ta384 thermal analysis investigation of a polylactic acid biodegradable plastic
TRANSCRIPT
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ThermalAnalysisInvestigationofaPoly(LacticAcid)BiodegradablePlastic
ABSTRACT
With thepush in recentyears for industrytodevelopandmanufactureproductsona
more environmentally friendly basis, a variety of new biodegradable polymer systems have
beendevelopedtofitthatmold. Poly(lacticacid)(PLA) isabiodegradablealiphaticpolyester
which is produced from lactides and lactic acid monomers that are derived from the
fermentationofcornstarchandsugar feedstocks.Thepolymerizationof lacticacid intoPLA
producesabiodegradablethermoplasticpolyesterthathashighmechanicalstrength,similarto
PETE, with good biocompatibility. PLA has most commonly been used in biomedical
applications for drug delivery systems as well as sutures and stents, but the number of
applications
for
PLA
is
constantly
growing.
Understanding
the
properties
of
PLA
becomes
essentialtothefuturedevelopmentofnewapplications. Thisstudywillexamineavarietyof
thethermalandmechanicalpropertiesofaPLAdrinkingcupusingthermalanalysistechniques
suchasDSC,MDSC,RapidHeat/CoolDSC(RHC)andDMA.
INTRODUCTION
AgenericdrinkingcupmadeofPLAwasusedasthesolememberofthis investigation
andwasselectedsimplybecauseofthephysicalappearanceofthecup. Thetophalfofthecup
hadanopticallyclear,uniformappearancewhilethebottomhalfofthecuphadamuchmore
irregularlookthatgavetheappearanceofmaterialroughnesswithoutanyphysicaltexture. It
wasassumed that the tophalfof thecupwasmoreamorphouswhile thebottomhalfmore
crystalline. Inordertodeterminetheamorphousandcrystallinecomponentsinthetopofthe
cupversusthebottomofthecup,theinvestigationstartedwithstandardDSCmeasurements,
which is probably the simplest technique. More advanced DSC methods as well as DMA
measurements were incorporated into the investigation to refine and verify the results
obtainedonthePLAcup.
RESULTS&DISCUSSION
AstandardDSCheatcoolheatmethodwasinitiallyrunonasampletakenfromthetop
halfofthecup,whichwasassumedtobemoreamorphous. ThedataisshownbelowinFigure
1. Thecupsamplewasheatedat20deg/minandcooledatacontrolled rateof10deg/min
between25
and
170C.
All
of
the
DSC
and
MDSC
samples
were
tested
on
aQ2000
DSC
in
TZero
Aluminumpanswith a nitrogen purge. The first heat, in this instance, shows a small glass
transition (Tg)around58Cwith some coldcrystallizationbeginningaround90Candamelt
withapeaktemperatureofabout148C. Thesecondheatonthissampleafteritwascooledat
10deg/minshowsalargerTgaroundthesametemperatureasthefirstheat,butnoevidence
ofcoldcrystallizationormelting. Theresultssuggestthatthetopportionofthecuphadsome
amountofamorphousstructure,butbecausethesampleundergoessomecoldcrystallization
or crystalperfection immediatelybefore themelt, theamountofcrystalline structure in the
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-0.3
-0.2
-0.1
0.0
0.1
0.2
HeatFlow(W/g)
Figure2:MDSCresultsonasampletakenfromthetopofthePLAcup
AsampletakenfromthebottomofthePLAcupwastestedusingthesameModulated
conditionsasthesample fromthetopofthecup. Theresultsareshown inFigure3. While
therearesomesimilaritiesbetweentheMDSCresultsofsamplestakenfromthetopandthe
bottomof
the
cup,
there
is
one
major
difference
that
directly
points
to
amajor
difference
in
materialstructure. TheTgisapproximatelyatthesametemperatureasbeforeandthereisstill
some enthalpic recovery, crystal perfection and melting that show up in both the Non
Reversing and Reversing Heat Flows out beyond 120C. The major difference seen in the
bottom of the cup is a large cold crystallization peak that begins around 80C. This peak
suggeststhatsomeoftheamorphousstructureinthematerialisorderingandconvertingtoa
morestructured,crystallinestructurewhichwasaneventthatdidnotshowup inthesample
fromthetopofthecup. TheotherinterestingcharacteristicdeterminedfromtheMDSCresults
isthefactthattheareaoftheNonReversingHeatFlow,includingthecoldcrystallization,and
theReversingHeatFlowarenearlythesamevalue. Thisresultsuggeststhatthesampledidnot
haveanycrystallinitytobeginwithandallofthecrystallinematerialthatmeltedwasformed
duringthe
cold
crystallization,
which
is
counter
to
the
initial
assumption
based
off
of
the
optical
appearancethatthesamplewasmorecrystalline.
142.89C
136.98C24.22J/g
142.24C
136.38C61.25J/g
61.25 - 24.22 = 37.03 J/g
Heat Only MDSC80 sec periods3 deg/min ramp
-0.3
-0.2
-0.1
0.0
0.1
0.2
RevHeatFlow(W/g)
-0.2
-0.1
0.0
0.1
NonrevHeatFlow(W
/g)
20 40 60 80 100 120 140 160 180 200
Temperature (C)Exo Up Universal V4.7A TA Instruments
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TA384 4
-0.3
-0.2
-0.1
0.0
0.1
0.2
0.3
RevHeatFlow(W/g)
Figure3:MDSCresultsonasampletakenfromthebottomofthePLAcup
Inorder toverifythatallofthecrystallinitywas formedduring theheatingrampand
wasnot inthesample initially,aRapidHeatCoolDSC(RHC)experimentwasusedtoheatthe
sample at 1000 deg/min in an attempt to suppress the cold crystallization. For the RHC
experiment,aBeta
RHC
DSC
was
used
and
approximately
0.3mg
of
sample
was
tested
in
aluminumpanscustomdesigned fortheRHC. Thetesttemperature rangewaswidenedto
150Conthelowendand225Conthehighendinordertoaccommodatethehigherheating
rateof1000deg/min. TheHeatFlowresultsfortheRHCexperimentareshowninFigure4and
showonlyaTgaround76Candnothingelse. TheshiftupintemperatureoftheTginthiscase
issimplyaresultoftheincreasedheatingratewhencomparedtoMDSCandDSC,whichboth
have heating rates over an order of magnitude slower. There is no evidence of cold
crystallization upon heating and the fact that there isno evidenceofmelting suggests that
there is no crystallinematerial in the sample tomelt. For comparisonpurposes, the same
sample taken from thebottomof the cupwas allowed to crystallizeby slowingheating the
material toa temperaturearound125Cand then testedagain in theRHCat1000deg/min.
Theresults
for
the
material
that
was
allowed
to
crystallize,
shown
in
Figure
5,
prove
that
a
samplewithcrystallinematerialthatmeltswillshowthatmeltingendothermevenifheatedat
1000 deg/minwith very little shift in the onset ofmelting. If the sample initially had any
crystallinestructure,themeltshouldhaveshownupinthefirstRHCexperiment.
98.67C
91.09C48.56J/g
145.54C
139.28C51.20J/g
Heat Only MDSC80 sec periods3 deg/min ramp
51.20 - 48.56 = 2.64 J/g
-0.3
-0.2
-0.1
0.0
0.1
HeatFlow(W/g)
-0.3
-0.2
-0.1
0.0
0.1
NonrevHeatFlow(W
/g)
20 40 60 80 100 120 140 160 180 200
Temperature (C)Exo Up Universal V4.7A TA Instruments
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TA384 5
75.97C(H)
0.296mg of sample1000 deg/min
0
500
1000
1500
Deriv.
Temperature(C/min)
-45
-25
-5
15
HeatFlow(W/g)
-150 -100 -50 0 50 100 150 200 250Temperature (C)Exo Up Universal V4.7A TA Instruments
Figure4: Thebottomofthecup,asreceived,testedintheRHCat1000deg/min
75.46C(H)
0.296mg of sample
1000 deg/min
0
500
1000
1500
Deriv.
Temperature(C/m
in)
-45
-25
-5
HeatFlow(W/g)
-100 -50 0 50 100 150 200 250
Temperature (C)Exo Up Universal V4.7A TA Instruments
Figure5: ThebottomofthecuptestedintheRHCat1000deg/minafteritwasallowedtocrystallize
To verify the conclusionsmade about the topof the PLA cup that therewas indeed
some crystalline structure in thematerial initially, the same RHC experimentwas run on a
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TA384 6
sample taken from the top of the cup. The results shown in Figure 6 actually show two
endothermic peaks around 75 and 125C. Based on some of the previous experiments,
however,thefirstendothermaround75Cismostlikelytheresultofsomeenthalpicrecovery
thatovershadowstheTgsincetheotherRHCexperimentsat1000deg/minshowtheTgright
around75Caswell. The secondendotherm isassociatedwith initialcrystallinity thatmelts
around 125Cwhich compareswellwith theMDSC experiments of the samematerial that
beginstomeltaround120Cminusthecrystalperfection.
0.145mg of sample1000 deg/min
0
500
1000
1500
Deriv.
Temperature(C/min)
-65
-45
-25
-5
HeatFlow(W/g)
-100 -50 0 50 100 150 200 250Temperature (C)Exo Up Universal V4.7A TA Instruments
Figure6: Thetopofthecup,asreceived,testedintheRHCat1000deg/min
Anothertechniqueavailabletoexaminethecrystallinityorthechangeincrystallinityas
afunctionoftemperature istheDMA. Figures7and8areexperimentsrunonthesamePLA
cupsamplesusingtheRSADMA. Theresultscollectedonasamplefromthetopofthecupin
Figure7showthattheStorageModulusofthesampledropsaround60Cwherethematerial
goesthrough
the
Tg
and
then
plateaus
before
dropping
again
around
130C
where
the
material
melts. Bothof theseeventscorrelatequitewillwith the resultscollectedbyDSC. Figure8,
whicharetheresultscollectedfromasamplefromthebottomhalfofthecupshowadropin
StorageModulus around 60C for the Tg and then a significant increase inModulus around
100C,which isusually indicativeofan increase instiffness/mobilityandcorrelatesverywell
withthecoldcrystallizationshownintheMDSCresultsaroundthesametemperature. Figure9
showsanoverlaycomparisonoftheStorageModulusbetweenthetwosamples.
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20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0
106
107
108
109
1010
0.0
0.2
0.4
0.6
0.8
1.0
Tem [C]
E'(
)
[Pa]
E"(
)
[Pa]
tan_delta(
)
[]
Figure7: DMAdatafromthetopportionofthecup
20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0
105
106
107
108
109
1010
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
Tem C
E'(
)
[Pa]
E"(
)
[Pa]
tan_delta(
)
[]
Figure8: DMAdatafromthebottomportionofthecup
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TA384 8
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0
106
107
108
109
1010
Tem C
E'(
)
[Pa]
E'
Top
Bottom
Figure9: OverlayoftheEDMAdatafromboththetopandbottomsectionsofthecup
CONCLUSIONS
A plastic drinking cup made from the biodegradable plastic, poly(lactic acid) was
examinedusingDSC,MDSC,RapidHeat/CoolDSCandDMA. Theaimoftheinvestigationwas
tocomparetwoareasthatappearedopticallyandstructurallydifferent,withthesupposition
thatadifferenceincrystallinitymayberesponsible. Resultswereconsistentacrosstechniques
showingadifferenceinitialcrystallinitybetweenthetwosections.
REFERENCES
1.E1269,DeterminingSpecificHeatCapacitybyDifferentialScanningCalorimetry,ASTM
International,West
Conshohocken,
PA.
2.L.ThomasandS.Aubuchon,HeatCapacityMeasurementsUsingQuasiIsothermal
ModulatedDSC,TAInstrumentsApplication(TA230).
3.L.Thomas,ModulatedDSCPaper#9,MeasurementofAccurateHeatCapacityValues,TA
InstrumentsApplication(TP014).
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