization
azeotropic dehydrative condensation
polymerization through lactide or lactic acid formation, which was developed by Cargill
Inc. in 1992 which is the most used mode of producing PLA.
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Figure 1. Synthesis methods of high molecular weight- PLA (Garlotta, 2001)
The synthesis of lactic acid into high molecular weight PLA can follow two different
routes of polymerization as depicted in Figure 1. Lactic acid is condensation polymerized to
yield a low molecular weight, brittle, glassy polymer, which is unusable for any applications,
unless external coupling agents are used to increase the molecular weight of the polymer.
The second route of producing PLA is to carry out ring opening polymerization of lactic acid
to yield high molecular weight PLA. Two types of ring opening polymerization can occur:
cationic and anionic polymerization.
PLA can undergo cationic ring opening polymerization where trifluoromethanesulfonic
acid (triflic acid) and methyl trifluoromethylsulfonate (methyl triflate) are the cationic
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initiators used to polymerize lactic acid. Polymerization proceeds via ester end groups which
yields an optically active polymer without racemization. The chain growth proceeds by
cleavage of the alkyl-oxygen bond. The propagation mechanism begins with the positively
charged lactic acid ring being cleaved at the alkyl-oxygen bond by SN2 attack by the triflate
anion. The triflate end group reacts with a second molecule of lactide again by SN2 reaction
to yield a positively charged lactic acid that is opened. The triflate anion opens the charged
lactic acid again and polymerization proceeds.
Figure 1.2. Cationic ring opening polymerization for PLA (Garlotta, 2001)
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Anionic polymerization proceeds by nucleophilic reaction of the anion with the carbonyl
and subsequent acyl-oxygen cleavage. This produces an alkoxide end group which continues
to propagate.
.
Figure 1.3. Anionic ring opening polymerization for PLA (Garlotta, 2001)
Due to the chiral nature of lactic acid, several distinct forms of PLA exist. Poly(l-lactic
acid) (PLLA) is the product resulting from polymerization of l-lactic acid. Polymerization of
d-lactic acid yields poly(d-lactic acid) (PDLA). The polymerization of a racemic mixture of
l-lactic acid and d-lactic acid leads to the synthesis of poly(dl-lactic acid) (PDLLA) which is
amorphous. In this study PLLA has been used.
The main objective of this research was to blend and study the miscibility of PLA with
Poly(vinyl butyral) (PVB), Poly(vinyl formal) (PVF), Poly(styrene-co-acrylonitrile) (SAN)
and ethylcellulose (EC) using FTIR, DSC, miscroscopy and tensile testing. In addition, the
blends were subjected to biodegradation by microorganisms isolated from the soil,
degradation in garden and rubbish dump soil in the natural environment and degradation in
garden and rubbish dump soil in a controlled environment.
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CHAPTER TWO
LITERATURE REVIEW
In the recent years, substantial attention has been paid to biodegradable polymers
mainly due to increase in interest for preservation of environment and substitution of
petrochemical polymers. Poly(lactic acid) (PLA) is one such polymer and is being considered
for use in a variety of industrial fields including car, computer and electrical appliances (Park
et al., 2004). PLA has unique physical properties that make it useful in diverse applications
including paper coating, films and serviceware, transparent food containers, blister packs and
cold drink cups (Drumright et al., 2000). PLA also has many potential uses in fibers and non-
wovens. It is easily converted into a variety of fiber forms using conventional melt-spinning
processes. PLA has a low density and excellent crimp and crimp retention. Some recent
potential applications include household and industrial wipes, diapers, feminine hygiene
products, disposable garments and UV resistant fabrics (Balkcom et al., 2002).
PLA has already become an important material in the medical industry, where it has
been in use for over 25 years. PLA is a bioresorable polymer, which means that it can be
assimilated by a biological system. Since the body can assimilate it, PLA has found
important applications in sustained release drug delivery systems. Its mechanical properties
and absorbability make PLA polymer an ideal candidate for implants in bone or soft tissue
(facial traumatology, orthopedic surgery, ophthalmology, orthodontics, local implants for
controlled release of anti-cancer drugs) and for resorbable sutures (eye surgery, conjunctional
surgery, surgery of the chest and abdomen). The mechanical, pharmaceutical and
bioabsorption characteristics are dependent on controllable parameters such as chemical
composition and molecular weight of the polymer (Balkcom et al., 2002).
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PLA has been blended with other polymer. The possible blends from a given set of
polymers offer better physical and chemical properties than do the individual polymers.
Miscibility and other properties such as thermal, mechanical and biodegradation of blends
have been investigated using various experimental techniques.
The condensation reaction product of PLA and a hydroxyl-terminated four-armed
poly( - caprolactone) (PCL) was studied using Size-Exclusion Chromatography (SEC), DSC
and NMR. The thermal stability and adhesive properties were measured for the different
formulations. The characterization results suggested the formation of a blend of PLA and a
block-copolymer of PLA and PCL. The results further indicated partial miscibility in the
amorphous phase of the blend showing only one glass-transition temperature (Tg) in most
cases. Differences in the morphology and in the adhesive properties were related to the
stereochemistry of PLA (Stolt et al., 2004). PLA – poly(caprolactone) [PCL] blend films
containing caprolactone- lactic acid block copolymer compatibilizer were prepared by
solvent casting and extrusion methods and their biodegradability were detected under the
conditions of in soil and in phosphoric acid buffer solution (pH = 7.2) by lipase. The surface
and bulk properties before and after degradation were evaluated by determining dynamic
contact angle and interfacial tension. The molding conditions gave the effect on the surface
and bulk structure and biodegradability of the polymer blend films (Kuriyama et al., 2001). A
study of the influence of random copolymer poly(lactide-co- -caprolactone) on the properties
of corresponding homopolymer blends was also conducted. Blends of the plain
homopolymers and blends containing 5 and 10 wt% of a copolymer of suitable composition
were prepared in the melt and characterized for their molecular interactions using thermal,
dynamic-mechanical, mechanical (tensile tests) and morphological analyses. The blends were
29
characterized by a good dispersion of the PCL minor phase into the PLA matrix and better
mechanical properties compared to plain PLA. Microporous blend membranes consisting of
PLA and PCL were then prepared by a phase inversion method and characterized by SEM.
The addition of compatibilising agent led to a highly homogenous structure while in absence
of compatibiliser a clear phase separation occurred (Aslan et al., 2000). Different processing
additives influencing the properties and the biodegradability of melt-pressed PLA and PCL
were monitored using SEC, DSC, contact angle measurements, infrared analysis (ATR-
FTIR) and Electron Spectroscopy for Chemical Analysis (ESCA). The melt-pressed films
were then subjected to pure fungal cultures Aspergillus fumigatus and Pencillium
simplicissimum and to composting. The study indicated that the degradation of the PLA films
was initially governed by chemical hydrolysis, followed by an acceleration of the weight
change and the molecular weight reduction which then remained unchanged during the
measurement period because of crystallization (Renstad et al., 1998). Oligo- -caprolactones
(o-CL) were utilised as principle secondary components within poly(lactic acid) blends. They
were also used as additives within larger-sized PCL/PLA blends. The aim was to fully
complement the mechanical attributes of the respective polyesters. DMTA shows that the
presence of o-CL plasticizers the PLA non-crystallization phase and the size of o-CL is
reduced. Moreover, it appears that the size of o-CL could also affect the static mechanical
properties of the ternary systems as material stiffness and strength reside between those
properties measured for high molecular weight PCL/PLA binary blends and the PLA
homopolymer (Lostocco et al., 1998). In another study PLA/PCL and PLA/Poly(ethylene
glycol) (PEG) blends were investigated by DSC and optical microscopy. PCL and PEG with
moderate molecular weight (MW=10000) were used as the blending components for PLA.
30
The crystallization rate of PLA could be enhanced upon blending with PCL. Since no
preferential nucleation at the domain interface was observed, the promotion of PLA
crystallization rate was attributed to its partial miscibility with PCL. PLA and PEG were
miscible in the melt over the composition range investigated (Yang et al., 1997). The effects
of mixing ratio of PLA and PCL on the thermal and mechanical properties and morphologies
of the solution cast blends were investigated by DSC, polarizing microscopy, tensile tests and
dynamic mechanical analysis. The presence of amorphous PLA did not disturb crystallization
of PCL over the PLA mole fraction from 0.1 to 0.9 and allowed PCL to form spherulites over
PLA mole fraction ranging from 0.1 to 0.6. The spherulite radius was larger for the blends
than for the pure PCL. Equations and parameters predicting these values of the blends were
proposed as function of composition (Tsuji et al., 1996). PLA was blended with PCL and
elastic -caprolactone-L-lactide copolymer [P(CL/LA)]. The mechanical properties and the
hydrolytic behaviour of the blends were investigated. The morphology of the blends affected
the degradation. The blends containing P(CL/LA) copolymer had a porous structure which
facilitated water absorption into the blend (Hiljanen et al., 1996).
Different types of starch have also been studied extensively with PLA. The effects of
the type of acetylated starch and the presence of PLA and ethanol on the functional properties
of extruded foams were evaluated and the specific mechanical energy requirements for
preparing these foams were compared. It was concluded that the functional properties (radial
expansion ratio, bulk density and compressibility) of acetylated potato starch-PLA and 25
and 70% amylose acetylated corn starch-PLA foams and the specific mechanical energy
requirements to prepare the foams were significantly affected by ethanol content, PLA
content and the type of acetylated starch (Guan et al., 2005). Hydrophobic PLA and
31
hydrophilic starch are thermodynamically immiscible leading to poor adhesion between the
two components, resulting in poor and irreproducible performance. The influence of a
polymeric dioctyl maleate (DOM), a derivative of maleic anhydride (MA), was researched on
the tensile strength and elongation of PLA/starch blends. MA is a nontoxic reactive
compatibilizer used to improve the mechanical properties of PLA/starch blends. DOM acted
as a compatibilizer at low concentations (below 5%) and markedly improved the tensile
strength of the blends. However, DOM functioned as a plasticizer at higher concentrations
(above 5%) and significantly enhanced elongation (Zhang et al., 2004). PLA/starch films
were exposed to ultraviolet (UV) treatment simulating UV exposure occurring in nature
before degradation in soil. The effects of UV light illumination on the degradation of
PLA/starch films in different media (liquid, inert and compost) according to International
Standards Organization/European Committee for Standardization (ISO/CEN) and American
Society for Testing Materials (ASTM) standard procedures were conducted. UV light
treatment showed visual degradation of the starch component and had an enhanced effect on
the degradation of PLA in the PL/starch films. Biodegradation of the films in different media
showed that the co-extruded films were biodegradable whatever the medium. The percentage
of biodegradation depended primarily on the nature of the medium and not on the procedure
used (Copinet et al., 2003). Two phase polymer blends of PLA and starch at various ratios
were prepared by using a laboratory-scale twin-screw extruder and compression molding.
Starch and PLA were immiscible polymers. Starch was used as filler in the starch and PLA
blends but the mechanical properties of the blends decreased significantly with increased
starch content (Ke et al., 2000). The effects of poly(vinyl alcohol) (PVA) concentrations and
molecular weights on the mechanical properties of starch/PLA blends were studied. PVA
32
and starch are polyols and hence starch forms continuous phase with PVA during blending.
The residual vinyl acetate group of PVA interacts with a hydrophobic PLA (Han et al.,
2004). Primary thermal properties and morphology of the blends were also characterized.
Tensile strength of the blends increased as PVA concentration increased up to 40% and
decreased as PVA molecular weight increased (Ke et al., 2003). Methylenediphenyl
diisocyanate (MDI) was found to improve the interfacial interaction between PLA and
granular starch. The effect of starch moisture content on the interfacial interaction of an
equal-weight blend of wheat starch and PLA containing 0.5% MDI by weight was
investigated. Addition of MDI improved the mechanical properties of the PLA/wheat starch
blends. Evidence from the microstructure, mechanical properties, dynamic mechanical
properties and water absorption showed that starch moisture affected the properties of
starch/PLA/MDI blends (Wang et al., 2002). To enhance the interfacial adhesion between
PLA and starch, gelatinized starches were prepared with various content of glycerol (Coffin
et al., 2003) and the effect of the glycerol addition on the characteristics of starch and its
blends were scrutinized. PLA and gelatinized starch were melt-blended using a twin screw
mixer. The blends were characterized by DSC thermal analysis, tensile strength and
morphological analysis. DSC data showed that starch played a role as a nucleating agent and
glycerol as a plasticizer. The combined effect contributed to an improvement in crystallinity
in the PLA blends. Mechanical properties and toughness of PLA/gelatinized starch blends
improved compared with PLA/pure starch blends (Park et al., 2000).
Poly(vinyl acetate-co-vinyl alcohol) copolymers [P(VAc-co-VA] were prepared by
acidic hydrolysis of poly(vinyl acetate) (PVAc) at various reaction time, and the degree of
hydrolysis was analyzed by 13C NMR. Blends of poly(lactic acid) (PLA) and P(VAc-co-VA)
33
were prepared by solvent casting method using chlor oform as a co-solvent. The PLA/PVAc
blends exhibited a single glass transition over the entire composition range, indicating that
the blends were miscible. On the contrary, for the blends with 10% hydrolyzed PVAc
copolymer, the phase separation and double glass transition were observed. With increasing
pure PVAc contents, the heat of fusion decreased and the melting peaks shifted to lower
temperature. The interaction parameter indicated negative values for up to 10% hyrolyzed
samples, but positive values at more than 20% hydrolyzed one. Small Angle X-ray Scattering
(SAXS) analysis revealed that the amorphous layer thickness increased with PVAc
composition, suggesting that a considerable amount of PVAc component located in the
interlamellar region. Polarized optical microscopy showed that the texture of spherulites
became rougher on increasing the PVAc content. In the case of P(VAc-co-VA) copolymer,
the intensity of polarized light decreased significantly, indicating that P(VAc-co-VA)
component seemed to be expelled out of the interfibrillar regions. SEM analysis revealed that
the significant phase separation occurred with increasing the degree of hydrolysis. In the case
of 70/30 blend of PLA and P(VAc-co-VA) with 30 mol% vinyl alcohol, the P(VAc-co-VA)
copolymer formed the regular domains with a size of about 10 m (Park et al., 2003).
Similar investigations were carried out with poly(vinyl acetate) (PVAc) where
miscibility, physical properties, degradation and surface morphology were characterized.
Gajria et al., (1996) investigated the miscibility and biodegradation of blends of PLA and
PVAc where the DSC results showed that the PLA/PVAc system is miscible since only one
Tg was observed. Results obtained from physical property testing indicated that the blends
exhibited synergism in the range of 5-30% PVAc due to interactions taking place in that
region. Enzymatic degradation studies showed that there was a vast difference in the weight
34
loss of pure PLA samples and the 95/5 PLA/PVAc blend. Surface tension results showed that
this was due to difference in the surface tension of pure PLA films and the 95/5 blend.
The thermo-oxidative degradation of poly(ethylene glycol)/poly(lactic acid)
(PEG/PLA) blends were investigated by Lai et al., (2003) where the blends were studied
using Infra-Red spectroscopy (IR), DSC, Gel Permeation Chromatography (GPC) and TGA.
The thermo- oxidative degradation of PEG occurred after a period time of aging in air at
80oC. The mechanism of thermo-oxidative degradation of PEG was found to be the random
chain scission of the main chain. As PLA blending with PEG, the existence of PLA appeared
to enhance the thermo-oxidative degradation of PEG. The enhancement of thermo-oxidative
degradation increased first and then decreased with the increase of PLA. The results could be
attributed to the ease of abstraction of the carboxylic hydrogen (-COOH) of PLA, which
enhanced the thermo-oxidative degradation of PEG. Also, the dilution effect of PLA on the
concentration of free radicals was an important factor of the thermo-oxidative degradation
PLA and poly(ethylene oxide) (PEO) blends were prepared by mechanical mixture
and homopolymers. Samples were subjected to vitro degradation tests (immersion in a
phosphate buffer solution with pH 7.4 at 37o). Independently of the blend composition, PEO
was dissolved after 14 days of immersion. As expected, after immersion, SEM showed that
the blends were porous, contrary to the samples, which were not immersed in the buffer
solution. Phase separation was not evident. Using DSC, the melting points of both PLA and
PEO crystallized fractions were observed and remained practically constant, indicating no
miscibility. TGA showed that the temperature where the main mass loss stage starts (Tonset),
depended on the blend composition and period of immersion in the buffer (Zoppi et al.,
2001). Melting and crystallization behavior of PLA in a mixture with PEO under high
35
pressure was studied by high pressure Differential Thermal Analysis (DTA). DSC, Wide
Angle X- ray Diffraction (WAXD) measurement and optical microscopy for the sample
formed by cooling from the melt under pressure were performed at 0.1 MPa. Pressure change
of melting temperature (Tm) of pure PLA in the mixture with PEO was detected by high
pressure DTA up to 400 MPa (Nafoku, 1997).
Melt-blended PLA with poly(butylene succinate) (PBS) was probed for phase
behavior, crystallization behavior and morphology using DSC, synchrotron Wide-Angle X-
ray Scattering (WAXS) and SAXS techniques. In the DSC analysis two distinct peaks were
observed over the entire composition range, indicating that the PLA and PBS blend systems
could be classified as semicrystalline-semicrystalline blends. A depression in the melting
point of PLA component via blending was also observed. The synchrotron WAXS revealed
that the two polymers underwent crystallization separately. Synchrotron SAXS data showed
well defined double-scattering peaks indicating that the PBS lamellae and PLA lamellae
formed at different locations (Park et al., 2002).
The miscibility of poly(butylene succinate-co-butylene carbonate)/poly(lactic acid)
P(BS-co-BC)/PLA) in various blend ratios was studied by DSC and the dependence of glass
transition temperature of the blends on the PLA content was determined. The morphology of
the blend and the radial spherulitic growth rates of P(BS-co-BC) and PLA were examined
using polarizing optical microscopy. The single glass transition temperature of the DSC
curves that changed according to the Fox equation indicated miscibility of P(BS-co-BC)/PLA
blends. P(BS-co-BC) spherulites continued to grow after the collision with PLA spherulites,
while PLA spherulites stopped growing. The change of birefringence of PLA spherulites
indicated the penetration of P(BS-co-BC) lamellae into PLA spherulites (Hirano et al., 2002).
36
In another study, the spherulitic morphology in P(BS-co-BC)/PLA) blends were
investigated by Atomic Force Microscopy (AFM) to obtain direct evidence for the formation
of interpenetrated spherulites (IPS), where the spherulites of P(BS-co-BC) penetrate into
PLA spherulites. The observation actually revealed that P(BS-co-BC) crystals penetrated into
interfibrillar regions of edge-on-lamellae in a PLA spherulite. The penetration process was
also investigated by AFM with a temperature controller. An edge-on PLA lamella or a fibril
that ran nearly perpendicular to the growth direction of a P(BS-co-BC) spherulite obstructed
the growth of P(BS-co-BC) spherulite. The P(BS-co-BC) crystals filled the blocked space
after growing around the PLA lamella. These results showed that the spherulites of P(BS-co-
BC) and PLA grow on the same layer instead of forming a layered structure of two
spherulites. All the results supported the formation of IPS (Ikehara et al., 2003).
Chemical and morphological analysis of surface enrichment PLA and poly(sebacic
anhydride) (PSA) blends were investigated using phase-detection imaging AFM. In addition
to detecting chemical and mechanical variations on polymer blend surfaces, phase-detection
imaging can improve the resolution and contrast of images on single- component films. This
was demonstrated by the identification of lamellae with widths of less than 5nm within PSA
spherulites (Chen et al., 199).
Homogenous blends of PLA with poly(aspartic acid-co-lactide) (PAL) were inspected
and the effects of PAL addition on the degradation rates of PLA in water, compost and soil
and on its thermal stability were examined. PAL, when added in small amounts, was reported
to have enhanced the degradation rate of PLA effectively. It also improved the thermal
stability of PLA containing an appreciable amount of residual catalyst (Shinoda et al., 2003).
37
Porous PLA scaffold was reinforced by chitin fibers and the structures of the
composites were characterized by SEM. The chemical characteristics of the chitin fibers were
evaluated by FTIR and X-ray Photoelectron Spectroscopy (XPS). From the results obtained it
was evident that after successful linkage with PLA, the chitin fibers reinforced the scaffold
much more effectively. The linked scaffold also had better structure and pore size thereby
increasing its potential in tissue engineering (Li et al., 2005). Furthermore, research has been
conducted in improving the water vapor barrier of chitosan by blending it with PLA.
Mechanical, thermal and barrier (water vapor permeability) properties and hydrophobicity of
the resultant blends were evaluated. Incorporation of PLA to chitosan improved the water
barrier properties and decreased the water sensitivity of chitosan film. Mechanical and
thermal properties revealed that chitosan and PLA blends were incompatible which was then
confirmed by FTIR analysis that showed the absence of specific interaction between chitosan
and PLA (Suyatma et al., 2004).
In another study biobased composites were obtained from PLA and cellulose fibers
(from newsprint). DMA results showed that the storage modulus of PLA increased on
reinforcements with cellulose fibers. DSC and TGA indicated that the presence of cellulose
fibers did not significantly affect the crystallinity or the thermal decomposition of PLA
matrix up to 30% cellulose fiber content concluding that recycled cellulose fibers from
newsprint could be a potential reinforcement for the high performance biodegradable
polymer composites (Huda et al., 2005). In a separate study, enzymatic degradation of PLA
and cellulose blend films was investigated. Trifluoroacetic acid solution of PLA and cellulose
was cast to prepare the blend films, which led to partial trifluoroacetylation of cellulose.
FTIR, DSC and WAXD analysis were performed on the blends and degraded by enzymes
38
such as proteinaze K and cellulase. According to the data, one hydroxyl group from each
glucose unit was esterified by trifluoroacetic acid and this trifluoroacetyl group was
hydrolyzed completely during degradation. Weight loss by proteinaze K for films containing
90% and 75% PLA were greatly increased compared to pure PLA due to large depression of
the crystallinity of the PLA component. Cellulase was only effective for the film comprising
of 100% cellulose (Nagata et al., 1998).
Composite scaffolds of PLA with bioactive wollastonite were fabricated by the
conventional solvent casting-particulate leaching method. Wollastonite is a naturally
occurring calcium silicate which has been widely used as filler in polymers to improve their
mechanical properties. SEM and simulated body fluid (SBF) were used for characterization.
Incorporation of wollastonite into PLA improved the hydrophilicity of the composites hinting
it to be a useful approach for the preparation of composite scaffold for tissue repair
applications (Li et al., 2004).
Recent investigation has been done on the influence of collagen on the physical
properties of PLA. The resulting PLA/collagen blended films were subjected to enzymatic
hydrolysis, tensile, bending and impact testing, thermal analysis and microscopy. A
dependence of PLA Tg and crystallinity on the blends was observed by DSC. SEM showed
PLA/collagen to be a partly compatible system. Introduction of collagen reduced the
mechanical properties. However, biodegradability increased with increasing collagen content
(Yang et al., 2004).
PLA has been blended with poly(cis-1,4-isoprene) (PIP), which is the major
ingredient of natural rubber, in an attempt to reduce brittleness. PLA/PIP blend was proved to
be incompatible, indicated by the presence of two Tg's, which were identical to the Tg of PLA
39
and PIP respectively. PVAc that is compatible with PLA was then grafted on PIP to yield
PIP-g-PVAc. This was then blended with PLA. PLA/ PIP-g-PVAc blend showed improved
tensile properties and much higher elongation and toughness values compared to PLA/PIP
blend (Jin et al., 2000).
Interrelationship between the filler dispersion state and the electrical property of
poly(ethylene-co-vinyl acetate) (PEVAc) and PLA blend filled with carbon black (CB)
composite was studied using SEM and electrical volume resistivity measurements. DMA
results suggested PEVAc/PLA to be an immiscible polymer blend since two Tg peaks were
seen. It was reported that the CB particles selectively located in the PEVAc formed
conductive networks in the PEVAc/PLA blend matrix to the networks in PEVAc single-
polymer matrix (Katada et al., 2005).
PLA was grafted to both ends of poly(ethylene oxide)-poly(propylene oxide)-
poly(ethylene oxide) (PEO-PPO-PEO) block copolymers to obtain amphiphilic P(LA-b-EO-
b-PO-b-EO-b-LA) block copolymer. The aggregation and gelation behaviors were studied.
The aggregation behavior was found to be complex because of the rather complicated block
structure. A reversible solution-gel transition was observed (Xiong et al., 2005).
In a study by Nguyen et al., 2003, Poly(lactic acid)-methoxypoly(ethylene glycol)
nanoparticles were synthesized. Incubation of the nanoparticles with human blood monocytes
was then performed in serum. It was observed that in serum, a protective effect was obtained
and the interaction of particles with mononuclear leukocytes decreased to 40%. Further
research has been carried out to develop a reproducible formulations of poly(lactic acid-co-
glycolic acid) (PLAGA) nanoparticles using several combinations of organic solvent and
surfactant. Optimal nanoparticles were produced using either acetone or ethyl acetate as the
40
organic solvent and PVA or human serum as the surfactant. The most critical measure of
performance of these nanoparticles proved to be their ability to re-suspend after freeze-drying
(Birnbaum et al., 2000).
41
CHAPTER THREE
METHODOLOGY
3.1 Materials
The following polymers were employed in this study:
i. Poly(lactic acid) (PLA)
ii. Poly(vinyl butyral) (PVB)
iii. Poly(vinyl formal) (PVF)
iv. Poly(styrene-co-acrylonitrile) (SAN)
v. Ethyl cellulose (EC)
All the polymers were purchased from Aldrich Chemicals and were used without further
purification. Analytical grade chloroform, also purchased from Aldrich Chemicals, was used
as the solvent for dissolving the polymers.
3.2 Study of the Blends
3.2.1 Preparation of the Films
Solution cast films of PLA, PVB, PVF, SAN and EC were prepared by firstly making
individual 2% (wt/vol) solutions of the polymers under study in chloroform. The solutions
were kept overnight with constant stirring to ensure that the polymers have dissolved
completely in the solvent. Solution of each polymer was then mixed with PLA solution in
various proportions to obtain blend solution containing different mass ratios of the polymers.
The resulting solutions were stirred thoroughly and left overnight to ensure that no phase
separation occurred. 10 cm3 of the blend solutions were cast onto glass petri dishes with a
42
75mm diameter to obtain films of uniform thickness. The petri dishes were covered with
watch glass in order to allow the solvent to evaporate slowly at room temperature. The films
were peeled off and dried in vacuum at 450C for several days to ensure complete removal of
residual solvent. The films were then stored in a desiccator for analysis use.
The films prepared as above were too thick for FTIR analysis. Therefore, the blend
solutions were cast onto sodium chloride (NaCl) disc and dried slowly at room temperature.
The resulting films were peeled off and mounted on cardholders. These films were also dried
in vacuum at 450C for several days and stored in the desiccator for FTIR analysis.
PLA30PVB, PLA50PVB and PLA70PVB blends were prepared using an IDM Hot
Press at 1800C. These films were analyzed for thermal properties using a DSC.
PLA50PVB film was prepared by letting the solvent vaporize at 550C. The resulting
film was scanned using DSC.
3.2.2 Visual Observations
All the different blend films were inspected for clarity by viewing them against
natural light.
3.2.3 Fourier Transform Infrared Spectroscopy (FTIR)
A Perkin-Elmer, Fourier Transform Infrared Spectrometer Spectrum was employed
for the infrared analysis. Spectra of all the samples were scanned at an average of sixty-four
scans using a resolution of 4cm-1 from 4000- 400cm-1. All the spectra were corrected for
baseline, normalized and saved. The instrumental software was used to analyze all the
spectra.
43
3.2.4 Differential Scanning Calorimetry (DSC)
Thermal analysis of the films was carried out using a Perkin Elmer DSC-6. Sample
weight ranged between 1-5 mg. Samples were scanned twice from 0oC to 220oC at a heating
rate of 10oC per minute under nitrogen flow. Two minutes holding time was allowed at
220oC and five minutes at 0oC in each scan for isothermal scanning of the blend films. Glass
transition temperature (Tg), melting temperature (Tm) and crystallization temperature (Tc) and
heat of enthalpy were obtained from the graphs.
3.2.5 Mechanical Analysis
The sample films were cut into 50mm x 10mm strips, the accurate dimensions were
measured using a digital vernier caliper. Thickness of the strips were measured at five
random points using a digital micrometer with an accuracy of + 0.001mm and averaged. Area
of each strip was calculated using these parameters. A Shimadzu Material Tester, following
the ASTM D882-90 was used to test for the tensile properties of the films. A load stress of -
10 - 100 N/mm2 was used. The crosshead speed was maintained at 5mm/min. Young’s
modulus, maximum tensile strength and elongation values were calculated using the
instrument’s software. All the measurements were repeated 3 times and the data presented
were the average values of each sample.
3.2.6 Optical Microscopy
Optical microscopy of the films was done at Royal Melbourne Institute of
Technology, Victoria, Australia, using an Olympus microscope fitted with a polarizer. The
films were cut into desired sizes, placed onto glass slides, covered with coverslips and
44
mounted onto a Mettler FP82HT Hot Stage and heated to 200oC and then cooled to room
temperature. The microphotographs were taken using a Nikon digital camera.
3.2.7 Degradation of PLA and its Blends In Various Media
A. Biodegradation by Specific Microorganisms
ASTM: D 5247- 92 which is a standard test method for determining the aerobic
biodegradability of degradable plastics by specific microorganisms was used as a guide. This
test method describes the procedures required to carry out a pure culture study for evaluating
the biodegradation of degradable plastics in submerged culture under aerobic conditions.
Degradation is evaluated by weight loss. This method follows the test method developed by
Lee et al., 1991 and is described below:
The films were cut into 2cm x 2cm sizes.
They were then chemically disinfected and aseptically dried. Initial weights of the films
were recorded.
The disinfected films were aseptically added to the appropriate growth medium incubated
with shaking for 24 hours at the appropriate temperature for the specific microorganism
being used. The medium was inoculated with a pure culture.
The inoculated and uninoculated control flasks were incubated with shaking for specific
period of time. Each film was evaluated with a minimum of four replicates.
The residual films were washed in 70% ethanol for 30 minutes and then dried.
Biodegradation by weight loss was determined.
45
I. Isolation of Microorganisms from Garden and Rubbish Dump Soil
Microorganisms from soil and rubbish dump soil were isolated and utilized in the
biodegradation study of the films. Each soil sample was subjected to the following
procedure.
Water was sterilized by autoclaving. 1g of soil was weighed and mixed in 99 mL of
sterile water. The resulting soil solution was diluted up to 1/10000. 1 mL of 1/1000 and
1/10000 solutions were plated onto plate count agar. The plates were incubated at room
temperature for 48 hours.
The number of colonies present were counted and well separated colonies were
isolated onto nutrient agar slants. The agar slants were then stored for degradation studies in
microbial medium.
II. Characterization of Isolated Microorganisms
One well separated colony from garden soil and one from the rubbish dump soil
was selected for microbial degradation of the films. These bacterial colonies were then
characterized by using some of the most widely used staining procedures. Both colonies
yielded gram- positive bacilli bacteria. Further staining and tests identified the bacterial
colony from garden soil as Mycobacterium and from rubbish dump soil as Bacillus.
III. Preparation of Microbial Medium
i. Mineral Salts Solution
This solution was prepared by dissolving the following amounts of reagents in 1L
of deionized water:
46
Sodium phosphate, dibasic 5.03g
Potassium phosphate, monobasic 1.98g
Magnesium sulfate 0.20g
Sodium chloride 0.20g
Calcium sulfate 0.05g
ii. Bacterial Trace-elements Solution
This solution was prepared by dissolving the following reagents in 1L
of deionized water:
Cupric sulfate 6.1g
Iron sulfate 1.1g
Manganese chloride 7.9g
Zinc sulfate 1.5g
One mL of trace-element solution was added to 1L of mineral salts solution to get the
resulting microbial medium. This medium is a carbon and nitrogen free solution and is of pH
7.1.
iii. Medium Sterilization
The microbial medium was sterilized by autoclaving at 1210C for 20 minutes.
IV. Sample Preparation and Disinfection
All the film samples were cut into 1cm x 1cm squares. 14 mL of polyoxyethylene
47
sorbitan monooleate (Tween 80 detergent) and 20 mL of chlorine bleach was added to about
98 mL of sterilized water to make a fresh solution of universal disinfectant.
The film samples were placed into the universal disinfectant and stirred at room
temperature for an hour. Different polymer blend films were placed separately at one time.
Using sterile forceps, the film samples were then placed in a beaker of fresh sterile water at
room temperature and stirred for at least an hour. The films were then transferred into a fresh
solution of 70% ethanol in a covered beaker for 30 minutes.
Each film sample was aseptically placed into a sterile pre-weighed Petri dish. The
dishes were stored at room temperature for 24 hours until the films had dried. The films were
further dried in the vacuum oven at room temperature for 1 hour before reweighing.
V. Culture Inoculation and Incubation
The disinfected films were aseptically added to the specimen jars containing 10
mL of sterile microbial medium inoculated with Mycobacterium. Each culture medium was
incubated in an orbital shaker at 125 r/min at 370C for 14 days. Each culture incubation was
performed in two replicates.
The same inoculation and incubation procedure was carried out for Bacillus.
Uninoculated control was carried out for all the samples where disinfected film samples were
aseptically placed in sterile microbial medium without microorganisms.
VI. Weight- Loss Determination
The residual films were washed with 70% ethanol for 30 minutes at room
48
temperature. They were then transferred to sterile petri dishes and dried at room temperature
for 24 hours. The films were further dried in the vacuum oven at room temperature for an
hour. The final weight of the films was determined and compared to that of the films in the
uninoculated control.
B. Degradation in the Natural Environment
I. Degradation in Garden Soil
This degradation study was carried out in the garden under natural conditions.
5 pre-weighed film samples of each blend were placed in the soil in triplicates over a period
of 5 months. Each triplicate sample set was removed after each progressive month and
washed in water followed by 70% ethanol. The films were dried for 24 hours at room
temperature and further dried in vacuum at 450C for an hour. The change in weight of the
samples was recorded.
II. Degradation in Rubbish Dump Soil
This investigation was carried out similar to the one for degradation in garden soil
except that the film samples were placed in the rubbish dump soil.
C. Degradation in Controlled Environment
I. Degradation in Garden Soil under Controlled Conditions
Soil from the garden was packed in plastic trays and placed in an insulated
cupboard where temperature was maintained at a constant 350C. The water content of the soil
was maintained at 50% of its saturated value i.e. the highest water holding capacity.
49
5 pre-weighed film samples of each blend were placed in the soil in triplicates over a
period of 5 months. Each triplicate sample set was removed after each progressive month and
washed in water followed by 70% ethanol. The films were dried for 24 hours at room
temperature and further dried in vacuum at 450C for an hour. The change in weight of the
samples was recorded.
III. Degradation in Rubbish Dump Soil under Controlled Conditions
This degradation study was carried out similar to that of garden soil under
controlled conditions except that rubbish dump soil was used for the study.
50
CHAPTER FOUR
RESULTS
4.1 Visual Observations
Pure PLA film was white and opaque confirming it to be a semi- crystalline polymer.
PLA/PVB blend films with PLA contents of 30 wt% or less were semi- transparent. Films
with more than 50 wt% PLA content were cloudy in appearance and not transparent.
PLA/PVF blends films with PLA contents of 10 wt% or less gave transparent films while the
films became cloudy with increasing PLA content. Films of blends of PLA/SAN of all
compositions appeared cloudy and became opaque with more than 50 wt% of PLA. Films of
blends of PLA/EC of all compositions were semi- transparent in appearance.
4.2 Physical Appearance after Degradation
All the samples showed signs of degradation after a month in the soil. After three
months the films had become discolored and brittle.
Blends of PVB, PVF and SAN had become hard and more opaque after four months.
They could be broken easily when rubbed. EC blends had network of holes in the film and
become fibrous. These films had almost degraded by the fifth month.
4.3 Fourier Transform Infrared Spectroscopy
4.3.1 Spectra of Homopolymers
I. Poly(lactic acid) (PLA)
As shown in Figure 4.1 PLA contains both the hydroxyl and carboxyl groups. Peaks
for these groups are seen clearly in the spectrum. The peak present at 3503cm-1 indicates the
51
presence of O-H. A strong peak at 1761cm-1 is due to the presence of C=O. All the major
peaks in PLA have been assigned and tabulated in Table 4.1.
52
Table 4.1 Assignment of major peaks in PLA
53
Wavenumbers
(cm-1)
Assignment
3503 O-H stretch (free)
2995 Asymmetrical stretching of CH
2945 Symmetrical stretching of CH
1761 C=O carbonyl stretch
1454 CH3 bend
1382 Asymmetrical deformation of CH
362 Symmetrical deformation of CH
1267 Bending mode of C=O
1188
1129
1096
Stretching mode of C-O
1046 O-H bend
955 C-C stretch
869 Absorption peak in crystalline phase
756 Absorption peak in the amorphous phase
II. Poly(vinyl butyral) (PVB)
Figure 4.2 shows the spectrum of PVB. PVB is a terpolymer and is synthesized from
PVA which in turn is obtained from PVAc. Acetate and hydroxyl groups therefore are
present in PVB. The broad peak at 3482cm-1 shows the presence of hydrogen bonded
54
hydroxyl group. The peak present at 1733 cm-1 is due to the presence of C=O of the acetate
group. Table 4.2 shows the major peaks present in PVB.
Table 4.2 Assignment of major peaks in PVB
Wavenumber
(cm-1)
Assignment
3482 O-H stretching (hydrogen bonded)
2957 Asymmetric stretching of C-H
2871 Symmetric stretching of C-H
2736 C-H stretch of aldehyde
1733 C=O stretch of amorphous carbonyl group
1433
1413
Deformation of CH2
1379 Asymmetric deformation of CH3
1342 Symmetric deformation of CH3
1239
1132
1054
999
Bending, stretching and scissoring modes
of C-O-C
55
56
III. Poly(vinyl formal) (PVF)
Chemical structure of pure PVF is similar to that of PVB therefore the spectrum of
PVF is very similar to that of PVB. Figure 4.3 shows the spectrum of PVF. PVF is derived
from the family of polymers formed from poly(vinyl alcohol) (PVA) and formaldehyde as
copolymers with poly(vinyl acetate) (PVAc). These reactions do not go to completion hence
PVF shows residual acetate and hydroxyl peaks in the spectrum. The broad peak at 3508 cm-1
is attributed to stretching due to O-H groups. The sharp peak at
1734 cm-1 is attributed to stretching due to C=O of the acetate group. The major peaks of
PVF have been assigned and are listed in Table 4.3.
Table 4.3 Assignment of the major peaks of PVF.
Wavenumbers
(cm-1)
Assignment
3508 Hydrogen bonded hydroxyl groups from alcohol.
2944 Asymmetrical stretch of aliphatic C-H.
2859 Symmetrical stretch of aliphatic C-H.
2776 C-H stretch of aldehyde.
1734 C=O stretch of amorphous carbonyl group.
1474 Bending of CH2 group attached to C=O group.
1432 Bending of CH2 attached away from C=O group.
1405 Peaks associated with CH2 group.
1393 Bending and rocking modes of C-H group.
57
1373
1242
Bending and rocking modes of C-H group.
1179
1132
1067
1020
Stretch, bending and rocking modes of C-O-C
group.
IV. Poly(styrene-co-acrylonitrile) (SAN)
SAN is a copolymer of styrene and acrylonitrile. Figure 4.4 shows the spectrum of
SAN. The major peaks in SAN have been assigned and tabulated in Table 4.4.
Table 4.4 Assignment of major peaks in SAN
Wavenumber
(cm-1)
Assignment
3082
3060
3027
Aromatic C-H stretching
2926 Tertiary C-H stretch
2857 Non-tertiary C-H stretch
2236 Nitrile C N stretch
1601 In plane stretching of aromatic ring
1493 C=C stretch in aromatic ring
1453 In plane bending of aromatic ring
58
1366
1155
In plane bending of C-C-H
1069
1028
In plane C-H bending
910 In plane stretching of aromatic ring
760
702
Out of plane deformation of C-H (in ring)
547 Out of plane deformation of C=C (in ring)
V. Ethyl Cellulose (EC)
EC is a versatile and thermoplastic polymer made from reaction of ethyl chloride with
alkali cellulose. The spectrum of EC is given in Figure 4.5 and the major peaks of EC are
shown in Table 4.5.
Table 4.5 Assignment of major peaks in EC
Wavenumber
(cm-1)
Assignment
3481 Hydroxyl group
2973
2870
Stretching C-H bands
1374 C-H bending
1099 C-O-C stretching vibration
59
60
61
6262
6363
4.3.2 Spectra of Blends
The following polymer blends were studied at various mass ratios and the spectra
were recorded at room temperature.
i. Poly(lactic acid)/ Poly(vinyl butyral)
ii. Poly(lactic acid)/ Poly(vinyl formal)
iii. Poly(lactic acid)/ Poly(styrene-co-acrylonitrile)
iv. Poly(lactic acid)/ Ethyl cellulose
4.3.2.1 Poly(lactic acid)/ Poly(vinyl butyral)
PLA/PVB blends were studied at various ratios and their spectra are shown in Figures
4.7 and 4.8. Figures 4.9 and 4.10 show blend-PVB difference spectra. To obtain the
difference spectrum, the peak at 3482 cm-1 in the spectra of the blends was reduced to zero.
Second derivative spectra of the carbonyl region were taken to obtain information about the
peaks which may be hidden due to overlapping. The second derivative spectra are given in
Figure 4.11.
4.3.2.2 Poly(lactic acid)/ Poly(vinyl formal)
The spectra of PLA/PVF blends at different ratios are shown in Figures 4.12 and
4.13. The blend-PVF difference spectra of the blends are shown in Figures 4.14 and 4.15.
The difference spectra were obtained by reducing the peak at 3508cm-1 to zero. Figure 4.16
shows the second derivative of the carbonyl region for the various blends of PLA and PVF.
64
4.3.2.3 Poly(lactic acid)/ Poly(styrene-co-acrylonitrile)
Figures 4.17 and 4.18 show the blend spectra of PLA/SAN at various ratios. The
blend-SAN difference spectra of the blends are shown in Figures 4.19 and 4.20. The peak at
2236cm-1 was reduced to zero to obtain the difference spectra. The second derivative of the
carbonyl region for all the PLA and SAN blends is given in Figure 4.21.
4.3.2.4 Poly(lactic acid)/ Ethyl Cellulose
The spectra of PLA/EC blends at various ratios are shown in Figures 4.22 and 4.23.
Figures 4.24 and 4.25 show the blend-EC difference spectra for the blends. The peak at
3481cm-1 was reduced to zero to obtain the difference spectra. Figure 4.26 shows the second
derivative of the carbonyl region for all the blends of PLA with EC.
65
6666
6767
6868
6969
7070
7171
7272
7373
7474
7575
7676
7777
7878
7979
8080
8181
8282
8383
8484
8585
Table 4.6. Area of crystalline and amorphous peaks from FTIR spectra of PLA/PVB blends
Blend Area of amorphous
peak
Area of crystalline
peak
Ratio
PLA 661 607 1.09
PVB10 799 993 0.80
PVB30 651 930 0.70
PVB50 400 812 0.49
PVB70 223 527 0.42
PVB90 92 336 0.27
Table 4.7. Area of crystalline and amorphous peaks from FTIR spectra of PLA/PVF blends
Blend Area of amorphous
peak
Area of crystalline
peak
Ratio
PLA 661 607 1.09
PVF10 351 480 0.73
PVF30 534 1154 0.46
PVF50 525 926 0.57
PVF70 596 1085 0.55
PVF90 424 620 0.68
86
Table 4.8. Area of crystalline and amorphous peaks from FTIR spectra of PLA/SAN blends
Blend Area of amorphous
peak
Area of crystalline
peak
Ratio
PLA 661 607 1.09
SAN10 216 454 0.48
SAN30 719 1317 0.55
SAN50 452 1972 0.23
SAN70 395 2150 0.18
SAN90 337 2466 0.14
Table 4.9. Area of crystalline and amorphous peaks from FTIR spectra of PLA/EC blends
Blend Area of amorphous
peak
Area of crystalline
peak
Ratio
PLA 661 607 1.09
EC10 889 1548 0.57
EC30 957 1769 0.54
EC50 854 1673 0.51
EC70 375 3042 0.12
EC90 319 - -
87
4.4 Differential Scanning Calorimetry (DSC)
4.4.1 Thermal Analysis of Homopolymers
Samples were scanned twice from 0oC to 220oC at a heating rate of 10oC per minute
under nitrogen flow. Two minutes holding time was allowed at 220oC and five minutes at
0oC in each scan for isothermal scanning of the blend films. The second heating scans of the
pure polymers showing the melting temperature (Tm), glass temperature (Tg), and
crystallization temperature (Tc) of PLA, PVB, PVF, SAN and EC are shown in Figure 4.27.
A double melting peak around 1620C and 1680C in the PLA thermogram relates to the
melting of PLA crystals. No melting peaks were seen for PVB, PVF, SAN and EC, however,
Tg was observed.
Tg of the polymers are shown in Table 4.10. The Tg of EC was not evident in the
thermogram. However, it has been reported to be in the 125-1300C range. In PLA
crystallization, a peak was observed after glass transition which appreared at 1110C while
other polymers do not show this property. Thermal results of the homopolymers are shown in
Table 4.10. Literature values of these polymers are shown in brackets in the same table.
Table 4.10 Thermal results of the Homopolymers
Polymer Tm (0C) Tg (0C) Tc (0C) Xc
PLA 162, 168(130-1800C)
63(50-800C)
111 40.7(37.0)
PVB - 71(51-610C)
-
PVF - 105(1050C)
-
SAN - 102(99-1050C)
-
EC - - (125-1300C)
-
88
8989
4.4.2 Thermal Analysis of the Blends
Figures 4.28-4.35 display the DSC scans for the PLA blends. The first and second
heating cycles of the DSC scans for all the blends are given. The thermograms are arranged
vertically in order of decreasing PLA content in the blends, with the thermogram of the blend
with 90 wt% PLA at the bottom and 10 wt% PLA at the top.
The thermal results of the blends are presented in Tables 4.11 - 4.16. Tm, Tc and Tg
are shown in columns 3, 4 and 5 respectively.
4.4.3 Percentage Crystallinity (Xc)
PLA is a semi- crystalline polymer and it can exist as amorphous or crystalline phase
in the blends. The amount of crystalline PLA in the blends was calculated using the
enthalpies of fusion of the blends and of pure PLA crystal which were determined by the
instrument’s software. The Xc in the blends was estimated according to the following
equation
Xc = Hm/ ØPLA x 100%
Hom
where Hm and Hom are the enthalpies (J/g) of fusion of blend and PLA crystal of infinite
size with a value of 93.6 J/g respectively and ØPLA is the PLA fraction in the blend (Garlotta,
2001).
Percentages of crystallinity present in the different blends are shown in the last
columns of Tables 4.11 - 4.16.
90
Pure PLA was calculated to have a percentage crystallinity of 40.7 as shown in Table
4.10. Literature value is around 37% (Garlotta, 2001).
91
9292
9393
9494
9595
9696
9797
9898
9999
Table 4.11 Thermal analysis results of PVB blends from the second heating
Blend H
J/g
Tm
(0C)
Tc
(0C)
Tg
(0C)
Xc
PVB 10 34.0 162, 168 113 63 40.3
PVB30 26.5 165, 169 124 63, 71 40.4
PVB 50 18.0 164 125 63, 72 38.5
PVB 70 10.0 164 123 61, 72 35.6
PVB 90 3.7 163 120 62, 72 39.5
Table 4.12 Thermal analysis results of PVF blends from the second heating
Blend H
J/g
Tm
(0C)
Tc
(0C)
Tg
(0C)
Xc
PVF 10 34.7 163, 169 113 60 41.2
PVF30 26.2 163, 169 114 60 40.0
PVF 50 25.1 168 114 60 53.6
PVF 70 12.7 166 103 59 45.3
PVF 90 4.1 166 - 103 43.8
100
Table 4.13 Thermal analysis results of SAN blends from the second heating
Blend H
J/g
Tm
(0C)
Tc
(0C)
Tg
(0C)
Xc
SAN 10 33.2 162, 170 112 60 39.4
SAN 30 19.8 164 131 60 30.2
SAN 50 17.6 164 129 59 37.6
SAN 70 15.3 164 127 58 54.5
SAN 90 3.9 164 - 58, 105 41.2
Table 4.14 Thermal analysis results of EC blends from the second heating
Blend H
J/g
Tm
(0C)
Tc
(0C)
Tg
(0C)
Xc
EC 10 33.4 160, 166 123 60 39.6
EC 30 28.7 157, 163 120 60 43.8
EC 50 20.5 154, 160 123 60 43.8
EC 70 12.5 158, 165 112 58 44.5
EC 90 1.7 165 - 57 18.2
101
Table 4.15 Thermal analysis results of Hot-pressed PLA/PVB blends from the second
heating
Blend Heat of fusion ( H)
J/g
Tm
(0C)
Tc
(0C)
Tg
(0C)
Xc
PVB30 27.8 164 98 59, 72 42.4
PVB50 18.8 167 100 59, 72 40.2
PVB70 11.5 163 98 57, 71 41.0
Table 4.16 Thermal analysis results of PLA/PVB blend prepared at 550C from the second
heating
Blend Heat of fusion ( H)
J/g
Tm
(0C)
Tc
(0C)
Tg
(0C)
Xc
PVB50 21.3 164 124 60, 73 45.5
102
4.5 Mechanical Analysis of Homopolymers and their Blends
Tensile strength results and percent elongation for pure polymers and their blends
with PLA are summarized in Figures 4.36- 4.43.
0
5
10
15
20
25
30
35
40
45
50
PVB
PLA
10
PLA
30
PLA
50
PLA
70
PLA
90
PLA
Tens
ile s
tren
gth
(x10
6 N/m
2 )
Figure 4.36 Tensile strength of PLA/PVB Blends
0
10
20
30
40
50
60
70
80
PV
B
PLA
10
PLA
30
PLA
50
PLA
70
PLA
90
PLA
% E
long
atio
n
Figure 4.37 Percentage Elongation of PLA/PVB Blends
103
0
5
10
15
20
25
30
35
PVF
PLA
10
PLA
30
PLA
50
PLA
70
PLA
90
PLA
Tens
ile S
tren
gth
(x10
6 N/m
2 )
40
Figure 4.38 Tensile Strength of PLA/PVF Blends
0
5
10
15
20
25
30
PV
F
PLA
10
PLA
30
PLA
50
PLA
70
PLA
90
PLA
% E
long
atio
n
Figure 4.39 Percentage Elongation of PLA/PVF Blends
104
0
10
20
30
40
50
60
SA
N
PLA
10
PLA
30
PLA
50
PLA
70
PLA
90
PLA
Tens
ile S
tren
gth
(x10
6N
/m2 )
Figure 4.40 Tensile Strength of PLA/SAN Blends
0
1
2
3
4
5
6
7
8
SA
N
PLA
10
PLA
30
PLA
50
PLA
70
PLA
90
PLA
% E
long
atio
n
Figure 4.41 Percentage Elongation of PLA/SAN Blends
105
0
5
10
15
20
25
30
35
40
EC
PLA
10
PLA
30
PLA
50
PLA
70
PLA
90
PLA
Tens
ile S
tren
gth
(x10
6N
/m2 )
Figure 4.42 Tensile Strength of PLA/EC Blends
0
1
2
3
4
5
6
7
8
EC
PLA
10
PLA
30
PLA
50
PLA
70
PLA
90
PLA
% E
long
atio
n
Figure 4.43 Percentage Elongation of PLA/EC Blends
106
4.6 Microscopy
The micrographs of PLA and PLA blends with PVB, PVF, SAN and EC are shown in
the following photographs. Optical micrograph 4.1 was taken without the use of a polarizer,
therefore, the crystallites in pure PLA are not evident. Polarized light improves the quality of
image obtained with birefringent materials. The film of pure PLA was photographed using a
polarizer shown in Polarized optical micrograph 4.2. The PLA crystallites are very clearly
seen. Polarized optical micrograph 4.3 very clearly presents the “Maltese Cross” shaped PLA
crystallite. Polarized optical micrograph 4.4 shows distribution of PLA crystallites with
ranging diameter.
Polarized optical micrographs 4.5 - 4.28 show the distribution of PLA crystallites in
the blends.
Optical micrograph 4.1 Pure PLA film taken without a polarizer (400x)
107
Polarized optical micrograph 4.2 Crystallites in pure PLA (400x)
Polarized optical micrograph 4.3 PLA spherulite in pure PLA film(400x)
108
Polarized optical micrograph 4.4 Crystallites in pure PLA film (400x)
Polarized optical micrograph 4.5 Amorphous pure PVB (400x)
109
Polarized optical micrograph 4.6 PLA crystallites in PVB90 blend (400x)
Polarized optical micrograph 4.7 PLA crystallites in PVB70 blend (400x)
110
Polarized optical micrograph 4.8 PLA crystallites in PVB50 blend (400x)
Polarized optical micrograph 4.9 PLA crystallites in PVB30 blend (400x)
111
Polarized optical micrograph 4.10 PLA crystallites in PVB10 blend (400x)
Polarized optical micrograph 4.11 Amorphous pure PVF (400x)
112
Polarized optical micrograph 4.12 PLA crystallites in PVF10 (400x)
Polarized optical micrograph 4.13 PLA crystallites in PVF30 blend (400x)
113
Polarized optical micrograph 4.14 PLA crystallites in PVF50 blend (400x)
Polarized optical micrograph 4.15 PLA crystallites in PVF70 blend (400x)
114
Polarized optical micrograph 4.16 PLA crystallites in PVF90 blend (400x)
Polarized optical micrograph 4.17 Amorphous pure SAN (400x)
115
Polarized optical micrograph 4.18 PLA crystallites in SAN10 blend (400x)
Polarized optical micrograph 4.19 PLA crystallites in SAN30 blend (400x)
116
Polarized optical micrograph 4.20 PLA crystallites in SAN50 blend (400x)
Polarized optical micrograph 4.21 PLA crystallites in SAN70 blend (400x)
117
Polarized optical micrograph 4.22 PLA crystallites in SAN90 blend (400x)
Polarized optical micrograph 4.23 Amorphous pure EC (400x)
118
Polarized optical micrograph 4.24 PLA crystallites in EC90 blend (400x)
Polarized optical micrograph 4.25 PLA crystallites in EC70 blend (400x)
119
Polarized optical micrograph 4.26 PLA crystallites in EC50 blend (400x)
Polarized optical micrograph 4.27 PLA crystallites in EC30 blend (400x)
120
Polarized optical micrograph 4.28 PLA crystallites in EC10 blend (400x)
4.7 Degradation of PLA and its Blends In Various Media
PLA is considered to be biodegradable as well as compostable. PLA and its blends were
tested under different environmental conditions: controlled as well as natural and in different
soil types. In addition biodegradability of PLA and its blends were determined by specific
microorganisms isolated from two different types of soil.
4.7.1 Biodegradation by Microorganisms
Percentage mass losses of PLA and its blends in mineral broth media inoculated with
Mycobacterium isolated from garden soil and in mineral broth media inoculated with
Bacillus isolated from rubbish dump soil over the incubation period of 14 days were studied.
121
4.7.2 Degradation in Natural Environment
Degradation of PLA and its blends were carried out in garden soil in the
natural environment. Figures 4.44 - 4.48 show the average percentage mass losses over the
period of 5 months.
01020304050607080
0 1 2 3 4 5 6
M onths
% M
ass
Loss
Figure 4.44 Degradation of pure PLA film in garden soil in the natural environment
-20
0
20
40
60
0 2 4 6
Months
% M
ass
Loss
PLA30PVB70PLA50PVB50PLA70PVB30
Figure 4.45 Degradation of PLA/PVB blends in garden soil in the natural environment
122
-100
102030405060
0 2 4 6Months
% M
ass
Loss
PLA30PVF70PLA50PVF50PLA70PVF30
Figure 4.46 Degradation of PLA/PVF blends in garden soil in the natural environment F blends in garden soil in the natural environment
-100
102030405060
0 2 4 6
Months
% M
ass
Loss
PLA30SAN70PLA50SAN50PLA70SAN30
Figure 4.47 Degradation of PLA/SAN blends in garden soil in the natural environment Figure 4.47 Degradation of PLA/SAN blends in garden soil in the natural environment
123
-50
0
50
100
150
0 1 2 3 4 5 6
Months
% M
ass
Loss
PLA30Ec70PLA50Ec50PLA70Ec30
Figure 4.48 Degradation of PLA/EC blends in garden soil in the natural environment garden soil in the natural environment
Figures 4.49- 4.53 show the average percentage mass losses over the period of 5 months for
the degradation of PLA and its blends that were carried out in rubbish dump soil in the
natural environment.
Figures 4.49- 4.53 show the average percentage mass losses over the period of 5 months for
the degradation of PLA and its blends that were carried out in rubbish dump soil in the
natural environment.
0
20
40
60
80
100
120
0 1 2 3 4 5 6
Months
% M
ass
Loss
Figure 4.49 Degradation of pure PLA film in rubbish dump soil in the natural environment Figure 4.49 Degradation of pure PLA film in rubbish dump soil in the natural environment
124
-20
0
20
40
60
80
0 2 4 6
Months
% M
ass
Loss
PLA30PVB70PLA50PVB50PLA70PVB30
Figure 4.50 Degradation of PLA/PVB blends in rubbish dump soil in the natural environment
-100
10203040506070
0 2 4 6Months
% M
ass
Loss
PLA30PVF70PLA50PVF50PLA70PVF30
Figure 4.51 Degradation of PLA/PVF blends in rubbish dump soil in the natural environment
125
-10
0
10
20
30
40
50
0 2 4 6
Months
% M
ass
Loss
PLA30SAN70PLA50SAN50PLA70SAN30
Figure 4.52 Degradation of PLA/SAN blends in rubbish dump soil in the natural environment
-50
0
50
100
150
0 2 4 6
Months
% M
ass
Loss
PLA30Ec70
PLA50Ec50
PLA70Ec30
Figure 4.53 Degradation of PLA/EC blends in rubbish dump soil in the natural environment
126
4.7.3 Degradation in Controlled Environment
Degradability of PLA and its blends was determined in garden soil maintained in
a controlled environment where temperature was kept at a constant 350C and water content
kept at 50% of its saturated value. Average percentage mass loss of PLA and its blends are
shown in Figures 4.54- 4.58.
0
10
20
30
40
50
60
70
0 1 2 3 4 5
Months
% M
ass
Loss
6
Figure 4.54 Degradation of pure PLA film in garden soil at 35oC with constant water content
127
-10
0
10
20
30
40
0 2 4 6
Months
% M
ass
Loss
PLA30PVB70PLA50PVB50PLA70PVB30
Figure 4.55 Degradation of PLA/PVB blends in garden soil at 35oC with constant water ontent
56 Degradation of PLA/PVF blends in garden soil at 35oC with constant water ontent
c
-10
0
10
20
30
40
50
0 2 4 6
Months
% M
ass
Loss
PLA30PVF70PLA50PVF50PLA70PVF30
Figure 4.c
128
05
101520253035
0 2 4 6
Months
% M
ass
Loss
PLA30SAN70PLA50SAN50PLA70SAN30
Figure 4.57 Degradation of PLA/SAN blends in garden soil at 35oC with constant water ontent
58 Degradation of PLA/EC blends in garden soil at 35oC with constant water ontent
c
05
1015202530354045
0 2 4 6
Months
% M
ass
Loss
PLA30Ec70PLA50Ec50PLA70Ec30
Figure 4.c
129
Rubbish dump soil also kept in a controlled environment with a constant temp
of 350C and 50% of its saturated water content was used to determine the degradability of
PLA and its blends. The results are shown in Figures 4.59- 4.63.
erature
igure 4.59 Degradation of pure PLA film in rubbish dump soil at 35oC with constant water
Figure 4.60 Degradation of PLA/PVB blends in rubbish dump soil at 35oC with constant water content
05
101520253035404550
0 1 2 3 4 5 6
Months
% M
ass
Loss
Fcontent
Power (PLA30PVB70)Power (PLA50PVB50)Expon. (PLA70PVB30)
00
1020304050
2 4 6
Months
% M
ass
Loss
130
05
10152025303540
0 1 2 3 4 5 6
Months
% M
ass
Loss
PLA30PVF70PLA50PVF50PLA70PVF30
Figure 4.61 Degradation of PLA/PVF blends in rubbish dump soil at 35oC with constant water content
-10
0
10
20
30
40
0 2 4 6
Months
% M
ass
Loss
PLA30SAN70PLA50SAN50PLA70SAN30
Figure 4.62 Degradation of PLA/SAN blends in rubbish dump soil at 35oC with constant water content
131
05
1015202530354045
0 1 2 3 4 5 6
Months
% M
ass
Loss
PLA30Ec70PLA50Ec50PLA70Ec30
Figure 4.63 Degradation of PLA/EC blends in rubbish dump soil at 35oC with constant water content
132
CHAPTER FIVE
DISCUSSION
This chapter is divided into two sections. Section A discusses the miscibility study of the
PLA blends using FTIR, DSC, microscopy analysis and mechanical properties. Section B
discusses degradation studies of PLA and its blends.
Section A
Miscibility Studies
In this section miscibility of PLA with PVB, PVF, SAN and EC is discussed. The
structures of these polymers are given in Table 5.
Table 5. Structures of polymers
Polymer Abbreviation Structure
Poly(lactic acid) PLA
C
O
CH
CH3
O
n
Poly(vinyl butyral) PVB
CH 2 CH CH 2 CH
nO O
CH
C 3H 7
133
Poly(vinyl formal) PVFCH2 CH CH2 CH
nO O
CH2
Poly(styrene-co-
acrylonitrile)
SANCH2 CH CH2 CH
C6H6 CN n
Ethyl cellulose EC
For a polymer system to be miscible, it should exhibit the following characteristics:
There is no phase separation in solution form.
The blend films should normally appear transparent.
There is homogeneity in the microstructure with uniform distribution of the two
phases.
Infrared analysis shows shifts in the absorbance frequency of the peaks.
Thermal analysis shows a single glass transition temperature for the polymer blends.
Depression in the melting point and decrease in the percentage crystallinity for blends
of crystalline polymers.
5.1.1 Poly(lactic acid)
Infrared spectroscopy is useful to study the hydrogen bonding and other interactions
134
as well as the miscibility of the polymer blends. PLA is capable of forming miscible blends
with a number of polymers. Intermolecular interactions are responsible for the miscibility of
PLA with other polymers. In many miscible blend systems, one polymer containing the
carbonyl group usually undergoes some interaction such as hydrogen bonding etc. at the
carbonyl group. Figure 4.1 shows the FTIR spectrum of the PLA film. The peak centered at
1761 cm-1 is attributed to the carbonyl group. (Younes et al., 1988) reported that two bands
that are related to the crystalline and the amorphous phases of PLA can be found at 755cm-1
and 869cm-1. The peak at 755cm-1 can be assigned to the crystalline phase while the peak at
869cm-1 can be assigned to the amorphous phase. PLA is a semi-crystalline polymer with
amorphous and crystalline phases. In the FTIR spectrum only one carbonyl peak at 1761 cm-1
was observed. A second derivative analysis was performed to see if there was overlap of the
carbonyl peak of the amorphous region with the carbonyl peak of the crystalline region. The
second derivative spectrum is shown in Figure 4.6. It can be seen that the carbonyl peak
separated into two peaks, one at 1767 cm-1 and the second at 1745 cm-1. The peak at 1767
cm-1 can be assigned to the carbonyl region of the amorphous phase in PLA and the peak at
1745 cm-1can be assigned to the carbonyl region of the crystalline phase.
DSC has been used extensively to characterize the thermal properties of PLA and its
blends. Generally, two heating cycles are carried out during DSC. The first heating cycle
represents thermal history and the effects of aging and the second heating cycle represents
the intrinsic properties of the polymer. In the first heating cycle, the previous thermal history
is erased and any volatile impurities or residual solvents are eliminated (Park et al., 2006).
One important parameter used to investigate whether two polymers are miscible in
the amorphous phase is the glass transition temperature, Tg. In DSC, the miscibility of two
135
polymers can be evaluated by the presence of a single, composition- dependent Tg value
between those of the two constituent polymers (Peesan et al., 2005). In miscible blends, the
Tg’s of the blend lies between the Tgs of the two polymers whereas the Tg of a polymer in
immiscible blends does not change with composition and is expected to maintain its bulk
value (Thirtha et al., 2005).
PLA is a semi-crystalline polymer and crystallizes from the melt and solution. The
equilibrium melting point and the glass transition temperature were found to be about 2150C
and 550C respectively by Kalb et al. 1980. Pure PLA has an equilibrium crystalline melting
point of 2070C but typical melting points in the 170-1800C range have been reported
(Vasanthakumari et al. 1983). This is due to small imperfect crystallites. It is not possible to
obtain a definitive temperature for Tg since it not only varies with the method of
measurement but is also affected by such factors as molecular weight, chain branching and
presence of impurities such as residual monomer (Stevens, 1975). In this present study, PLA
shows its Tg around 630C and a double melting peak appeared around 1620C and 1680C as
shown in Figure 4.27. These double peaks indicate that two populations of crystals with
different lamellar thicknesses exist. The lower temperature peak, 1620C, is due to the melting
of less thick lamellar crystals. These are considered less perfect crystals and have lower
melting point. The one at higher temperature, 1680C is that of thick crystals which are
considered higher- melting, more perfect crystals (Park et al., 2003). The same spherulitic
structure is shown very clearly in Polarized optical micrograph 4.3. Spherulites with varying
lamellar thickness are shown in Polarized optical micrograph 4.4. The fastest rates of
crystallization for pure PLA are found in the temperature range of 110-1300C (Kishore et al.,
1984). The present study showed that crystallization of PLA occurred at 1110C.
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It is well known that mechanical properties might be used to assess the miscibility
in polymer blends. Mechanical properties of polymer blends depend on intermolecular
forces, chain stiffness and molecular symmetry of the individual polymers used to prepare
the blend (Joseph et al., 2002). Furthermore, according to Willemse et al., 1999 tensile
modulus of polymer blends is strongly dependent on the composition and morphology of
blends.
Mechanical properties of the PLA film were studied. All the measurements were
repeated 3 times and the data presented in the respective plots were the average values of
each sample.
In the present study, pure PLA film showed relatively good tensile strength but poor
percentage elongation which is in agreement with the results reported by Martin et al., 2001
where PLA was found to be a brittle material with high tensile strength but low elongation.
The tensile results of pure PLA film are summarized in Figures 4.35-4.42.
5.1.2 Poly(lactic acid)/Poly(vinyl butyral) Blends
FTIR spectra of PLA/PVB blends are shown in Figures 4.7 and 4.8. Figure 4.2 shows
the characteristic carbonyl stretching peak of pure PVB at 1733 cm-1. The spectra of the
blends show that the characteristic carbonyl stretching absorption peak of PLA at 1761 cm-1
shifts to 1758 cm-1 with the addition of PVB in the blend and shifts further to 1756 cm-1 as
the PVB content is increased to 70 wt% and more. It is also seen that the carbonyl peaks
becomes narrow in the blends with 70 wt% and more PVB content. This indicates that the
carbonyl group may be involved in some interaction. The absorption peak of the crystalline
phase of PLA at 755cm-1 and the absorption peak of the amorphous phase of PLA at 869cm-1,
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both decreased slightly in intensity with the decreasing PLA content in the blends. However,
the decrease in the intensity of the crystalline peak is more pronounced than the decrease in
the intensity of the amorphous phase. The intensity of the crystalline peak decreased the most
in the blend film with PVB content of 70 wt%. The results suggest that the degree of
crystallinity of the PLA phase in the blend films decreases slightly with the addition of PVB
content. The amount of crystalline and amorphous PLA phases present in the blends was
obtained from the areas under the two peaks in the FTIR spectra and is given in Table 4.6.
The ratio of the two peaks varied with the change in PLA concentration in the blends. This
behavior is expected from an immiscible system. It indicates that the system is not
homogenous.
The blend-PVB difference spectra of these blends are given in Figure 4.9 and 4.10. They are
similar to the spectrum of pure PLA except that there is some shift in the carbonyl peak of
PLA and very slight decrease in the intensity of the crystalline and amorphous phase
absorption peaks of PLA as shown in the spectra of the blends. The second derivative of the
carbonyl peaks in the blends is given in Figure 4.11. The carbonyl peaks of the amorphous
and crystalline phases of PLA can be observed in the blends.
The PLA/PVB blends were thermally analyzed using DSC. Figure 4.29 shows the
characteristic Tg of PVB around 710C. The PLA/PVB blends showed two Tg’s as shown in
Table 4.11 indicating that this system is immiscible over the entire composition range. It is
evident from the scans that all the blends have crystallinity in them indicating that the blends
are in a heterogeneous state. A double melting peak appeared around 1620C and 1680C for
blends containing more than 50 wt% PLA. The thermograms are shown in Figure 4.29.
However, it clearly shows that with increasing PVB content in the blends the melting peak at
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1640C increases and the peak at 1680C gradually diminishes indicating that the presence of
PVB restricts the formation of thick crystals of PLA. Similar DSC results were obtained by
Zhang et al., 2003 in the PLA/PVP system. The amount of crystallinity in the blends was
calculated from the area under the endothermic peak in the DSC scans. In the PLA/PVB
blends, the area under melting endotherm peak decreased with the increasing PVB content in
the blends. Percentage crystallinity (Xc) calculations showed that crystallinity decreased
slightly with the addition of PVB to the blends as shown in Table 4.11. The lowest Xc was
found with 70 wt% PVB. The results obtained in the thermal analysis shows good correlation
with the results obtained with the FTIR analysis. It was observed that the crystallization
temperature (Tc) of the blends increased as the content of PVB increased. Blend with 90 wt%
and 70 wt% PVB showed a Tc of 1200C and 1230C respectively. The temperature reached its
highest at 1250C at 50 wt% PVB and then decreased to 1230C at 30 wt% and 1130C at 10
wt% PVB content in the blends.
For the hot-pressed PLA/PVB system, the thermal results are similar to the solution
cast blends. However, a significant decrease in the crystallization temperature from 1250C to
1000C was observed (Table 4.15).
The PVB50 blend films prepared at 550C had similar DSC results to the films
prepared at room temperature as shown in Table 4.16.
Optical microscopy of a miscible polymer system normally shows uniform phase
distribution of the component polymers in the system. In immiscible polymer systems, phase
separation between the polymers in the system is generally observed. Polarized optical
micrographs 4.6- 4.10 show the significant phase separation in the PLA/PVB blends, the dark
spots indicating the amorphous PVB among the PLA crystals. As indicated by the FTIR and
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thermal results, the crystalline phase in the blends decrease with decreasing PLA content in
the blends.
Figures 4.36 and 4.37 summarize the results for tensile strength and percent
elongation for all the PLA/PVB blend compositions respectively. When looking at the
characteristic of pure polymer, it can be seen that PVB has a better performance than PLA.
As a consequence, all blends show a decrease in tensile strength and percent elongation with
the increase in PLA contents. Maximum percent elongation was observed in pure PVB.
Blend with 90 wt% PVB showed similar strength as in pure PVB. Minimum tensile strength
was observed for blend with 50 wt% PVB content. Hydrogen bonds and adequate cross-
linking between the polymers is known to enhance the strength of blends (Yang et al., 2004).
However, in this experiment, no hydrogen bonds or cross-links were produced between PLA
and PVB chains as supported by FTIR and DSC results. PVB chains did not distribute
uniformly in the blend demonstrating poor mutual compatibility.
With all these observations it is clear that no specific interactions are present between
PLA and PVB and the present study confirms that this system is immiscible.
5.1.3 Poly(lactic acid)/Poly(vinyl formal) Blends
The PLA/PVF blends showed a similar behavior to that of the PLA/PVB blends. The
spectra of the blends are shown in Figures 4.12 and 4.13. Figure 4.3 shows the carbonyl peak
of PVF at 1734 cm-1. The absorption peak of carbonyl group in PLA shifts from 1761 cm-1 to
1757 cm-1 as the PVF content in the blends is increased to 50 wt%. The PLA carbonyl peak
shifts further to 1753 cm-1 as the PVF content is increased to 90 wt%. In contrast to the
observations made in the PLA/PVB blends, the intensity of the absorption peak of the
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crystalline phase of PLA at 755cm-1 and the absorption peak of the amorphous phase of PLA
at 869cm-1, both increased in intensity with the decreasing PLA content in the blends. The
increase in the intensity of the crystalline peak was much more obvious than the increase in
the amorphous peak. The most distinct increase in the crystalline peak was observed in the
blend film with 90 wt% PVF. The amount of crystalline and amorphous phases of PLA
present in the blends determined from the peak areas of the respective peaks is given in Table
4.7. The ratio fluctuated with varying PLA concentration in the blends. This is another
indication that the two polymers are not miscible.
The difference spectra of blend-PVF are given in Figures 4.14 and 4.15. The
difference spectra shows that the blends with more than 50 wt% PVF showed change in the
carbonyl region where the carbonyl peak shifted from 1761cm-1 to 1754cm-1. This could be
an indication that there could be some interaction between the two polymers in blend films
with more than 50 wt% PVF content. The second derivative spectra of the carbonyl region of
blends are given in Figure 4.16 and it can be observed that PLA in the blends shows peaks as
seen in pure PLA.
Blends of PLA/PVF are a semi-crystalline- amorphous system. PVF shows its Tg
around 1050C. The thermograms of the blends are shown in Figure 4.31 and the DSC results
are tabulated in Table 4.12. In this investigation, the Tg of PLA in the blends did not shift
from its characteristic Tg in pure PLA. The Tg of PVF in the blends could not be distinguished
because the crystallization temperature of PLA overlapped the Tg region of PVF. Zoppi et
al., 2001 has reported that a composition- dependent melting endotherm usually indicates a
miscible blend whereas a fully phase separated immiscible system displays a constant Tm.
Under complete immiscibility conditions, each of the polymer components of the blend will
141
exhibit the Tm of the corresponding pure homopolymer. No depression in the Tm in the
blends was observed. A double melting peak as seen in the PLA/PVB blend system was also
evident in this study. However, in this case, as the PVF content was increased, the melting
peak at 1640C gradually disappeared while the peak around 1680C became dominant. PVF
seemed to favor the formation of more perfect, high- melting PLA crystals. There was
insignificant variation in the crystallization temperature in the blends. The percentage
crystallinity in the system increased with increasing PVF content in the blends. Xc calculated
for this system agreed with the results got with FTIR analysis. Taking into consideration the
features of a miscible system, it was concluded that PLA/ PVF is not a miscible blend pair.
Phase separation in PLA/PVF blend system is shown in Polarized optical
micrographs 4.12- 4.16. PLA crystals in the photographs are segregated by the dark spots of
the amorphous phase of PVF. The amount of crystallinity in the blends is shown to increase
with increasing PVF content in the blends. This trend is supported by the FTIR and thermal
results as discussed earlier.
Results for tensile strength and percent elongation for PLA/PVF blend system are
shown in Figures 4.38 and 4.39. The results were similar to the PLA/PVB blends. Maximum
tensile strength and percent elongation was seen in pure PVF. With increasing PLA content,
the tensile strength and percent elongation decreased with the lowest tensile strength reported
in blend with 50 wt% PVF. The drop in tensile strength and percent elongation with the
increase in PLA content could be the result of the phase separation of the blend systems and
another indication that PLA/PVF blends are incompatible. Similar conclusions were made by
Suyatma et al., 2004 in one of their studies on PLA and chitosan blends.
Based on the above observations it is clear that the two polymers are not miscible.
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5.1.4 Poly(lactic acid)/Poly(styrene-co-acrylonitrile) Blends
Figures 4.17 and 4.18 show the spectra of PLA/SAN blends. The carbonyl stretching
peak of PLA shifts from 1761cm-1 to 1766cm-1 in the blend film with 30 wt% SAN content
and to 1758cm-1 with more than 50 wt% SAN in the blends. The intensity of the amorphous
and crystalline phase peaks increased with the decreasing PLA content in the blends. A
similar increase was observed in the PLA/PVF blends. The increase in the intensity of the
crystalline phase peak at 760cm-1 is more prominent than the increase in the amorphous
phase peak at 870cm-1. Table 4.8 shows the amount of crystalline and amorphous PLA
phases present in the PLA/SAN blends. The ratio of the two peaks did not stay constant but
changed with PLA content in the blends. This is another indication that no specific
interactions are present between the two polymers.
The blend-SAN difference spectra are given in Figures 4.19 and 4.20. The
difference spectra confirm the PLA carbonyl peak shift and the increase in intensity of the
crystalline peaks in the blends. The shift in the PLA carbonyl peak in the blends with 30 wt%
SAN indicates that there might be some interaction between the two polymers. Figure 4.21
gives the second derivative of the carbonyl region of the blends. The carbonyl peak of the
crystalline phase of PLA can not be seen in blends with less than 50 wt% PLA. However, it
is present in the blends with more than 50 wt% PLA content.
PLA/SAN blends were subjected to DSC analysis. The results obtained for this
system were similar to that of the PLA/PVF blend system. Tg of SAN was assigned at 1020C.
The thermograms of the blends are shown in Figure 4.33 and the DSC results are given in
Table 4.13. The Tg value of PLA in the PLA/SAN blends were slightly different from those
of pure PLA. The crystallization peak in the blends superimposed the glass transition region
143
of SAN, therefore, the Tg values of SAN could not be determined except for in blend with 90
wt% SAN content where no PLA crystallization occurred. Blend with 10 wt% SAN showed
two melting peaks indicating presence of uneven crystal formation. With 30 wt% and more
SAN content, only one melting peak at 1640C was observed indicating that SAN in the blend
encourages growth of imperfect, low- melting crystals. An increase in the crystallization
temperature was seen for 30 wt% and more SAN content in the blends, the highest
temperature noted at 1310C. This behavior coincided with the formation and presence of only
low-melting PLA crystals in the blend. No crystallization peak was evident in blend with 90
wt% SAN. This could be due to very small amount of PLA present in the blend. The amount
of crystallinity increased with the increasing SAN content in the blends with maximum Xc
shown in the blend with 70 wt% SAN content. These results agree with the results attained
with the FTIR analysis where the amorphous/crystalline peak ratio decreased gradually from
0.48 with 10 wt% SAN to 0.14 with 90 wt% SAN in the blends.
Polarized optical micrographs 4.18- 4.22 show the distribution of crystalline
phase in the PLA/SAN blend system. The degree of crystallinity is observed to increase with
the addition of more SAN content in the blends. The PLA spherulites are seen to become
distorted under the microscope in this blend system. Similar observation was reported by
Vasanthakumari et al., 1983 in the study of crystallization kinetics of PLA.
Mechanical properties of PLA/SAN blend system are given in Figures 4.40 and 4.41.
Pure SAN showed highest tensile strength and percent elongation. An increase in the PLA
content showed gradual reduction in the tensile strength of the composites. Percent
elongation did not show drastic reduction but more or less maintained similar elongation with
blend with 50 wt% SAN showing almost same percent elongation as in pure SAN. There was
144
no adhesion between the PLA and SAN phase which may account for the poor mechanical
properties in the blends.
Taking into consideration the findings of this present study, it is apparent that PLA
and SAN are immiscible.
5.1.5 Poly(lactic acid)/Ethyl cellulose Blends
The spectra of PLA/EC blends are given in Figures 4.22 and 4.23. It is obvious from
the spectra that the absorption peak of carbonyl group in PLA shifts from 1761 cm-1 to
1757cm-1 only in blends with more than 50 wt% EC content. The PLA carbonyl peak does
not show any shift in blends with less than 50 wt% EC content. The absorption peak of the
crystalline phase of PLA at 755cm-1 increased significantly in intensity with increasing PLA
content in the blends. The amorphous phase peak of PLA showed little or no change in
intensity with increasing PLA content in the blends. The amount of two phases present in the
blends, determined from the areas of amorphous and crystalline peaks is given in Table 4.9.
It is seen that the ratios vary with varying PLA content in the blends. This indicates the
immiscibility of the two polymers.
Figures 4.24 and 4.25 show the difference spectra of blend-EC. Blends with 70 wt%
and 90 wt% PLA showed some change in the carbonyl. The second derivative spectra of the
carbonyl peak of the blends are given in Figure 4.26. Blends with less than 30 wt% PLA
content do not show any peak at 1745cm-1 which is due to the carbonyl peak of the
crystalline region of PLA. The peak is present in blends with 50 wt% and more PLA content.
The results indicate that very little interaction is seen between EC and PLA polymers.
The behavior of PLA/EC blend system is similar to the other systems investigated in
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this research. EC was found to exhibit its Tg around 1290C. The PLA Tg in the blends did not
display any shift from its typical value. The DSC results are given in Table 4.14 and the
thermograms of the blends are shown in Figure 4.35. The Tg for EC could not be noted
because it fell in the crystallization area of PLA. Double melting peaks were also evident in
this system as in the others. It was observed, however, that the increasing EC content up to
90 wt% did not have much effect on the size or type of crystals formed. The crystallization
temperature in the blend increased with EC addition but decreased at 70 wt% EC content in
the blend. The percentage crystallinity calculated for the system showed little change and
remained more or less constant in blends with 70 wt% and less EC in the blends. Blend with
90 wt% EC content showed very less crystallization which could be presence of insignificant
amount of PLA present in the blend. This behavior is supported by FTIR analysis.
Polarized optical micrographs 4.24- 4.28 show separate PLA and EC phases in the
PLA/EC blend system. The PLA spherulites can be seen very clearly in this blend system in
contrast to the distorted PLA spherulites observed in the PLA/SAN blend system.
Pure EC film was very weak and tore easily. Tensile strength and percent elongation
for pure EC film and blends with more than 70 wt% EC content could not be determined due
to high brittleness of the films. In this case pure PLA showed better mechanical properties
than EC. The mechanical properties of PLA/EC blends are shown in Figures 4.42 and 4.43.
With all these observations it is evident that PLA/EC is an immiscible system as there
are no specific interactions between them.
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Section B
5.2 Degradation Studies of PLA and its Blends
This section describes the degradation of PLA and its blends under different
environmental conditions: controlled as well as natural and in different soil types. In addition
biodegradability of PLA and its blends was determined by specific microorganisms isolated
from two different types of soil.
PLA degrades to its monomer, lactic acid. The degradation of PLA proceeds
essentially via hydrolysis of ester group which takes place heterogeneously (Andreopoulos et
al., 2000). Although its degradation rate in compost is rapid, the non-enzymatic degradation
rate in water, soil or in human body is not sufficiently fast enough for applications where
degradation times of few months is desired (Shinoda et al., 2003). PLA has been reported to
have a degradation time in the environment on the order of six months to two years (Garlotta,
2001). Degradability is significantly altered when one utilizes blends instead of
homopolymers.
Blending decreases the hydrophobicity or crystallinity in the polymer, thereby
enhancing the degradation rate. Additionally, degradability is affected by the macro-
molecular architecture; branched structures display faster degradation rates than the
corresponding linear ones due to lower crystallinity (Shinoda et al., 2003). Crystallinity in
the film prevented enzymatic degradation since the enzyme is known to preferentially attack
the amorphous regions of PLA (Gajria et al., 1996). The rate of enzymatic degradation of
PLA decreased with the increase in crystallinity. PLA with low percentage crystallinity
showed no weight loss during the period it was subjected to degradation (Cai et al., 1996).
Suyama et al., 1999 reported that environment bacteria capable of degrading available
147
biodegradable plastics were diverse, however, 15 strains of Amycolatopsis bacteria were
found to be PLA degraders by Pranamuda et al., 1999.
5.2.1 Biodegradation
Mycobacterium and Bacillus are common degrading bacteria found in soil. These
bacteria were isolated from garden soil and rubbish dump soil and they showed similar
biodegradation behavior for PLA and its blends. The study was conducted over a period of
14 days. Controls were maintained for all the samples tested. They showed no weight loss.
PLA, however, showed up to 32.4% weight loss in the cultured mineral broth.
Pure PVB showed no loss at all. The PLA/PVB blends showed between 6- 22%
weight loss with both the bacteria.
The blends of PLA with PVF showed weight loss between 7- 18% with pure PVF
showing almost insignificant loss.
It was observed that pure SAN was not affected by the bacteria at all. However, the
PLA/SAN blends showed biodegradation of about 2- 4% weight loss.
Pure EC showed up to 1% weight loss while its blends with PLA exhibited 2- 22%
weight loss. It is known that PVB, PVF and SAN are not biodegradable but the cellulose
component of EC is known to be biodegradable.
It has been reported by Renstad et al., 1998 that a longer time is required until biotic
degradation becomes noticeable because microorganisms find it difficult to degrade longer
chains. SiO2 and CaCO3 are two inorganic additives used to roughen the surfaces of films
that provide a prerequisite for biodegradation. This concept could also be used to explain
why the blends show higher biodegradability than pure PLA film. Pure PLA film has a
148
smooth surface while the blend films exhibit a rough surface due to phase separation. This
provides better adhesion of microorganisms to the film to start the biodegradation process.
5.2.2 Degradation in the Natural Environment
Many researchers have already reported that degree of crystallinity is closely related
to degradation (Lam et al., 1994). During the present study, pure PLA showed almost no
weight loss in garden soil in the first month, increasing to almost 9% in the second month,
25% in the third month and dramatically increasing to almost 62% after 5 months. The
weight losses are shown in Figure 4.44. While in the rubbish dump soil, the weight loss
increased gradually for the 5 months, degrading as much as 93% and the results are shown in
Figure 4.49. It has been observed by Renstad et al., 1998 that degradation occurs from the
surface through bioerosion and the onset of degradation occurs after significant period of
chemical hydrolysis. The degradation occurs rapidly initially after which the rate decreases
by crystallization. Chain scission in the soil cause crystallization during degradation. This
phenomenon could explain the increasing brittleness and opaqueness of the films as
degradation progressed. It can be postulated that the faster degradation in rubbish dump soil
could be due to the synergistic effect of the degrading bacteria already present in the soil.
The PLA/PVB blends show higher degradation for the first 2 months than pure PLA
in the two different types of soil. This behavior could be due to surface roughness in the
blend films. Rough surface would have a greater surface area increasing the accessibility to
extracellular enzymes. A trend was observed in the degradation of the blends. Blends with
less PLA content showed less weight loss compared to those with higher PLA contents. As
shown in Figure 4.45, blends with 30 wt% PLA content showed a weight loss of around
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20%, blends with 50 wt% PLA content showed a weight loss of around 40% and blends with
70 wt% PLA content showed a weight loss of around 50% after 5 months in the garden soil.
In the rubbish dump soil, a similar degradation trend to the one observed in garden soil was
observed. Weight loss increased with increasing PLA content in the blends. Blends with 30
wt% PLA content showed a weight loss of 20%, blends with 50 wt% PLA content showed a
weight loss of around 40% and blends with 70 wt% PLA content showed a weight loss of
almost 70%. Figure 4.50 shows the percentage weight loss for the PLA/PVB blends.
Results obtained for the PLA/PVF blends are similar to that of the PLA/PVB blends.
In the garden soil, blends with 30 wt% PLA content showed a weight loss of around 15%,
blends with 50 wt% PLA content showed a weight loss of 25% and blends with 70 wt% PLA
content showed a weight loss of around 50% after 5 months. The percentage weight loss of
the blends has been plotted in Figure 4.46. In rubbish dump soil, the degradation rate of the
blends was seen to increase slightly with 30 wt% PLA composition blends showing a weight
loss of around 20%, blends with 50 wt% PLA showing a weight loss of around 30% and
blends with 70 wt% PLA content showing a weight loss of around 60% after 5 months as
shown in Figure 4.51. Degradation of the blends increased with increasing PLA content in
them.
As shown in Figure 4.47, the blends of PLA/SAN with 30 wt% PLA content showed
a weight loss of around 10%, blends with 50 wt% PLA showed a weight loss of around 25%
and blends with 70 wt% PLA showed a weight loss of around 42% in garden soil after 5
months. As observed in the PLA/PVF system, degradation in rubbish dump soil increased
slightly. The results are shown in Figure 4.52. The blends with less than 50 wt% PLA content
150
showed a weight loss of around 30% and blends with 70 wt% PLA content showed a weight
loss of almost 50%.
In the PLA/EC system, the films which were semi-transparent with a smooth surface
initially had become extremely perforated and became powdery when rubbed between
fingers. The blends had achieved almost 100% degradability in the garden and rubbish dump
soil by the end of 5 months. Figures 4.48 and 4.53 show the degradation results for the blends
in garden and rubbish dump soil respectively.
5.2.3 Degradation in Controlled Environment
Degradation of PLA and its blends with other polymers exhibited similar behavior as
in the natural environment. However, it was observed that the weight loss in each sample
when compared to the same samples in the natural environment was lower. The decreased
degradation in the controlled environment cannot be explained conclusively. Degradation in
the natural environment could be due to the synergistic effect of many factors such as
temperature, water content, organic and inorganic compounds, microorganisms present. The
accumulative effect of these factors could account for the higher rate of degradation in the
natural environment.
Pure PLA film degraded as much as 50% in garden and rubbish dump soil where the
temperature was kept at a constant 350C and water content at 50% of its saturated value. The
percentage weight loss of PLA film in garden and rubbish dump soil is shown in Figures 4.54
and 4.59.
The PLA blends exhibited similar behavior as observed in degradation in the natural
environment. The degradation of the blends decreased with decreasing PLA content. As
151
shown in Figure 4.63, PLA/PVB blends with 30 wt% PLA, 50 wt% PLA and 70 wt% PLA
content showed weight losses of around 10%, 20% and 30% respectively in the garden soil.
The weight loss in the rubbish dump soil was the same as shown in Figure 4.68.
PLA/PVF, PLA/SAN and PLA/EC systems showed the same degradation rate as
noted in the PLA/PVB system. The degradation results for these blends are shown in Figures
4.56 - 4.63.
The findings of the degradation study in this section conclusively show that the
degradation of the PLA blends depended on the PLA content in the blends. The degradation
rate increased with increasing PLA content.
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CHAPTER SIX
CONCLUSION
During the present investigation, the miscibility and biodegradation behavior of PLA
with polymers such as PVB, PVF, SAN and EC was studied.
The binary blends were prepared by casting films from mixed polymer solutions
made in chloroform. The miscibility of these blends was studied using DSC, FTIR
spectroscopy, tensile testing supported by polarized microscopy of the films. DSC
measurements revealed that in all the PLA/PVB, PLA/PVF, PLA/SAN and PLA/EC blends,
Tg of PLA and the other polymers in the binary system did not change over the entire
composition range investigated. No depression in the Tm of PLA in the blends was observed.
Percent crystallinity of PLA in the blends remained constant throughout the entire system
indicating that no interaction between PLA and the respective polymers in the blend
occurred. The crystallization process of PLA was not significantly affected by the addition of
the second polymers in the blends. These observations concluded that PLA blends with PVB,
PVF, SAN and EC are immiscible.
The FTIR measurements indicated that no intermolecular interactions between PLA
and the other polymers existed. The FTIR spectra of the blends exhibited almost all the
features of PLA and the corresponding polymer in the respective systems as they individually
showed. It was observed that there was practically no shift in the characteristic absorption
bands of any of the polymers after blending showing incompatibility. These results are in
agreement with the DSC results. However, PLA/PVB blends with less than 30 wt% PLA and
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PLA/PVF blends with less than 50 wt% PLA showed possibility of some interaction
occurring.
Optical microscopy showed phase separation in all the blends systems. The PLA
crystallites could be seen clearly with dark spots of the amorphous phases from PVB, PVF,
SAN and EC in the respective blends.
In the present study it was observed that an increase in the PLA content showed
gradual reduction in the tensile strength and percent elongation of the composites. The drop
in tensile strength and percent elongation with the increase in PLA content could be the result
of the phase separation of the blend systems. There was no adhesion between the PLA and
the other polymer phases in the blend which accounted for the poor mechanical properties in
the blends. These results are yet another indication of poor mutual compatibility.
The blends showed lower degradation rate than pure PLA film in this study. PVB,
PVF and SAN are non-degradable in nature. Degradation in the natural environment showed
higher weight loss compared to degradation in the controlled environment. No definite
conclusion could be reached to explain this degradation phenomenon. It was, however,
postulated that the degradation in the natural environment could have been due to the
synergistic effect of the biotic and abiotic factors, the effects of which were reduced or even
eliminated in the controlled environment.
The present research investigation has concluded that immiscibility results in poor
adhesion between the two components in the blend system, resulting in poor and
irreproducible performance. Two approaches are usually used to improve blend
compatibilization. The first approach is to introduce a third component into the polymer
system, reducing interfacial energy, improving dispersion and consequently enhancing
154
adhesion between binary polymer phases. A block copolymer is often used for this purpose.
The second method is reactive blending where chemical reactions are promoted between the
two polymers in a molten state by introducing a reactive third component with appropriate
functional groups or a catalyst. Degradation of polyesters can be controlled practically by
using additives. Plasticizers such as citrate esters accelerate the degradation rates of
polyesters while water insoluble additives such as zinc carbonate or calcium carbonate retard
degradation (Renstad et al., 1998)
Further work needs to be carried out with the PLA binary systems investigated in this
study. The two methods mentioned above could be employed to improve miscibility in the
PLA blends studied. While adding plasticizers to the PLA systems could control the
degradation rate as desired.
155
CHAPTER SEVEN
REFERENCE
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Andrady, A.L., (2003). Plastics and the Environment. John Wiley & Sons Publication,
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