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Carbon Particulate Assisted Extrusion Foaming of Polyethylene Terephthalate (PET) by
Controlled-Hydrolysis for Thermal Insulation Applications
Thesis
Presented in Partial Fulfillment of the Requirements for the Degree Master of Science in
the Graduate School of The Ohio State University
By
Junjie Pan
Graduate Program in Chemical Engineering
The Ohio State University
2018
Thesis Committee
Dr. L. James Lee, Advisor
Dr. Jose Castro
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Copyrighted by
Junjie Pan
2018
i
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Abstract
IR-absorbing foams as roofing and external wall materials have gained
considerable interest for their enhanced insulation and sustainability. However, the most
widely used polystyrene (PS) foam in the insulation industry is not feasible for IR-
absorbing application due to its low thermal stability. As a semi-crystalline polymer,
polyethylene terephthalate (PET) is a desirable substitute which has excellent thermal
stability and mechanical strength. Also, PET’s recyclability is very important due to the
severe plastic pollution. However, obtaining low-density semi-crystalline PET foam is a
great challenge. Chemical modification of the PET resins such as chain extension and
branching is the most widely used way to enhance its foamability. However, it inevitably
reduces the crystallinity and thus leads to relatively poor mechanical and thermal properties.
Herein, we developed a simple and affordable controlled-hydrolysis approach to prepare
low-density PET foam with high crystallinity. The effect of the water content and type of
hydrolysis agents on the foam expansion ratio, cell morphology, extent of degradation and
crystallinity were investigated. Since controlled-hydrolysis kept the linear chain structure
and decreased the molecular weight to an acceptable level, our PET foam has high
crystallinity and thus excellent tensile strength and high thermal stability (>200℃). Based
on the optimized hydrolysis conditions, both activated carbon (AC) and micrographite
(mGr) were selected as the infrared attenuation agent for IR absorbing. We also
investigated the influence of AC and mGr as a nucleation agent on foam density and cell
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morphology. By simulating the housing and vehicle roofing conditions, we successfully
demonstrated the superiority of the carbon particulate containing PET foam over the PS
foam for future IR-absorption roofing application.
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Acknowledgments
First, I would like to express my sincerest gratitude to my advisor Dr. L. James Lee
for his guidance and support on my thesis. Without his patient and detailed instruction, I
couldn’t became well trained in polymer processing research within only one year.
Furthermore, I benefit a lot from his constructional suggestion and encouragement on my
future career plan.
I would like to express my special appreciation to my co-advisor Dr. Jose Castro.
He helped developed the methodology of this thesis and his knowledge on rheology always
impressed me. Also, this thesis couldn’t have progressed smoothly without his help on
sample testing in his lab.
I also would like to thank Dr. Feng Chen and Dr. Xiangmin Han. Their previous
research provided a basis for my work. Also, thank you Dr. Eusebio Duarte Cabrera, Mr.
Dan Zhang and Mr. Min Wu for instructing me on the use of various devices and help
testing some of the samples. And it’s really helpful when discussing with you about
technical details in this thesis.
Finally, thanks to Mr. Leigh Evrard, Mr. Michael Wilson and Joshua Hassenzahl
from both CBE and ISE machine shops. Without their help, I could not have finished this
thesis smoothly.
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Vita
September 1991 ...........................................Shanghai, China
2010..............................................................Shanghai Qibao High School
2014..............................................................B.E., East China University of Science and
Technology
2016..............................................................ThermoFisher Scientific (China)
2018..............................................................Graduate Student, The Ohio State University
Fields of Study
Major Field: Chemical Engineering
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Table of Contents
Abstract ........................................................................................................................... ii
Acknowledgments.............................................................................................................. iv
Vita ........................................................................................................................... v
Table of Contents ............................................................................................................... vi
List of Tables ..................................................................................................................... ix
List of Figures ..................................................................................................................... x
Chapter 1. Background and Literature Review .................................................................. 1
1.1 Introduction .............................................................................................................. 1
1.2 Extrusion Foaming ................................................................................................... 3
1.3 Polyethylene Terephthalate ...................................................................................... 6
1.4 Challenges of PET foaming ..................................................................................... 7
1.5 Conventional Approaches ........................................................................................ 8
1.5.1 Copolyester ....................................................................................................... 9
1.5.2 Resin Chain Extension ...................................................................................... 9
1.6 Non-chemical Modification Approach ................................................................... 11
1.6.1 Optimization of Foaming conditions .............................................................. 11
1.6.2 Controlled-Hydrolysis..................................................................................... 12
1.6.3 Selection of Hydrolysis Agent ........................................................................ 13
1.6.4 Mircographite as IAA and Nucleation Agent ................................................. 14
1.7 Objectives ............................................................................................................... 15
Chapter 2. Materials and Experiments ............................................................................. 16
2.1 Materials and Processing Equipment ..................................................................... 16
2.2 Foam Extrusion of Crystalline PET (CPET) Resins by Controlled-Hydrolysis .... 17
2.2.1 CPET Foaming with Moisture ........................................................................ 17
2.2.2 CPET Foaming with Wet Activated Carbon .................................................. 17
2.2.3 Extrusion Foaming and Condition Optimization ............................................ 18
2.3 Sample Characterization ......................................................................................... 20
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2.3.1 Foam Density .................................................................................................. 20
2.3.2 Water Content ................................................................................................. 20
2.3.3 Cell Morphology ............................................................................................. 21
2.3.4 Molecular Weight ........................................................................................... 22
2.3.5 Shear Viscosity ............................................................................................... 23
2.3.6 Crystallinity..................................................................................................... 23
2.4 Functional Properties Measurement ....................................................................... 24
2.4.1 Tensile Test ..................................................................................................... 24
2.4.2 Thermal Stability ............................................................................................ 24
2.4.3 Insulation Measurements ................................................................................ 25
2.5 Strand Die Design and Experiments ...................................................................... 26
Chapter 3. Results and Discussion ................................................................................... 29
3.1 Optimization of Processing Conditions .................................................................. 29
3.2 Neat PET Foams ..................................................................................................... 30
3.3 Foaming CPET by Controlled-hydrolysis .............................................................. 32
3.3.1 Foaming with Moisture ................................................................................... 33
3.3.2 Foaming with Activated Carbon (AC) ............................................................ 34
3.3.3 Comparison between Moisture and Wet AC .................................................. 37
3.3.4 Chain Extension vs. Controlled-hydrolysis .................................................... 43
3.4 Adding micrographite (mGr) as IAA and nucleation agent ................................... 44
3.5 Mechanical and Thermal Properties of CPET Foams ............................................ 47
3.5.1 Tensile Properties............................................................................................ 47
3.5.2 Thermal Stability ............................................................................................ 48
3.5.3 IR-absorbing and Insulation Properties .......................................................... 49
3.6 Strand Die Experiment ........................................................................................... 52
Chapter 4. Conclusion and Future Work .......................................................................... 53
Bibliography ..................................................................................................................... 54
Appendix A. Experimental Design ................................................................................ 63
Appendix B. Optimization of Foaming Conditions ....................................................... 65
Appendix C. Water Content Measurement .................................................................... 68
Appendix D. Shear Viscosity of CPET and XPET Resins ............................................ 70
Appendix E. Cell Morphology of Dry CPET/Carbon Particles Foam (less than 0.05
wt. % water) .................................................................................................................. 71
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Appendix F. Crystallinity Calculation from DSC Thermograms .................................. 72
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List of Tables
Table 1.1 Foam applications 1 ............................................................................................. 1
Table 2.1 Material description and pre-treatments ........................................................... 16
Table 2.2 Theoretical design of the strand die .................................................................. 27
Table 3.1 Density, cell morphology and crystallinity of neat PET foams ........................ 30
Table 3.2 Crystallization behavior of PET foams ............................................................. 43
Table A.1 Neat PET foams ............................................................................................... 63
Table A.2 Foaming CPET resins with moisture ............................................................... 63
Table A.3 CPET/AC with water foams ............................................................................ 64
Table A.4 Using mGr as IAA and to further manipulate the foams morphology ............ 64
Table B.1 Optimized processing condition of neat CPET foaming.................................. 65
Table B.2 Optimized processing condition of XPET foaming ......................................... 66
Table B.3 Optimized processing condition of foaming CPET with moisture .................. 66
Table B.4 Optimized processing condition of foaming CPET using AC as water carrier 67
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List of Figures
Figure 1.1 Foaming mechanism 14 ..................................................................................... 4
Figure 1.2 Polyethylene Terephthalate (PET) .................................................................... 6
Figure 1.3 Chain extension and branching of PET by PMDA 22 .................................... 10
Figure 2.1 Leistritz twin screw extruder ........................................................................... 17
Figure 2.2 Preparation of wet AC ..................................................................................... 18
Figure 2.3 Foam extrusion diagram .................................................................................. 19
Figure 2.4 Capillary die and its geometry ......................................................................... 20
Figure 2.5 Viscometer ....................................................................................................... 22
Figure 2.6 Thermal stability test within the temperature ranging from 25℃ to 220℃ .... 24
Figure 2.7 Diagram of Mimicking the IR-absorbing roof application .............................. 25
Figure 2.8 Experiment setting of the IR-absorbing roof application ................................ 26
Figure 2.9 Schematic of the strand die.............................................................................. 26
Figure 2.10 Optimized strand die geometry ..................................................................... 28
Figure 3.1 SEM picture of neat CPET foam and the cell size distribution ....................... 31
Figure 3.2 SEM picture of crosslink PET foam and the cell size distribution .................. 31
Figure 3.3 SEM picture of commercial PET foam and the cell size distribution ............. 31
Figure 3.4 CPET foams with moisture or wet AC as hydrolysis agent ............................ 32
Figure 3.5 Effect of water content on foam density .......................................................... 32
Figure 3.6 SEM picture of neat CPET foam with 0.09 wt. % moisture ........................... 33
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Figure 3.7 SEM picture of neat CPET foam with 0.12 wt. % moisture ........................... 33
Figure 3.8 SEM picture of neat CPET foam with 0.25 wt. % moisture ........................... 34
Figure 3.9 Water content change of filtrated AC under ambient condition...................... 35
Figure 3.10 SEM picture of CPET/0.5 wt. % AC /0.05 wt. % water foam ...................... 36
Figure 3.11 SEM picture of CPET/0.5 wt. % AC/0.13 wt. % water foam ....................... 36
Figure 3.12 SEM picture of CPET/0.5 wt. % AC/0.2 wt. % water foam ......................... 37
Figure 3.13 SEM picture of CPET/1.0 wt. % AC/0.40 wt. % water foam ....................... 37
Figure 3.14 Cell density change with increasing extent of hydrolysis ............................. 38
Figure 3.15 Cell size change with increasing extent of hydrolysis................................... 38
Figure 3.16 Die pressure under different water contents .................................................. 39
Figure 3.17 Intrinsic viscosity of CPET foams ................................................................. 40
Figure 3.18 Shear viscosity of CPET foams ..................................................................... 41
Figure 3.19 Water content change of dried resin and AC................................................ 42
Figure 3.20 DSC Thermograms of PET foams ................................................................. 43
Figure 3.21 Cell morphology of CPET with 0.12 wt. % moisture /0.2 wt. % mGr foam 45
Figure 3.22 Cell morphology of CPET with 0.12 wt. % moisture /0.5 wt. % mGr foam 46
Figure 3.23 Cell density change with increasing mGr content ......................................... 46
Figure 3.24 Cell size change with increasing mGr content .............................................. 46
Figure 3.25 Mechanical properties of PET foams prepared by controlled hydrolysis ..... 47
Figure 3.26 Welding extruded rods into thin sheets. ....................................................... 48
Figure 3.27 Thermal stability of different foams from 25℃ to 200 ℃ ............................ 49
Figure 3.28 Temperature of the air at 2 inches above the roof ......................................... 51
Figure 3.29 Roof upper surface temperature change using different roofing materials ... 51
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Figure 3.30 Indoor temperature change using different roofing materials ....................... 51
Figure 3.31 Foam samples prepared by strand die ........................................................... 52
Figure C.1 TGA and water content of wet activated carbon put in the atmosphere after
water filtration (wet AC = dried for around 20 hours in this thesis) ................................ 68
Figure C.2 TGA and water content of different types of activated carbon ....................... 68
Figure C.3 Water content of neat CPET resin with moisture (measured by HR83 Halogen
Mettler Toledo and data points collected manually)......................................................... 69
Figure D.1 Shear viscosity of CPET and XPET Resins ................................................... 70
Figure E.1 SEM picture of CPET/0.2 wt. % mGr (both dried) foam ............................... 71
Figure E.2 SEM picture of CPET/0.5 wt. % CNT (both dried) foam ............................... 71
Figure F.1 DSC thermograms of Commercial PET foam ................................................ 72
Figure F.2 DSC thermograms of Crosslink PET (XPET) foam ...................................... 73
Figure F.3 DSC thermograms of Virgin CPET resin ........................................................ 73
Figure F.4 DSC thermograms of Neat CPET foam (moisture content ~ 0.05 wt. %) ..... 74
Figure F.5 DSC thermograms of Neat CPET foam (moisture content ~ 0.09 wt. %) ..... 74
Figure F.6 DSC thermograms of Neat CPET foam (moisture content ~ 0.12 wt. %) ...... 75
Figure F.7 DSC thermograms of Neat CPET foam (moisture content ~ 0.25 wt. %) ...... 75
Figure F.8 DSC thermograms of CPET/0.5 wt. % AC /0.05 wt. % water foam .............. 76
Figure F.9 DSC thermograms of PET/0.5 wt. % AC/0.13 wt. % water foam .................. 76
Figure F.10 DSC thermograms of PET/0.5 wt. % AC/0.20 wt. % water foam ................ 77
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Chapter 1. Background and Literature Review
1.1 Introduction
Polymeric foam, an extension of polymer materials, is a two-phase structure with gas
voids surrounded by a continuous polymer phase. In the context of light-weight and eco-
friendly materials, polymeric foams gained considerable interest from the industry.
By selecting appropriate polymers and adjusting the foam density and morphology,
people can tailor the foam properties for a variety of applications 1 (Table 1.1). Polymer
foam is an ideal packaging material because of its light weight and excellent
chemical/electrical resistance. Also, due to the low thermal conductivity of the gas phase,
Table 1.1 Foam applications 1
Functions Markets Properties Typical polymers
Cushioning Furniture,
transportation,
construction
Energy
absorption,
flexibility
Flexible PU, PE,
ABS
Insulators Construction,
automotive
Low thermal
conductivity,
sound absorption
Rigid PU, PS, PE,
rigid PVC
Protection Packaging Soft and flat
surface cushioning
RIM PU, PS bead,
PE and PP sheet
Strength/weight Athletics, construction,
marine, medical,
decoration, household
Strength and
softness
RIM PU, x-linked
PE, PS, PVC,
flexible PU
phenolic, acrylics
Chemical/electrical Packaging, electrical Chemical and
electrical inertness
Flexible vinyl
epoxy, silicones,
rubber
low density foam is widely used as thermal insulator. Depending on the rigid/flexible
nature, foams can also serve as structural materials for construction and furniture. Currently,
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both industry and academia have a wide range of research interest on polymeric foams,
including nanocellular foams with ultra-low thermal conductivity, nanocomposite foams,
biodegradable foams, etc. 2-8.
With increasing demand on energy conservation and environmental protection, the
insulation properties of the foam as roofing or external wall need to be further improved.
If more heat can be shielded, less energy (air conditioning) will be consumed to control the
indoor temperature. Basically, heat transfer through foam block can be divided into
conduction (in both gas and solid phase), convection (gas phase) and radiation (block). Due
to the closed cell structure, the convection is almost negligible. Also, it is difficult to change
the heat conduction in gas and solid phase (accounts for 75% of total heat transfer) when
the blowing agent and polymer matrix are selected 9. Radiation heat transfer, which
accounts for about 25% of total heat transfer, provides room for further improvement by
reducing the transmission of infrared radiation (IR). Infrared attenuation agent (IAA) is an
effective additive for absorbing IR. A wide range of IAA has been reported including
carbon particles, certain organic chemicals and conductive polymers 10-12.
Currently, polystyrene foam (PS) including expanded polystyrene (EPS) and
extruded polystyrene (XPS) is the major insulator material and it occupies around 75 % of
the external wall insulation markets 13. However, PS and IAA do not seem to be a feasible
combination. The foam roof made with IAA can easily reach around 100℃ which is
beyond the extreme temperature of PS. To find a suitable substitute for PS foam, we
attempted to prepare semi-crystalline polyethylene terephthalate (PET) foams with high
thermal stability and good IR-absorption performance for roofing and external wall
applications.
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1.2 Extrusion Foaming
Among various mainstream foaming technologies (batch foaming, injection
molding foaming, reactive foaming for thermoset polymer, etc.) 14, extrusion foaming is a
continuous and large-scale processing method for thermoplastic foams.
Blowing agent is used to introduce gas voids into the polymer matrix. It can be
categorized into physical blowing agent (PBA) and chemical blowing agent (CBA).
Physical blowing agent includes inert gas such as nitrogen (N2), argon (Ar) or carbon
dioxide (CO2) and volatile hydrocarbon such as hydrochlorofluorocarbon (HCFC),
hydrofluorocarbon (HFC), pentane, etc. Chemical blowing agent generates gas bubbles
through chemical reactions or thermally induced deposition 14. Generally, physical blowing
agent is more widely used for low density foams 1.
Extrusion foaming is a complicated process and it covers a wide range of disciplines
such as thermodynamics, mass transfer, gas/polymer rheology, kinetics of crystallization,
and chemical reactions (for reactive foaming)14. The mechanism basically applies to almost
all foaming methods using either chemical or physical blowing agents (Fig 1.1).
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Figure 1.1 Foaming mechanism 14
Step 1: Formation of gas/polymer homogeneous phase
With a blowing agent injected to extruder in the melting zone, a homogeneous
phase of polymer melt and gas blowing agent is formed. Adequate solubility of blowing
agent is required. Also, a specified ratio of gas/polymer melt flow rate is required to ensure
the formation of saturation blends. If the gas flow rate is too high, the undissolved gas
would shot out from the extruder and lead to a unstable processing condition. If the gas
flow rate is too low, the low concentration of dissolved gas would limit the foam expansion.
Step.2: Bubble nucleation
Under sudden pressure drop (e.g. extruded from the die during extrusion foaming),
the saturated gas/polymer mixture reaches over-saturated. The instability of the metastable
system leads to the formation of nuclei which become growing sites for the gas bubble in
later stages. The steady state homogeneous nucleation rate can be described by the classical
nucleation theory 4
𝑁1 = 𝐶0𝑓1 exp (−∆𝐺𝑐𝑟𝑖𝑡
𝑘𝐵𝑇)
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∆𝐺𝑐𝑟𝑖𝑡 = 16𝜋𝜎3
3∆𝑃2
C0 - Number of gas molecules dissolved per unit volume of primary phase;
f1 - Coefficient weakly depending on temperature
𝐺𝑐𝑟𝑖𝑡 - Critical Gibbs free energy of nucleation
𝑘𝐵 - Boltzmann constant
T - Foaming temperature
∆𝑃 - Pressure drop
𝜎 – Surface tension of gas bubble/polymer interface
The nucleation rate is strongly influenced by the solubility of the blowing agent,
foaming temperature and rate of pressure drop. If the nucleation happens at the interface
of the two-phase (heterogeneous nucleation), the classical theory above can be modified
which will be discussed in Section 1.6.
Step.3: Bubble growth
When the gas nuclei form, the gas molecules in the polymer matrix start to diffuse
into the nuclei and the gas bubbles start to grow. The phase separation becomes more
significant and the metastable system gradually stabilizes. During this period, the gas
bubble may collapse or combine with one another. Depending on the interconnectivity of
the gas bubbles (resulting from cell wall breaking when bubbles grow bigger), open cell
or close cell foams can be obtained for completely different applications. Gas diffusivity,
polymer melt viscosity, the rate of polymer crystallization, etc. are closely related to
bubble growth. Basically, bubble growth and gas nucleation compete with each other,
significantly affecting the final cell morphology.
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Step.4: Stabilization and solidification
Upon further cooling, the polymer melt viscosity increases and the gas bubbles
gradually stop growing when the melt solidifies. Due to the concentration difference of
the blowing agent inside and outside the foam, the air gradually replaces the blowing
agent in the gas bubble after foaming and eventually a new balance is obtained.
1.3 Polyethylene Terephthalate
Polyethylene terephthalate (PET) is a well-known synthetic polyester. The PET
molecular structure is shown in Fig 1.2. It has wide applications including water bottles,
containers, films (food packaging), fibers (clothing), electrical instruments, etc.15. As a
thermoplastic polymer, PET resins are mostly melt processed by extrusion and injection
molding into products of various geometries. Virgin PET resins can be either amorphous
PET (APET) or semi-crystalline PET (CPET) 1. The transparent APET is widely used as
water bottles while the opaque CPET is mainly used for the trays of oven-ready meals due
to its high thermal stability 16.
Figure 1.2 Polyethylene Terephthalate (PET)
However, PET is not biodegradable due to the difficulty of breaking up the ester
linkage and current technology requires complex procedures to decompose it biologically
17. Therefore, due to the tremendous demand of PET products, huge amount of PET bottles
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end up in landfill, causing severe environmental concerns around the world. It is predicted
that ‘by 2050, there will be as much waste plastic in the ocean by mass as there are fish’ 18.
Moreover, researchers also reported the health concern due to the migration antimony (Sb)
from landfill PET products, an important catalyst during polycondensation 19.
Attempts of developing approaches for treating plastics are being pursued. Some
bacteria were discovered and engineered for biodegrading PET with high efficiency 20.
However, it is a long way to go for those trials to be realized at industrial scale. So far,
post-consumer recycling is still the most practical and economic treatment. The
conventional mechanical recycling process includes washing of PET flakes (removing the
contamination), drying and melt processing into new resins again for further new product
manufacturing 21.
Foaming of Recycled PET, as a possible recycling application, has been gaining
great interest from the industry. In addition to protecting the environment, foaming PET
has huge potential for high temperature and high mechanical strength applications due to
its semi-crystalline nature, which can further expand the application spectrum of the current
market dominating foams such as polystyrene (PS), polyurethane (PU) or poly (vinyl
chloride) (PVC).
1.4 Challenges of PET foaming
It’s challenging to foam virgin PET resins into low density by extrusion foaming
since linear PET has low melt strength 1, 21, 22. The melt strength is closely related to the
rheological behavior. Due to the low melt viscosity/elasticity, the gas bubble cannot be
stably retained during foaming. The weak cell walls cannot hold the growth of gas bubble,
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leading to the collapse and coalescence of the fine cell structures. The low melt strength
also results from the slow rate of crystallization of neat PET 1, 23, 24. Therefore, it takes a
relatively long time period to stabilize and harden the foam from melt state, during which
collapse and shrinkage may inevitably take place. Also, the high processing temperature of
PET (Tm ~250℃) and its crystallization behavior further narrow the processing window
during foaming. Another difficulty of getting low density foams is that the density of PET
is 1.38 g/cm3, higher than many other polymers 21. It’s much more challenging to make the
density of PET foam as low as the commercial PS foam whose resin density is merely 1.04
g/cm3.
Other concerns are the hydrolysis and thermal degradation of PET under high
temperatures25-28. When the materials are exposed to oxygen, thermal oxidation of PET
also happens 29. As a result, chain scission and the corresponding loss of molecular weight
will lower the melt viscosity, which further worsens the foaming behavior. The mechanical
property of the final products could be severely reduced as well due to the low molecular
weight. Therefore, thoroughly removing moisture before melt processing is the key to
obtain high quality foams, which is adopted by almost all of the research and industrial
studies mentioned below 33-42.
1.5 Conventional Approaches
To improve the foamability and avoid the problems mentioned above, chemical
modification of PET resins is currently the most common approach.
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1.5.1 Copolyester
Copolyester of PET is synthesized by adding comonomer during the
polycondensation reaction (monomer: terephthalic acid and ethylene glycol). The
properties of PET are changed significantly due to the comonomer introduced. Glycol-
modified PET (PETG) is a typical example developed by Eastman 1. By adding
cyclohexanedimethanol as a comonomer, the melt strength of PETG is much higher than
that of normal PET. Also, its glass transition temperature (Tg) and melt temperature (Tm)
become much lower. PETG shows no crystallization and changes the resin from semi-
crystalline to amorphous. Therefore, it can be more easily foamed and allows for wider
processing window and easier processing conditions 30. Handa, C.P. et al successfully
produced PETG foam with a density of 0.04 g/cm3 by batch foaming using CO2 as a
blowing agent 31. Park, C.P. et al investigated the foaming behavior of PETG under
extrusion foaming using a mixed blowing agent of HCFC-142b and ethyl chloride (EtCl)
32. The secondary foaming and moldability were also investigated. Despite the improved
foamability, PETG suffers from low thermal stability (Tg ~ 80℃) and weak mechanical
strength due to its amorphous structure. Therefore, its application is largely limited.
1.5.2 Resin Chain Extension
Besides starting from polymerization, resin modification by melt modification (in
a batch mixer or extruder) or solid-state polycondensation has been widely reported. The
basic principle of chain extension is to increase the molecular weight of linear PET and the
corresponding intrinsic viscosity ([η]). The chain extenders are basically chemicals with
multifunctional groups that can react with hydroxyls and carboxyl end groups of PET
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molecules. Common chain extenders contain functionalities such as cyclic anhydride,
epoxide, oxazoline, isocyanate or carbodiimide, etc.33. The reaction of PET with
pyromellitic dianhydride (PMDA), one of the most widely used chain extender, is shown
in Fig 1.322. Depending on the extent of the reaction, the branching or even crosslinking or
gel-like structures can be formed. The long-chain, branching, or crosslink PET has higher
melt strength and improved foamability compared to the linear PET.
Figure 1.3 Chain extension and branching of PET by PMDA 22
Xanthos, M et al investigated the extrusion foaming of different PET resins by both
chemical and physical blowing agents 34. Resins modified by branching agent or reactive
processing showed significantly higher expansion than virgin resins. Foams with density
of around 0.10 g/cm3 were obtained by using CO2 as a blowing agent. They also compared
the foamability of both virgin resins and modified resins using different physical blowing
agents (N2, Ar, CO2) 35. Also, the rheological behavior of the resins was investigated and
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correlated to the foamability. Xanthos group also investigated the effect of a variety of
chain extension and branching agents on PET rheology and foaming behavior such as
diepoxide, ethylene-glycidyl methacrylate copolymer 36, triglycidyl isocyanurate 37,
dianhydride 38 and some commercial oligomers 39. To modify the resin with these additives,
batch mixing, reactive extrusion and their processing conditions were researched 36-38. In-
situ Polymerization-modification and solid state polycondensation were also applied as a
supplemental approach for chain extension reaction 40, 41. The modified PET resins are also
widely used in batch foaming process foaming 39-42.
However, resin modification by chain extension or branching tends to reduce the
relatively high crystallinity of the final products. The loss of the linear chains inhibits the
crystallization and leads to relatively poor thermal and mechanical properties.
1.6 Non-chemical Modification Approach
To the best of our knowledge, very few non-chemical method of PET foaming has
been reported. In this thesis, we try to develop a non-resin modification approach to foam
CPET for thermal insulation applications. Without changing the PET linear structure, the
high crystallinity can be kept and thus high thermal stability and mechanical strength.
1.6.1 Optimization of Foaming conditions
It’s highly challenging to significantly improve the foaming behavior of PET by
simply controlling the processing conditions. Xanthos, M et al investigated the relation
between foam expansion and screw rotation speed, resin intrinsic viscosity, and ratio of
chemical blowing agent 33. Barzegari, M. R. et al compared die pressure influence on the
foam expansion and cell density of different PET resins 43. Fan, C. et al systematically
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investigated the amount of physical blowing agent and die temperature during PET
extrusion foaming 44. Both higher gas flow rate and lower die temperature were
advantageous to lower the foam density. Although optimization of processing condition is
advantageous for foaming modified resins, but this approach does not work well for
crystalline resins because of the very narrow processing window. In this study, we take all
the mentioned parameters into consideration for the experimental design.
1.6.2 Controlled-Hydrolysis
Although degradation or hydrolysis of PET during melt processing is not favorable
in most cases and should be avoided (Section 1.4), controlled-degradation can allow for
better foam expansion of PET 1. Very few research was reported on controlled-degradation
for extrusion foam, but the effect of molecular weight (or intrinsic viscosity) on PET foam
was investigated in many cases.
Guo, H. et al compared the foam expansion of virgin PET resins with different
molecular weight 45. They found that lower IV resins might be more favorable for low
density foams. Zheng, W.G. et al reported that a high IV PET (1.19 dL/g) led to
microcellular foams but with poor expansion ratio in extrusion foaming, while a higher
expansion ratio was obtained by foaming a lower IV resin (0.8 dL/g) 46. Wet and dry PET
resins were compared by Barzegari, M. R. et al for extrusion foaming, and they found that
the expansion ratio of a wet PET resin was 3 times higher than that of a dry resin 43.
However, they didn’t try to optimize the water content so that excessive degradation
happened and the molecular weight became too low, which led to low melt strength and
cell collapse. All these studies indicated that lowering the molecular weight is likely to
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obtain low-density crystalline PET foam if we can carefully control the extent of
degradation reaction.
Herein, we define the controlled-hydrolysis as lowering the molecular weight to an
acceptable level for better foam expansion (not too low in case of poor mechanical
property). In this thesis, we would like to systematically investigate the effect of water
content and the choice of hydrolysis agent (or water carrier) to balance the foam density,
cell morphology and crystallinity for low-density foam with desirable mechanical and
thermal properties.
1.6.3 Selection of Hydrolysis Agent
Water is widely used in extrusion foaming mainly as a co-blowing agent to
manipulate the cell morphology because it is low-cost, benign and environmentally-
friendly. The way to introduce water may make a great difference to the foam morphology
47. For hydrophilic materials, using moisture is the simplest approach 48, 49. PET resins
absorb water under ambient temperature and pressure. The moisture not only attaches to
the surface of the resins but also diffuses into the core of the resins which cannot be easily
removed due to the hydrogen bond. Activated carbon (AC) is another choice of water
carrier. Due to its complicated porous structure, it has great potential to trap a large quantity
of water. The water held by the micro-scale porous structure is quite stable under high
pressure during extrusion while gasifies under sudden pressure drop. Therefore, we expect
water in AC can act as a co-blowing agent as well. Research on using water as a co-blowing
agent to manipulate the cell morphology was reported by our group in the past years. Yeh,
S.K. et al applied CO2 and water (carried by AC) as a dual blowing agent to prepare PS
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14
foams which had large cell size and lower density for improved the insulation property 47.
Zhang, C.L. et al formed the bimodal cell structures when using the dual blowing agent to
foam PS 50 and they further investigated the effect of carbon particles on the cell
morphology 51.
1.6.4 Mircographite as IAA and Nucleation Agent
We also use micrographite as IAA for IR-absorption application. Micrographite has
high IR-absorption efficiency among the carbon particle family, which was demonstrated
by our lab before 10. Also, carbon micro/nano-scale particles are widely used as nucleation
agents in extrusion foaming. The heterogeneous nucleation rate can be simply obtained by
modifying the free energy term in classical nucleation theory (Section 1.2) which can be
described by
∆𝐺𝑐𝑟𝑖𝑡 = 16𝜋𝜎3
3∆𝑃2
𝑓(𝑚, 𝑤)
2
𝑓(𝑚, 𝑤) is the energy reduction factor (≤ 1 ) which is a function of the contact angle
between gas, polymer and nanoparticle, and the relative curvature of the nucleant surface
to the critical radias of the nucleated phace 4. The cell morphology of the composite foam
is affected by aspect ratio, dispersion and surface chemistry of nanoparticles. The effect of
carbon nanotube, nanoclay, carbon nanofiber, etc. on foaming PS, PMMA and PP were
reported 52-56. So far very few research has been reported on using carbon particles to
manipulate the PET foaming behavior (several batch foaming of PET/clay nanocomposite
foam was reported 57, 58). Therefore, this will be another highlight of this thesis.
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1.7 Objectives
• Proposed formulation: crystalline PET (CPET)/ moisture or activated carbon
(AC) (hydrolysis agent) / micrographite (mGr) (IAA);
• Foaming CPET resin by controlled-hydrolysis to produce low density foams
(density < 0.20 g/cm3), comparable to the foam made by chemical-modified
resins;
• Investigating the effect of water content and the type of hydrolysis agent on foam
density/morphology, extent of degradation and crystallinity;
• Keeping high crystallinity of PET and the corresponding high thermal stability
and mechanical strength;
• Using mGr as IAA and nucleation agent to manipulate the foam morphology;
• Conducting lab demo of applying our PET foam for IR-absorbing roofing and
external wall applications.
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Chapter 2. Materials and Experiments
2.1 Materials and Processing Equipment
A crystalline PET resin (Laser+® C E60A) with crystallinity > 50% and a
crosslink PET resin (Array 3962) were supplied by DAK Americas. The blowing agent
hydrofluorocarbon (HFC, R134a) was purchased from DuPont. The boiling temperature
is -26.3°C. Coconut shell activated carbon (AC) from Carbon Resources was chosen as
water carrier. Micro-graphite (mGr) from Qingdao Yanhai Carbon Materials Inc. was
chosen as nucleation and IAA agents.
Table 2.1 Material description and pre-treatments
Material Specification Description Treatments
before use
Crystalline PET
(CPET)
Laser+ E60A, DAK
America
I.V.= 0.81 dL/g
Tm = 245 ℃
Dried at 130℃
overnight
Crosslink PET
(XPET)
Array 3962, DAK America I.V.= 0.67 dL/g
Tm = 230 ℃
Dried at 120℃
overnight
Activated carbon
(AC)
Carbon Resources
Company, USA
Made from
coconut shell,
diameter 7 µm
Varied from
different purposes
Micro-Graphite
(mGr)
Qingdao Yanhai Carbon
Materials Inc., China
Thickness: ~0.5
µm
Stored in a
desiccator
A Leistritz (German) twin screw extruder (Fig 2.1) was used for foaming. The
diameter of the screws is 27 mm and the length to diameter ratio (L/D) is 40:1. There are
11 temperature zones under control (9 in the extruder and 2 in the die). The materials are
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fed into the extruder by a feeder and the speed can be controlled automatically. The
physical blowing agent is injected into the extruder in zone 4 by a syringe pump.
Figure 2.1 Leistritz twin screw extruder
2.2 Foam Extrusion of Crystalline PET (CPET) Resins by Controlled-Hydrolysis
2.2.1 CPET Foaming with Moisture
To control the water content, we dried the resin for different time periods under
120℃ (conditions listed in Appendix A). To note, the drying condition varied with the
moisture content which depends on the storage time and conditions. Therefore, it was
necessary to change the drying condition from time to time. The reins with different water
contents were for further water content test and extrusion foaming.
2.2.2 CPET Foaming with Wet Activated Carbon
Activated carbon (AC) was used as a water carrier. Fig 2.2 shows how to fill the
porous structure of AC with water. First, AC particles were completely immersed in water,
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during which stirring was necessary to make a uniform suspension. Second, the AC/water
suspension was placed overnight to allow water diffusion into the porous structure, which
was then vacuum filtrated and left under ambient condition for 24 hours to evaporate the
excessive water. Third, the filtrated cake was grinded into wet AC particles for extrusion
foaming. The wet AC was dried for 5 min at 100℃ and we also compared AC without
treatment (contain certain amount of water under storage condition)
AC was premixed with dried PET resins by handshaking in a plastic bag for foam
extrusion (formulations listed in Appendix A).
Figure 2.2 Preparation of wet AC
2.2.3 Extrusion Foaming and Condition Optimization
3 kg of all the ingredients for each formulation mentioned in Sections 2.2.1 and
2.2.2 were prepared for extrusion foaming. The previous residue inside the extruder was
purged out and the steady processing condition was reached before each run.
Fig 2.3 shows the procedures of extrusion foaming. PET resins with
micro/nanofillers or water carriers were continuously fed into the hopper by a single screw
feeder. The HFC was first filled in a syringe pump and then injected into the polymer melt
(zone 4). Then the blowing agent was mixed with and dissolved into the PET melt in the
extruder. The temperature setting of the first nine zones were fixed for all formulations.
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Temperatures of zones 1 to 3 increased gradually from 230℃ to 260℃ for solid conveying.
Temperatures of zones 3 to 10 changed from 260℃ to 250℃ for melting, mixing and
pressurizing. When the gas/polymer mixture was extruded from the capillary die (Fig 2.4),
the foam was obtained under the pressure drop. The strand-shaped samples were collected
manually 15 ~ 20 cm below the outlet of the die by a putty knife when the whole system
reached steady state (stable die pressure, no blowing agent shooting out).For foaming with
water, all the foaming conditions with different water content were kept the same as
foaming dry PET resins (Appendix C.1). Therefore, the foaming behaviors under different
water contents were mainly attributed to the water content, while any difference caused by
processing conditions was excluded.
Figure 2.3 Foam extrusion diagram
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Figure 2.4 Capillary die and its geometry
2.3 Sample Characterization
2.3.1 Foam Density
According to ASTM D792, a homemade device is used to measure the bulk density
of the foam samples. It can be expressed as
ρ𝑓𝑜𝑎𝑚 = 𝑚𝑓𝑜𝑎𝑚
𝑚𝑓𝑜𝑎𝑚 + 𝑤 − 𝑏 ρ𝑤𝑎𝑡𝑒𝑟
𝑚𝑓𝑜𝑎𝑚 is the true mass of the foam sample in air. 𝑤 is the weight measured when
the sinker is immersed completely in water without the foam sample. To note, the water
bath is on a shelf without any contact with the balance. 𝑏 is the weight measured when the
sinker bundled with the foam is immersed completely in water.
2.3.2 Water Content
The water content in AC was measured by thermogravimetric analysis (TGA). The
weight loss in the range from 50 to 200℃ was determined as the water percentage.
The water content of PET resins was measure by a HR83 Halogen Mettler Toledo
instrument. The water content was determined by the total weight loss at 180℃ for 8 hours
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in which we assume all water can be removed from the resins under this condition. The
weight loss under resin drying condition (120℃) was also measured. Based on these two
tests, the water content of the resins could be obtained.
2.3.3 Cell Morphology
A FEI Nova NanoSEM 400 scanning electron microscope (SEM) system was used
to characterize the cell density and cell size of the foam. Foam samples were first immersed
in the liquid nitrogen for 5 minutes before cracking. The sample was then stick to a SEM
platform with the fracture surface upwards. A 1 to 2 nm thin layer of platinum was coated
on the sample for imaging.
The cell density (N0) is the number of cells per cubic centimeter and can be
expressed by
𝑁0 = (𝑛
𝐴 )
32
ρ𝑢𝑛𝑓𝑜𝑎𝑚𝑒𝑑
ρ𝑓𝑜𝑎𝑚
Where n is the number of the cells in a single SEM picture and the A is the area of
this SEM picture. ρ𝑓𝑜𝑎𝑚 is the foam density and ρ𝑢𝑛𝑓𝑜𝑎𝑚𝑒𝑑 is the density of the sample
following the same formulation and processing condition but not adding blowing agent.
By analyzing the SEM picture using ImagePro Plus software, the average cell
diameter (D) can be obtained, which can be expressed by:
𝐷 = ∑ 𝑛𝑖𝑑𝑖
∑ 𝑛𝑖
Where 𝑛𝑖 is the number of cells with the diameter 𝑑𝑖 in the SEM pictures.
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2.3.4 Molecular Weight
To quantify the extent of hydrolysis during extrusion, the molecular weight of the
foams was determined by measuring the intrinsic viscosity according ASTM D4603-18.
The solvent was a mixture of phenol and 1,1,2,2-tetrachloroethane with a mass ratio of
60:40. PET foams were dissolved in the solvent with a concentration of 0.5 g/dL at 110°C
for 15 min. The time of the PET solution flowing through the two marks of the ubbelohde
type viscometer was recorded (Fig 2.5).
Figure 2.5 Viscometer
The intrinsic viscosity [𝜂] of PET was defined by the Billmeyer relationship:
[𝜂] = 0.25𝜂𝑟 − 1 + 3ln (𝜂𝑟)
𝐶
𝜂𝑟 − 𝑟𝑒𝑑𝑢𝑐𝑒𝑑 𝑣𝑖𝑠𝑐𝑜𝑠𝑖𝑡𝑦 𝑒𝑞𝑢𝑎𝑙𝑙𝑖𝑛𝑔 𝑡1
𝑡0;
𝑡0 − average solvent flow time, s;
𝑡1 − average solution flow time, s;
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C – concentration of the PET solution, 0.5 dL/g
The viscosity-average molecular weight (Mv) can be calculated by the Mark–
Houwink equation: [η] = KMv𝑎 . For PET, constant K and a equals 7.44 × 106 mL/g and
0.648 respectively 59.
2.3.5 Shear Viscosity
Flowability of the polymer melt is determined by measuring the shear viscosity.
The resin or pellets samples were dried under 120℃ overnight and then hot-pressed into
disks with at least 1 mm thickness. The foam samples were first grinded into small pieces
and dried under 120℃ overnight before hot press. Then the shear viscosities were
measured by a parallel plate rheometer (ARES II, TA instrument) at 260℃ for the shear
rate ranging from 0.1 to 1000 rad/s. In addition, the polymer chain length is closely related
to the shear viscosity, from which we can also qualitatively compare the molecular weight
of PET foams.
2.3.6 Crystallinity
Crystallinity of the foam was characterized by Differential Scanning Calorimetry
(DSC, Q200, TA Instrument). The heat flow of the foam samples was recorded by heating
the samples from 30℃ to 300℃ at a rate of 10℃ per minute. To obtain the crystallinity,
the area of the melt peak and cold crystallization peak can be integrated from the heat flow
versus temperature graph. The crystallinity can be calculated by 60:
Crystallinity X𝑐 % = ∆𝐻𝑚−∆𝐻𝑐
∆𝐻𝑚0 × 100 %
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Where ∆𝐻𝑚 is the melt enthalpy; ∆𝐻𝑐 is the cold crystallization enthalpy; ∆𝐻𝑚0 is the 100%
crystallization enthalpy of PET and can be found in the polymer handbook 61.
2.4 Functional Properties Measurement
2.4.1 Tensile Test
The tensile behavior of the foams were measured by an RSA3 instrument (TA
Instruments, USA). The cylindrical-shaped foams with diameter ranging from 1.90 mm to
2.5 mm depending on the expansion ratio were collected during extrusion and cut into 30
mm length. During the test, the samples were fixed tightly to avoid slippery between two
clamps with a gap of 10 mm. The stress and stain were recorded when the sample were
stretched under a constant strain rate (0.008 s-1).
2.4.2 Thermal Stability
The strand-shaped foams were first welded into sheets and cut into the same size (1
cm × 3 cm). As shown in Fig 2.6, they were set at the margin of the plate with one side
pressed by a weight. The plate was heated up in an oven from room temperature to 220℃.
The thermal stability was observed at different temperatures when the samples softened,
collapsed or decomposed.
Figure 2.6 Thermal stability test within the temperature ranging from 25℃ to 220℃
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2.4.3 Insulation Measurements
The heat transfer of the foams under Infra-red radiation was measured by
mimicking the roof of the house or vehicles (Fig 2.7 and 2.8). Different foam samples (cut
into 2.5 cm × 2.5 cm) were used as roofing materials for comparing the insulation
performance. The side wall and the bottom wall with a cylindrical dimension (diameter: 2
cm, height: 2.5 cm) were made from polystyrene foam with a thickness of 2 mm. The infra-
red lamp was placed 25 cm top right above the foam roof. To better mimic the real
condition, convection was caused by a fan at the side of the infrared lamp. Accordingly,
the temperature above the roof would not be too high with more heat removed by air
convection. Otherwise, the heat of the roof would mostly transfer to the indoor region,
which is not likely to happen in the real condition.
During the experiment, the roof and indoor temperatures were measured
simultaneously by two thermocouples once the IR lamp was switched on. One more
thermocouple was used to monitor the temperature two inches above the foam roof.
Figure 2.7 Diagram of Mimicking the IR-absorbing roof application
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Figure 2.8 Experiment setting of the IR-absorbing roof application
2.5 Strand Die Design and Experiments
A strand die was designed to verify the applicability of our approach to the potential
industrial manufacturing. Due to the foam expansion at the outlet of the strand die, the
extrudate can be welded together and the plate-shaped foam can be obtained (Fig 2.9),
which is very widely applied to the industrial-scale processing.
Figure 2.9 Schematic of the strand die
We tried to repeat the optimum foaming results under the same processing condition by
simply dividing the 1 mm diameter hole into multiple holes (making total hole area the
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same). We can estimate the strand die geometry by using the capillary rheometer function
which can be expressed by 62:
𝑄 = (∆𝑃𝑅
2𝑚𝐿)
1𝑛
(𝑛𝜋𝑅3
1 + 3𝑛)
Q – flow rate;
∆𝑃 – pressure drop;
𝐿 – length of the capplilary;
R – radius of the capplilary;
n – power law parameter
Here, we assume the same total flow rate and set n = 1 by considering the polymer melt as
Newtonian fluid. Then the equation above can be simplified to 𝑃 ∝ 𝐿
𝑑4 . Therefore, we
can obtain the die geometry under several holes (Table 2.2), which are supposed to achieve
the equivalent function of the capillary die.C
Table 2.2 Theoretical design of the strand die
Hole number Diameter(mm) Length(mm)
Capillary die (one-hole) 1 12
3 0.58 4
4 0.5 3
5 0.45 2.5
6 0.41 2
The theoretical calculation can provide a good starting point while further modification by
trial and error is always necessary. In our experiment, we started from 5 holes, 0.5 mm
diameter and 2.5 mm length. However, such design causes unexpectedly high die pressure
under the same foaming condition and thus we put two more holes to reduce the die
pressure. In the end, we obtained the optimized die geometry (7 holes, 0.5 mm diameter
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and 2.5 mm length) shown in Fig 2.10. The deviation of the optimized condition from the
theoretical value is probably because of the Newtonian fluid assumption. Also, the same
total flow rate assumption may not be perfectly valid due to the geometry change of the die
(comparing Fig 2.4 and 2.9).
Figure 2.10 Optimized strand die geometry
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Chapter 3. Results and Discussion
3.1 Optimization of Processing Conditions
The optimized foaming conditions are summarized in Appendix B.
The melting zone setting for CPET is ranged from 260℃ to 245℃ (melt
temperature around 245℃). Due to the narrow processing window, the die temperature
was not able to be lower than 235℃ (heat transfer issue). Under each die temperature from
255℃ to 235℃, the influence of screw revolution rate, feeding rate and gas flow rate were
also investigated. They were adjusted and coordinated under each die temperature from
255℃ to 235℃. The optimized processing conditions is shown in Table B.1. To note, we
didn’t find any significant effect of die temperature difference on the expansion ratio of
CPET foams.
The crosslink PET (XPET) has a lower melting point and a much wider processing
window than CPET. The processing temperatures were thus much lower and the die
temperature could be lowered than 215℃. In this case, the lower die temperature
significantly increased the foam expansion ratio, which coincided with what was reported
by Barzegari, M.R. et al 43. Same procedure as mentioned above was adopted to optimize
the processing conditions which are shown in Table B.2.
When foaming PET by controlled hydrolysis approach, we adopted the same
optimized processing conditions of neat CPET (Table B.4&5). For both moisture and AC
based formulations, the foams were extruded at 15 rpm (screw revolution rate), 130 rpm
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(feeding rate) and 2 ml/min (blowing agent flow rate) to compare the results. Die pressure
for using AC as hydrolysis agent dropped to 600~1000 psi (depending on the water content)
while it dropped to 200 ~ 800 psi by adding moisture.
3.2 Neat PET Foams
The density and cell morphology of CPET and XPET foams prepared under the
optimized conditions are shown in Table 3.1. A commercial PET foam was also tested for
comparison. Both XPET foam and commercial PET foam has a much lower density than
the CPET foam. XPET foam prepared in our lab has a higher density than the commercial
one. This is probably because XPET resin has intrinsic viscosity around 0.66 dL/g, not
desirable enough for foam application. Most of modified resins showing excellent
foamability reported in the literature have a much higher IV (> 0.8 dL/g). The non-uniform
cell size and relatively low cell density can also be attributed to the low IV and the
corresponding low melt strength. In addition, our lab-scale extruder cannot reach high
pressure (maximum die pressure ~1600 psi), which limited the rate of pressure drop for
desirable nucleation efficiency.
Table 3.1 Density, cell morphology and crystallinity of neat PET foams
Sample Density
(g/cm3)
Cell density
(cells/cm3)
Average cell size
(µm)
Crystallinity
Xc (%)
CPET foam 0.6 4.43×106 44 8.6%
XPET foam 0.18 5.39×105 170 1.6%
Commercial PET foam 0.06 1.31×106 165 5.9%
CPET with IV around 0.80 dL/g showed a much lower expansion ratio than XPET
when using HFC 134-a as a blowing agent. Zheng, W.G. et al reported similar results of
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the foam made by a 0.80 dL/g non-modified virgin resin 46. Figs 3.1 to 3.3 show that CPET
foams has a much higher cell density (4.43×106 cells/cm3) and smaller cell size (44 µm)
than XPET foam and commercial PET foam. The crystallinity of CPET foam is much
higher than XPET due to its linear chain structure.
Figure 3.1 SEM picture of neat CPET foam and the cell size distribution
Figure 3.2 SEM picture of crosslink PET foam and the cell size distribution
Figure 3.3 SEM picture of commercial PET foam and the cell size distribution
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3.3 Foaming CPET by Controlled-hydrolysis
Using either moisture or wet activated carbon as hydrolysis agent, the expansion
ratio of CPET resin was significantly improved (Fig 3.4). The relation between foam
density and water content was plotted in Fig 3.5.
Figure 3.4 CPET foams with moisture or wet AC as hydrolysis agent
Figure 3.5 Effect of water content on foam density depending on different types of
hydrolysis agent (1) moisture (2) 0.5 wt. % AC (3) 1.0 wt. % AC
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3.3.1 Foaming with Moisture
The relation between foam density and water content was plotted in Fig 3.5. Under
the ordinary drying condition (Section 3.2), CPET resins with less than 0.05 wt. % moisture
showed a very low expansion ratio (density around 0.5~0.6 g/cm3). When increasing the
moistrue content, the foam density was significantly lowered. From Fig 3.6 to Fig 3.7, the
cell size became larger and more uniform with increasing the water content while the cell
density decreased to some extent. The cell morphology became more like that of the
commercial PET foam. The optimum water content was 0.12 % for this CPET resin and
the foam density was lowered to about 0.16 g/cm3.
Figure 3.6 SEM picture of neat CPET foam with 0.09 wt. % moisture
Figure 3.7 SEM picture of neat CPET foam with 0.12 wt. % moisture
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Figure 3.8 SEM picture of neat CPET foam with 0.25 wt. % moisture
However, excessive degradation was observed when the water content of the resins
reached higher than 0.2 wt. %. We observed that the extrudate could not hold the gas bubble
growth due to its low melt strength (molecular weight drop too much). Also, the foam could
hardly be shaped. The foam density became higher (Fig 3.5) due to the cell collapse. Low
cell density and large & nun-uniform cell size were also observed (Fig 3.8).
3.3.2 Foaming with Activated Carbon (AC)
The filter cake of activated carbon (AC) was dried under the ambient condition
before grinding into powder for foaming. The water content of AC particles was measured
by testing the sample of different time periods using TGA (Appendix C), which is plotted
in Fig 3.9. After 48 hours, the water content of AC finally reached a balance around 27
wt. %. To avoid particle aggregation due to excessive water, a minimum about 20 hour
drying was required for a 30 g filter cake under 25℃. Otherwise, the AC particles would
not disperse uniformly during premixing with PET resins and then aggregation during
premixing would cause periodical instability during processing. Therefore, in this thesis,
we used wet AC for extrusion foaming right after we grinded it into powder around 24
hours after filtration.
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Figure 3.9 Water content change of filtrated AC under ambient condition
Three types of AC with water content of 10 %, 30 % and 40% (Appendix C) were
prepared as mentioned in Section 2.2.2. A series of parallel experiments using 0.5 and 1.0
wt. % AC as water carrier were conducted to compare the effect of water content and carrier
loading on foam expansion. Due to the particle aggregation mentioned above, using 0.5
wt. % AC could get at most 0.20 wt. % water. Therefore, we also used 1.0 wt. % AC for
testing higher water content conditions.
Similar to the trend of foaming PET with moisture, the foam density decreased
with increasing the water content because of hydrolysis (Fig 3.5). The lowest foam density
was obtained with 0.2 wt. % water content when using 0.5 wt. % AC. Fine cell structure
and uniform cell size were achieved (Figs 3.10 ~ 3.12) with no cell collapse being observed
(no excessive hydrolysis). Although more water can be carried by 1.0 wt. % AC, the foam
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expansion was not as effective as 0.5 wt. % AC loading. This is probably because the slow
screw revolution rate (15 rpm) was not high enough for good dispersion of the AC under
higher filler loading. Also, the excessive hydrolysis was observed when the water content
was 0.40 wt. % (Fig 3.13). Judging from cell morphology, we cannot tell that water in AC
can act as a co-blowing agent as we expected before since the cell geometries obtained by
the two approaches are very much similar. Significant changes of the cell morphology such
as bimodal cell structure were reported when co-blowing agent was applied 47, 50, 51 .
Therefore, we assume that the water trapped by AC mainly served as a hydrolysis gent
while the co-blowing agent effect might be negligible.
Figure 3.10 SEM picture of CPET/0.5 wt. % AC /0.05 wt. % water foam
`
Figure 3.11 SEM picture of CPET/0.5 wt. % AC/0.13 wt. % water foam
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Figure 3.12 SEM picture of CPET/0.5 wt. % AC/0.2 wt. % water foam
Figure 3.13 SEM picture of CPET/1.0 wt. % AC/0.40 wt. % water foam
3.3.3 Comparison between Moisture and Wet AC
The cell morphology of CPET foams prepared by controlled hydrolysis is shown
in Fig 3.14 & 3.15. For both formulations, the cell size became more uniform, the cell
density decreased, and the averaged cell size increased with increasing water content,
particularly at the optimal condition (e.g. 0.12 wt.% moisture or 0.5 wt.% AC/0.20 wt.%
water) with the highest expansion ratio. Compared to the XPET foam at almost the same
expansion ratio, CPET foams show a more uniform cell size.
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Figure 3.14 Cell density change with increasing extent of hydrolysis
Figure 3.15 Cell size change with increasing extent of hydrolysis
The extent of the hydrolysis can be compared by both die pressure during extrusion
and the intrinsic viscosity of the foams (Figs. 3.16 & 3.17). When using moisture as the
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hydrolysis agent, the die pressure decreased from ~7.6 MPa (1100 psi) to ~ 4.2 MPa (600
psi) when the water content increased from 0.05 to 0.12 wt.%. The die pressure dropped to
~ 1.4 MPa (200 psi) when the resin contained 0.25 wt.% moisture, indicating the excessive
resin degradation and the melt viscosity became too low to be favourable for foaming.
When using wet AC as the hydrolysis agent, a different trend was observed where a much
higher die pressure (~ 6.2 MPa (900 psi)) was obtained even with a water content as high
as 0.20 wt.%. This is because the water was trapped in the AC during extrusion until the
pressure was released near the outlet of the die during foaming.
Figure 3.16 Die pressure under different water contents
However, the molecular weight of foams prepared by both moisture or wet AC
based formulations still dropped to a similar range judging from the intrinsic viscosity and
melt viscosity results. Although water in AC could inhibit hydrolysis during extrusion, the
molecular weight of the CPET/AC foam still decreased after foaming. At the lowest foam
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density (~0.15 g/cm3), the intrinsic viscosity of the CPET foams dropped from ~0.81 to
~0.52 dL/g for both formulations. The melt viscosity of the foam extrudate shown in Fig.
1(e) also reveals the same trend, i.e. a lower shear viscosity would lead to a higher
expansion ratio of the non-modified CPET resins, and the maximal expansion ratio was
reached when the resin shear viscosity was ~50 Pa•s for both formulations. When the shear
viscosity dropped to ~20 Pa•s, the foam lost its mechanical strength and could not be
shaped. This demonstrates that the controlled resin degradation is the key to achieve the
desirable foamability in PET foaming, and water/moisture acts more as a hydrolysis agent,
not a co-blowing agent as in PS foaming.
Figure 3.17 Intrinsic viscosity of CPET foams
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Figure 3.18 Shear viscosity of CPET foams
The water/moisture content needs to be tightly controlled in PET foaming as the
intrinsic viscosity would drop to ~0.3 dL/g when the moisture content reached 0.2 wt.%, a
typical moisture content in PET in ambient condition, and the molecular weight and melt
strength were too low for foaming. Even though we were able to control the moisture
content in PET during lab scale extrusion foaming, it would be much better to use the water
in AC based formulation in large scale production because the water content in AC could
remain stable for an extended time period, while the moisture content in resin kept
changing in a TGA experiment showing in Fig 3.19. Furthermore, less resin degradation
during extrusion in the CPET/AC case would allow a more stable operation condition.
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Figure 3.19 Water content change of dried resin and AC (after removal of
excessive water) under ambient condition
From the DSC thermograms, CPET foams showed much lower crystallinity (~ 10%)
than the virgin CPET resin (~36%). Even so, the crystallinity was still much higher than
that of the XPET foams (~1.6%). The CPET foams with wet AC showed a higher
crystallinity than neat PET foams with moisture. This is because micro-scale particles can
enhance the nucleation efficiency of crystallization63~66. The extent of controlled
hydrolysis did not affect the crystallinity much. However, when the molecular dropped too
much (e.g. 0.24 wt.% moisture or 1% AC/0.4 wt.% water), the foams showed a much
higher crystallinity. This is probably because the shorter chain and the wider molecular
weight distribution promoted crystallization when the molecular weight decreased
significantly 67,68.
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Figure 3.20 DSC Thermograms of PET foams
Table 3.2 Crystallization behavior of PET foams
Samples Tc (℃) ∆Hc (J/g) Tm (℃) ∆Hm (J/g) Xc %
Commercial PET foam none 0.0 243.5 6.7 5.9%
XPET foam 137.7 18.3 217.3 19.8 1.3%
Virgin CPET resin none 0.0 243.1 41.4 36.6%
CPET/0.05 moisture foam 123.7 21.5 247.7 31.2 8.6%
CPET/0.09 moisture foam 123.3 16.2 248.4 27.7 10.2%
CPET/0.12 moisture foam 121.7 20.0 250.2 27.3 6.4%
CPET/0.25 moisture foam none 0.0 250.2 31.1 27.5%
CPET/0.5 AC/0.05 water 122.7 18.6 249.1 28.3 8.6%
CPET/0.5 AC/0.13 water 118.8 18.3 248.3 34.1 14.0%
CPET/0.5 AC/0.20 water 121.7 19.9 249.9 31.3 10.1%
CPET/1.0 AC/0.40 water none 0.0 249.1 20.0 17.7%
3.3.4 Chain Extension vs. Controlled-hydrolysis
Chain extension is a kind of bottom-up strategy which is applicable to all kinds of
linear resins for improving foamability. It’s especially suitable for low IV resins that is
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almost useless for good-quality products. Also, it’s an important procedure during
mechanical recycling of PET to offset the molecular weight decrease under high
temperature melt reprocessing 69. However, it’s not a good choice for high crystalline
foams due to its damage to the crystallinity.
Linear PET resins (virgin or recycled resins) are a better choice for high crystalline
PET foams. However, it’s very challenging to be foamed without chemical modification.
The molecular weight is closely related to the foam expansion ratio for linear resins. To
achieve low-density foams, a relatively low molecular weight resin is preferred. Based on
our results (together with all the related work reported before 43, 45, 46), a IV lower than 0.8
dL/g but higher than a lower limit (to avoid severe cell collapse and poor foam quality) is
the best choice for low density PET foams. The exact value will be quantified by testing
IV in the future.
For both virgin and recycled PET resins with relatively high IV (IV > 0.8), the
controlled-hydrolysis, instead of chain extension, approach is a desirable choice for high-
crystallinity and low-density foams. We have to pay more attention to the extent of
hydrolysis to avoid decreasing the molecular weight too much.
3.4 Adding micrographite (mGr) as IAA and nucleation agent
Apart from AC, we designed another micrographite-based route to prepare IR-
absorbing foams. Because of its 2D planar structure, micrographite has high IR-absorption
efficiency. With a thickness at around 500 nm, it also can act as a gas nucleation agent to
munapulate the cell morphology. We started from the optimized formulation CPET/0.12
moisture. Compared to neat PET foam with moisture, the cell size distribution of the
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composite foam turned to be more uniform (Fig 3.21 & Fig 3.22). Also, the gas bubble
became smaller and the bubble density increased significantly due to the high efficiency of
heterogeneous nucleation (Fig 3.23 and Fig 3.24). With increasing the mGr content, the
foam density slightly increased. Similar results for nanocomposite foams were widely
reported. This can be explained by the competition between gas nucleation and bubble
growth. When the nucleation rate becomes faster, more gas bubbles nuclei are generated,
which inhibits the bubble growth in the confined space. Therefore, the bulk density of the
foam becomes higher. In our experiment, we didn’t try to add more mGr (> 0.5 wt. %).
According to our previous research, particle aggregation might happen due to the poor
dispersion under slow extrusion rate so that the gas nucleation can hardly be further
improved. Also, merely around 0.2 wt. % carbon IAA is already enough for IR absorbing
applications.
Figure 3.21 Cell morphology of CPET with 0.12 wt. % moisture /0.2 wt. % mGr foam
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Figure 3.22 Cell morphology of CPET with 0.12 wt. % moisture /0.5 wt. % mGr foam
Figure 3.23 Cell density change with increasing mGr content
Figure 3.24 Cell size change with increasing mGr content
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3.5 Mechanical and Thermal Properties of CPET Foams
3.5.1 Tensile Properties
The CPET foams prepared by controlled hydrolysis exhibited excellent mechanical
strength from the tensile test (Fig 3.25). The XPET foam showed the highest stress but less
than 20 % strain. The poor elongation ratio is probably because of the nonuniform cell
structure and large bubble size. Also, low intrinsic viscosity of the XPET resin might be
another reason. The CPET foam showed a slightly lower stress but a much better elongation
ratio than both XPET and commercial PET foams. Although the comparison between
foams with different densities may not be fair, it still demonstrates that even after a certain
extent of degradation the CPET foam quality could be decent enough. The foams prepared
by moisture-based and wet AC-based formulations show comparable mechanical
properties. This further verifies the similarity of the two approaches. To note, the wet AC-
based foam shows a lower elongation ratio but a higher stain. This is probably because of
the higher crystallinity of the foam with AC. The higher intermolecular attraction due to
the higher crystallinity limits the free motion of polymer chains, leading to a higher
stiffness (higher stress) but a lower extension ratio under the same external force.
Figure 3.25 Mechanical properties of PET foams prepared by controlled hydrolysis
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3.5.2 Thermal Stability
For the thermal and insulation property test, planar foam specimens were prepared
by welding the foam rods and cutting them into the same size (Fig 3.26). A PS foam with
the same geometry was cut from a commercial PS foam as a bench mark.
The thermal stability is compared by heating the samples from 25 to 200℃ (Fig
3.27). PS foam collapsed at <100℃ and gradually decomposed with increasing
temperatures, indicating its weakness for high temperature applications. XPET foam
softened at around 140℃, which shows comparable extreme application temperatures as
commercial PET foams . When adding micrographite, its thermal stability almost didn’t
improve. The CPET foam prepared by controlled-hydrolysis showed excellent thermal
stability even over 200℃. This is because the chain scission reaction of linear PET still
produces linear molecules and thus keeps much higher crystallinity than XPET, which
further demonstrates one of theadvantages of ourapproach over conventional chain
extension modification.
Figure 3.26 Welding extruded rods into thin sheets. From left to right: (1) Commercial PS
foam; (2) XPET foam; (3) XPET/0.2 wt. % graphite foam (4) CPET (0.12 wt. % water)/
0.2 wt. % graphite foam (5) CPET/0.5 wt. % AC/ 0.2 wt. % water foam
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Figure 3.27 Thermal stability of different foams from 25℃ to 200 ℃
3.5.3 IR-absorbing and Insulation Properties
Under the experiment settings, the real condition of IR absorbing was mimicked
successfully. This can be judged by the air temperature above the roof which was controlled
stably (within 26 to 35℃) and no hot spots existed due to the convection (Fig 3.28). Neat
PS or PET foam showed a lower roof temperature than foams with infra-red attenuation
agents (Figure 3.29). With merely less than 1 wt. % mGr or AC particles, the roof
temperature easily reached around 100℃, showing the high IR-absorbing efficiency of
carbon particles as IAA. Since most of the IR radiation was shielded by IAA in the foams,
the indoor temperature was about 10℃ lower than using neat PS or PET foams (Figure
3.30). Interestingly, the PET foam with mGr had a more stable roof and indoor temperature
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than that with AC. This is probably because mGr has a planar structure that can block and
absorb the radiation more efficiently than sphere-shaped AC which allows for more
transmission and the light scattering between particles. Therefore, more temperature
fluctuation happened.
For enhanced roofing insulation by IR-absorbing, the roof temperature can easily
reach ~100 ℃ due to the addition of IIA. Therefore, compare to PS with relatively low
thermal stability, PET is a more suitable polymer matrix for this application based on the
results we generated above.
Figure 3.28 Temperature of the air at 2 inches above the roof
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Figure 3.29 Roof upper surface temperature change using different roofing materials
Figure 3.30 Indoor temperature change using different roofing materials
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3.6 Strand Die Experiment
The optimized fomulations mentioned above were repeated on the strand die. When
the foams were extruded, several strands were welded together, forming a thin plate-
shaped sample (Fig 3.31). Almost the same foaming condition to the capillary die was
obtained. This demonstrates the logic of our die design which is applicable to a pilot-
scale extrusion foaming equipment.
Figure 3.31 Foam samples prepared by strand die
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Chapter 4. Conclusion and Future Work
A controlled-hydrolysis approach was developed to prepare the low-density and
high-crystallinity PET foams. The water content and two types of hydrolysis agent
(moisture and AC) were investigated to optimize and balance between the foam density,
extent of hydrolysis and cell morphology. Compared to conventional chain extension or
branch resin modification, controlled-hydrolysis may result in linear polymer chains and
thus high crystallinity. Due to the high crystallinity and acceptable molecular weight even
after degradation, the CPET foams show excellent mechanical strength and thermal
stability (>200℃). As an infrared attenuation agent, micrographite (mGr) further improves
the cell morphology. The CPET foam with mGr or AC shows excellent insulation
properties under IR radiation. With high thermal stability (stable even higher than 200℃),
CPET foam is more desirable than PS for high temperature applications (>100℃) such as
future IR-absorbing roofing and external wall applications.
Our future work will include the following:
• Further investigation on why liner PET of lower molecular weight is more
advantageous for low-density foams
• Strand die optimization and lab-scale production line build-up
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Appendix A. Experimental Design
Table A.1 Neat PET foams
Sample Density Crystallinity Molecular weight
Crystalline PET (CPET)
Crosslink PET (XPET)
Commercial PET foam
Table A.2 Foaming CPET resins with moisture
Sample Water content Density Molecular weight Crystallinity
Virgen PET resin (E60A+)
PET (dried 24 h at 120℃) foam
PET (dried 2 h at 120℃) foam
PET (dried 1 h at 120℃) foam
PET (not dried) foam
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Table A.3 CPET/AC with water foams
Sample Water content Density Molecular weight Crystallinity
CPET/0.2% AC with moisture
CPET/0.5% AC with moisture
CPET/1.0% AC with moisture
CPET/0.2% wet AC
CPET/0.5% wet AC
CPET/1.0% wet AC
CPET/0.2% wet AC (Dried for 5 min at 100 ℃)
CPET/0.5% wet AC (Dried for 5 min at 100 ℃)
CPET/1.0% wet AC (Dried for 5 min at 100 ℃)
Table A.4 Using mGr as IAA and to further manipulate the foams morphology
Sample Density
CPET/0.5% wet AC/0.1% mGr
CPET/0.5% wet AC/0.2% mGr
CPET/0.5% wet AC/0.5% mGr
CPET (0.12 wt. % water)/ 0.1% mGr
CPET (0.12 wt. % water)/ 0.2% mGr
CPET (0.12 wt. % water)/ 0.5% mGr
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Appendix B. Optimization of Foaming Conditions
Table B.1 Optimized processing condition of neat CPET foaming
Extruder zone temperature (℃)
Z1 Z2 Z3
Z4
PBA
Injection
Z5 Z6 Z7 Z8 Z9
die
Z10 Z11
230 250 260 260 260 260 250 245 245 245 245
Screw Speed (rpm) Torque (%) PDie
(PSI) PPBA
(PSI) FluxPBA
(mL/min)
15 10-30 1000~1100 900-1000 2.0
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Table B.2 Optimized processing condition of XPET foaming
Extruder zone temperature (℃)
Z1 Z2 Z3
Z4
PBA
Injection
Z5 Z6 Z7 Z8 Z9
die
Z10 Z11
200 220 235 235 235 235 230 225 225 220 215
Screw Speed (rpm) Torque (%) PDie
(psi) PPBA
(psi) FluxPBA
(mL/min)
10-30 <10 1200-1500 1000-1200 1.5-4.0
Table B.3 Optimized processing condition of foaming CPET with moisture
Extruder zone temperature (℃)
Z1 Z2 Z3
Z4
PBA
Injection
Z5 Z6 Z7 Z8 Z9
die
Z10 Z11
230 250 260 260 260 260 250 245 245 245 245
Screw Speed (rpm) Torque (%) PDie
(psi) PPBA
(psi) FluxPBA
(mL/min)
15 10-20
200-800
(depending on
water content)
200-600
(depending on
water content)
2.0
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Table B.4 Optimized processing condition of foaming CPET using AC as water carrier
Extruder zone temperature (℃)
Z1 Z2 Z3
Z4
PBA
Injection
Z5 Z6 Z7 Z8 Z9
die
Z10 Z11
230 250 260 260 260 260 255 245 245 245 245
Screw Speed (rpm) Torque (%) PDie
(psi) PPBA
(psi) FluxPBA
(mL/min)
15 20~30
600-1000
(depending on
water content)
500-800
(depending on
water content)
2.0
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Appendix C. Water Content Measurement
Figure C.1 TGA and water content of wet activated carbon put in the atmosphere after
water filtration (wet AC = dried for around 20 hours in this thesis)
Figure C.2 TGA and water content of different types of activated carbon
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Figure C.3 Water content of neat CPET resin with moisture (measured by HR83 Halogen
Mettler Toledo and data points collected manually)
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Appendix D. Shear Viscosity of CPET and XPET Resins
Figure D.1 Shear viscosity of CPET and XPET Resins
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Appendix E. Cell Morphology of Dry CPET/Carbon Particles Foam (less than 0.05
wt. % water)
Figure E.1 SEM picture of CPET/0.2 wt. % mGr (both dried) foam
Figure E.2 SEM picture of CPET/0.5 wt. % CNT (both dried) foam
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Appendix F. Crystallinity Calculation from DSC Thermograms
Figure F.1 DSC thermograms of Commercial PET foam
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Figure F.2 DSC thermograms of Crosslink PET (XPET) foam
Figure F.3 DSC thermograms of Virgin CPET resin
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Figure F.4 DSC thermograms of Neat CPET foam (moisture content ~ 0.05 wt. %)
Figure F.5 DSC thermograms of Neat CPET foam (moisture content ~ 0.09 wt. %)
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Figure F.6 DSC thermograms of Neat CPET foam (moisture content ~ 0.12 wt. %)
Figure F.7 DSC thermograms of Neat CPET foam (moisture content ~ 0.25 wt. %)
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Figure F.8 DSC thermograms of CPET/0.5 wt. % AC /0.05 wt. % water foam
Figure F.9 DSC thermograms of PET/0.5 wt. % AC/0.13 wt. % water foam
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Figure F.10 DSC thermograms of PET/0.5 wt. % AC/0.20 wt. % water foam