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University Of Toronto Mechanical & Industrial Engineering Department
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Processing and Characterization of
Autoclave-based EPP Beads
…………………………………………………
ABHISHEK PATEL
MUHAMMAD KASHIF FAROOQUI
…………………………………………………..
M.Eng. PROJECT REPORT
DEPARTMENT OF MECHANICAL AND INDUSTRIAL
ENGINEERING
UNIVERSITY OF TORONTO
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© Copyright by Abhishek Patel & Muhammad Kashif Farooqui (2010)
ACKNOWLEDGEMENTS
We would like to express our earnest gratitude to Dr. Chul Park for his leadership,
support and cooperative advice throughout the tenure of this project. This project
would not have been successfully completed without his guidance.
A big thank you to all members of Microcellular Plastics Manufacturing Laboratory
group: Nemat Hossieny for his advice and support in our experiments, Yanting Guo
and Dr. Wenli Zhu for their recommendations towards this project and assistance in
form of managing the DSC experiments, Anson Wong and Raymond Chu for their
constant inputs and guidance regarding the experimental setups.
Special note of appreciation to Ryan Mendell and all the machine shop crew for their
patience and tremendous help in assisting us with the setup in the shortest time
possible.
We also extend our gratitude to the Department of Mechanical and Industrial
Engineering, University of Toronto, Donna Liu and Brenda Fung for their aid in the
successful completion of our M.Eng program.
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Table of Contents
1.1 E.P.P 4
1.2 History of E.P.P 6
1.3 Properties of EPP Plastic Foaming 6
1.4 EPP Manufacturing Process 9
2.1 Objective of Study 12
2.2 Thermoplastic Foaming 13
2.3 EPP Pre-Expansion 13
2.4 Double Peak Mechanism 14
3.1 Solubility Analysis via PVT 18
3.2 PVT Relationship 18
3.3 PVT Experimental Design 19
3.4 PVT Experimental Results and Discussion 21
4.1 Solubility Analysis via MSB 23
4.2 MSB Experimental Apparatus and Procedure 24
4.3 MSB Experimental Results and Discussions 26
5.1 Autoclave Apparatus Setup 28
5.2 Procedure 30
5.3 Initial Results and Discussions 32
5.4 2nd Generation Chamber 35
5.5 Chamber and Propeller Modification 36
6 References 39
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CHAPTER 1
INTRODUCTION
1.1 E.P.P (EXPANDED POLYPROPYLENE)
Expanded polypropylene (EPP) is an engineered plastic foam material, highly
versatile closed-cell bead foam that provides a unique range of properties, including
outstanding energy absorption, multiple impact resistance, thermal insulation,
buoyancy, water and chemical resistance, exceptionally high strength to weight ratio
and 100% recyclability. [1]
1.2 HISTORY OF EPP
EPP was first developed in the 1970's by JSP, as a result of research into new
forms of polypropylene. The material's first applications were for automotive
products in Japan in 1982. Demand for EPP has since increased dramatically in
all regions of the world based partly on the need of auto makers to improve
energy management functions whilst reducing weight and improving
environmental benefits. The first automotive application for EPP was for an
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energy absorbing component in a bumper system. EPP is now widely utilized for
numerous other automotive parts and systems, including seating and other
interior components. [1]
Polypropylene resin is now increasingly utilized in various fields because of excellent
mechanical strengths, heat resistance, machinability, cost balance, combustibility
and recyclability thereof. Foamed, non-cross linked resin moldings of abase resin
including a polypropylene resin (hereinafter referred to simply as "PP"), which retain
the above excellent properties and which have exceptional additional characteristics
such as cushioning property and heat resistance are thus utilized for various
applications as packaging materials, construction materials, heat insulation materials
etc.
Recently, there is an increasing demand for PP moldings having higher rigidity and
lighter weight than the conventional ones. For example, in the field of vehicles such
as automobiles, PP moldings have been used in various parts such as bumper
cores, door pats, pillars, tool boxes and floor mats. In view of protection of
environment and saving of energy, light weight and high rigidity PP moldings
retaining excellent cushioning and shock absorbing properties are desired. In the
field of containers and boxes for storing and transporting foods such as fish, molded
polystyrene foams have been hitherto used. Because of inferior shock and heat
resistance, however, molded polystyrene foams are not suitably reused. Therefore,
the need for light weight and high rigidity PP moldings are also increasing in this
field. [2]
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1.3 PROPERTIES OF EPP PLASTIC FOAMS
• Lightweight with very high strength to weight ratio
• Withstands multiple impacts without significant damage
• Highly durable
• Resistant to water, chemicals and most oils
• Resistant to temperature extremes from -35°C (-31°F) up to 130°C
(265°F)
• 100% recyclable with environmental benefits [3]
• EPP is approved for use in conjunction with food products. Its thermal
insulation properties and structural strength make it appropriate for
containers such as food delivery containers and beverage coolers and the
like. EPP does not support microbial growth and can be made sterile with
steam cleaning. [10]
1.3.1 Unique performance characteristics
• Porous EPP is comprised of cylinder-shaped polypropylene beads, which
adds air space between the beads in the final molded form, which
enhances beneficial acoustical insulating effects and reduces weight.
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• EPP is commonly colored black for automotive applications, though is
often found in white for packaging products. EPP is available from some
suppliers in vibrant colours suitable for presentation-grade textured
surface. [10]
1.3.2 EPP Properties
Physical Properties
EPP density range, from 20 g/l through 200 g/l
Tensile strength (kPa) 270 to 1930
Tensile elongation (%) 21 to 7.5
Compressive strength (kPa)
25% strain 80 to 2000
50% strain 150 to 3000
75% strain 350 to 9300
Compression set (%)
25% strain, 22H, 23°C 13.5 to 10.5
Burning rate (mm / min) 100 to 12 [10]
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1.3.3 Applications
EPP is widely utilized by automotive manufacturers because of its performance
benefits for energy management, lightweight, enhanced functionality, durability
and recyclability. Applications include seating, bumpers, stowage systems, door
panels, pillars, floor levelers, parcel shelves, head rests, tool kits, sun visors and
myriad filler parts.
Reusable industrial packaging, known as dunnage, is frequently made from EPP
due to its durability and its inherent ability to absorb energy in transit. EPP is
used increasingly in furniture, toys such as model aircraft and other consumer
products due to its versatility as a structural material and its light weight, as well
as other performance characteristics.
EPP is approved for use in conjunction with food products. Its thermal insulation
properties and structural strength make it appropriate for containers such as food
delivery containers and beverage coolers and the like. EPP does not support
microbial growth and can be made sterile with steam cleaning. [10]
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1.4 EPP MANUFACTURING PROCESS
The manufacturing process is complex, requiring both technical expertise and
specialized custom equipment. Polypropylene resin is combined with other
ingredients in a multi-step proprietary process. Under tightly controlled
conditions, extruded pellets expand to become consistently shaped beads of
expanded polypropylene foam. Other specialized manufacturing techniques may
be employed to produce variations in the final product form.
EPP foam beads are then injected into molds. In many cases, cost-effective
multi-cavity aluminum molds are used. Pressure and steam heat fuse the beads
into a finished shape. The finished EPP foam part becomes a key component in
sub-assemblies incorporated in the original equipment manufacturer’s product.
[1]
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Fig. 1 Generic Overview of EPP Manufacturing Process [1]
The processing of all beaded foam resins generally involves two primary stages;
pre-expansion and steam chest moulding.
1.4.1 Pre-Expansion
In the pre-expansion stage raw beads containing a blowing agent are exposed to
a heat source, usually steam, causing the beads to increase by up to 50 times
their original size.
1.4.2 Moulding
The steam chest moulding stage begins when the pre-expanded beads are
injected into a mould. In the steam chest molding process, steam (water
vapor) is used as both a heating medium and a blowing agent in polymer foam
processing. The molding process consists of a series of operations:
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steaming, depressurizing, cooling, and ejection[Ref]. The steaming process
softens and fuses the polymeric beads, and the steam penetrates and
condenses in the polymeric bead foams. When depressurized, the water
condensed in the cells begins to gasify and expand the foams. With
subsequent water cooling, the interfaces of the beads solidify, and
efficient bonding between the beads occurs. The two important advantages of
steam chest molding are (1) good temperature uniformity throughout the
samples due to the use of steam as a heating medium for foaming, and (2)
three-dimensional (3D) shaping ability. The above advantages may be
beneficial in shaping fairly large parts with a 3D shape. The cycle time of
this final moulding stage is dependent on the mould configuration, part
density and the type of resin. In certain designs, this process allows to
mould around inserts placed within the tool. This allows for the manufacture
of ready-to-use components or for packaging and materials handling products
to be used as part of a system.
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CHAPTER 2
2.1 OBJECTIVE OF THE STUDY
2.1.1 Current State
Current market practice of EPP production and molding imposes excessive
transportation cost to bead purchasers (bead molders) because molders are
purchasing expanded foam beads, light weight with huge volume. In an attempt
to ease the burden that bead molders bear, a new EPP production method that
enables an alternative EPP manufacturing practice is suggested.
The research scope includes:
• Extensive experiments on the relationship between expansion ratio of
PP beads and various content of BA, foaming temperature and pressure.
• Understanding of mechanism of the double melting peaks' formation
during EPP manufacturing process.
• Solubility and diffusivity measurements of various content of BA
(Blowing Agent), temperature and pressure in the system of
polypropylene/water. [6]
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2.2 THERMOPLASTIC FOAMING
Foaming of thermoplastic is gaining interest because of its potential to decrease
the weight of automotive parts and its superior mechanical and acoustic
properties for packaging as well as building materials. Thermoplastic foamed
products can be distinguished from their unfoamed counterparts by virtue of their
cellular structure. A typical foaming process has three stages: (1) polymer/gas
solution formation, (2) cell nucleation, and (3) cell growth and stabilization. The
polymer/gas solution formation is achieved by saturating a polymer with high-
pressure gas, typically above its melting temperature. The solution formation is
governed by gas diffusion in the polymer matrix. Cell nucleation occurs when
thermodynamic instability is introduced in the polymer/gas solution system
through a rapid change in the gas solubility. After cell nucleation, the gas from
the polymer matrix diffuses into the cells promoting cell growth. The cells grow
and reduce the total polymer density as the gas molecules diffuse into the
nucleated cells from the polymer matrix. Cell growth is primarily controlled by the
time allowed for the cells to grow, the temperature of the system, the states of
the supersaturation, the hydrostatic pressure of stress applied to the polymer
matrix and the viscoelastic properties of the polymer/gas solutions [5].
2.3 EPP PRE-EXPANSION
Expanded polypropylene resin beads are generally obtained by the dispersion
method in which the resin particles are dispersed in a dispersing medium, such
as water, in an autoclave together with a physical blowing agent and heated
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under a pressure to a temperature higher than the softening point of the resin
particles to impregnate the resin particles with the blowing agent. The resulting
dispersion is discharged from a bottom portion of the autoclave into a lower
pressure atmosphere while maintaining the pressure within the autoclave at a
pressure higher than the vapor pressure of the blowing agent, so that the resin
particles are foamed and expanded to obtain the expanded beads. Because of
the surface tension of the dispersing medium acted on the softened resin
particles during the impregnation thereof with the blowing agent, the resin
particles are smoothed and rounded. Therefore, the expanded beads obtained
from such rounded resin particles are generally round in shape. The diameter of
the through holes of the resin particles generally increases as a result of the
expansion and foaming. Thus, the expanded beads generally have a greater
diameter than their raw material resin particles.
The blowing agent used in the dispersion method may be an organic physical
blowing agent such as an aliphatic hydrocarbon, e.g. propane, butane etc. or an
inorganic physical blowing agent such as nitrogen, carbon dioxide, argon or air.
From the standpoint of costs and environmental problem, the use of an inorganic
blowing agent, particularly nitrogen, air or carbon dioxide is preferred. [?]
2.4 DOUBLE PEAK MECHANISMS
A common way of promoting good bead fusion is to develop two melting peaks in
the bead materials [7], [8]. When the steam temperature is chosen between the
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two melting peaks, the higher temperature peak will maintain the expanded
shape of the beads, while the lower-temperature melting peak contributes to the
sintering of the beads. An alternative way to promote good bead fusion is to
generate one broad melting peak, but it is not as good as having two peaks.
Even with two peaks, providing a constant steam temperature is not easy
because heat transfer takes place when steam enters the mold. Therefore, two
distinct melting peaks with a wide temperature difference are needed for
expanded bead foam processing.
Fig. 2 Typical DSC Curve for EPP Bead [9]
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2.4.1 Material Used:
A random PP co-polymer (SEP-550) from Honam Petrochemicals was selected
as the material primarily because of its wide application capability and physical
properties.
Applications: Foam beads for energy absorption systems (bumper core)
Attributes: Good heat welding property, High impact resistance
Datasheet for SEP-550 [11]
Properties Test
Method Units Properties
Melt Flow Rate 230℃, 2.16kg D-1238 g/10min 7.5
Density D-1505 g/㎠ 0.9
Mold Shrinkage HPC
Method % -
Tensile Strength at Break D-638 kg/㎠ 255
Ultimate Elongation D-638 % 500 <
Flexural Modulus of Elasticity D-790 kg/㎠ 9,500
Hardness D-648 R -
IZOD Impact Strength 23℃ HPC
Method kg.cm/cm 11
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IZOD Impact Strength -10℃ HPC
Method kg.cm/cm -
DU-POINT Impact Strength 23℃
HPC Method kg/㎝ -
DU-POINT Impact Strength -10℃
HPC Method kg/㎝ -
Softening Point D-1525 ℃ 129
Weatherability W-O-M Hour -
Heat Resistance 130℃ Air Oven Hour -
Heat Distortion 4.6kg/㎠ D-648 ℃ -
HAZE(2mm) D-748 % -
Flammability UL
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CHAPTER 3
3.1 SOLUBILITY ANALYSIS via PVT
3.1.1 Determination Of CO2 Solubility in EPP & Water
The initial step was to attempt to determine the amount of solubility of CO2
in the material dispersed in water. There have been numerous experiments
conducted and sufficient data available to gauge the amount of carbon
dioxide soluble in EPP at various pressure-temperature combinations.
There though is not adequate experimental data to support how the
addition of water to the equation impacts the solubility of the gas in the
polymer.
Any liquid in which the resin particles are insoluble may be used as the
dispersing medium. Examples of the dispersing medium include water,
ethylene glycol, glycerin, methanol, ethanol and mixtures thereof. The
dispersing medium is preferably water or an aqueous dispersing medium.
Primary reason for selecting water was due to the known fact that water
acts as an economic dispersion medium for polymer autoclaving
processes. Expanded polypropylene resin beads are generally obtained by
a dispersion method which includes dispersing particles (or pellets) of a
polypropylene resin in water in an autoclave and impregnating the
polypropylene resin particles with a blowing agent at a temperature higher
than the softening point of the resin under pressurized conditions. The
dispersion is then discharged from the autoclave to the atmosphere so that
the resin particles are foamed and expanded [27].
3.2 PVT RELATIONSHIP (PP & Carbon Dioxide)
In polymer/gas solution system, when gas dissolves into a molten polymer,
the polymer swells (or dilates) due to gas sorption. The amount of polymer
swelling or dilation is characterized by its PVT properties, which can be
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obtained by measuring the equilibrium state volume of a polymer/gas
solution at any specific temperature and pressure. In polymer foaming
applications, cell nucleation and growth are governed by physical
properties such as solubility [12, 13], diffusivity [14] and surface tension
[15–17]. However, the determination of these properties relies on the PVT
data (i.e.), the polymer swelling caused by gas dissolution. For example,
currently, the most commonly used technique for gas solubility
measurement in polymer melts is the use of a magnetic suspension
balance system [18–21], in which the accurate determination of gas
solubility depends on the buoyancy correction of the equilibrium
polymer/gas solution volume, i.e., the swelling of the polymer due to the
dissolved gas. Therefore, knowing their PVT properties (the polymer
swelling by dissolved gas) is critical for understanding and controlling foam
processing
3.3 PVT EXPERIMENTAL DESIGN
3.3.1 PVT system
The overall system has two major functional traits (viz.) the software attribute and
the hardware attribute. The software attribute comprises of an integration of
modules with each function module implemented to perform individual tasks. The
individual tasks are as follows: image capture, image reconstruction, and volume
integration. The hardware attribute is the actual constructed and assembled
apparatus through which the function modules work. Fig. 5 shows a schematic of
the overall PVT system. Those two major functional attributes are integrated to
construct the complete apparatus. The software algorithm such as the camera
movement and image capture, etc. were developed and implemented in the
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actual system to facilitate the functions such as stage movement and camera
triggering for image capturing, etc. through the apparatus. [5]
Fig. 5 PVT System/Experimental Setup [5]
3.3.2. PVT Experimental setup
The experimental apparatus consists of the following components: a high-
pressure chamber with a sapphire visualization Y.G. Li et al. / Fluid Phase
Equilibria 270 (2008); a 2024×2024 resolution JAI Pulnix TM4100 CL camera
with a control software (Easy Grab); Schneider 4/80 lens and extension tubes; a
temperature controller (Omega CN132) with thermocouple (Omega RTD); four
cartridge heaters; an automatic high-precision XY stage with Galil motion
controller and control board; a manual 1 in. XYZ stage to adjust the position of
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the light source; a syringe pump connected to the gas tank; and a backlight
source with a light equalizer/diffuser [5]
3.4 PVT EXPERIMENTAL RESULTS AND DISCUSSIONS
3.4.1 PVT Behaviors for PP/CO2 & Water System
The current system setup for the PVT system in MPML Laboratory did not
adequately support the experimental conditions of attempting to determine
solubility of CO2 in EPP in an aqueous based medium. The PVT system was
used to predict the amount of gas solubility in the autoclave wherein the EPP
beads are suspended in water. Though water is primarily used as a dispersion
medium in the process of bead expansion it certainly affects the amount of CO2
that would dissolve in the EPP beads during saturation. Further experiments
need to be conducted with modified experimental setup to allow the water to
remain stable and aid determines the gas solubility in EPP. The scope of these
experiments exceeds the current project scope and has been dedicated as a part
of future work.
3.4.2 PVT Behaviors for PP/CO2 Only System
Under experimental conditions wherein the EPP beads are subjected to
saturation via Gas (CO2) only, under high pressure and temperature, sufficient
previous experimental data has been collected to help determine the solubility of
gas in polymer. When a polymer melt is exposed to a high pressure gas, the
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dissolved gas under high pressure will cause the polymer to swell and increase
the specific volume. This means that the presence of gas evidently enhances the
overall activity of the polymer/gas system, and thus, creates more free volume for
the CO2 molecule to penetrate into the polymer matrix after the gas fills the
existing free volume. Therefore, the specific volume will be increased under a
high pressure gas. The increased free volume causes an increase in solubility
and diffusivity [22]. The dissolved CO2 causes a plasticization effect to reduce
the viscosity of the polymer/gas mixtures and increases the chain mobility [23].
This increased specific volume also decreases the surface tension of polymer
[24]. In summary, despite the hydraulic compression effect, the dissolved gas
increases the specific volume and thereby, affects the solubility, diffusivity,
viscosity and surface tension. All these fundamental factors are decisive in
determining the foaming behavior of a polymer and hence determining the
solubility and the swelling caused by gas dissolution is of utmost importance,
since it governs all of these parameters.
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CHAPTER 4
4.1 SOLUBILITY ANALYSIS via MAGNETIC SUSPENSION BALANCE
Inconclusive PVT Experimental results for determination of CO2 solubility in EPP
suspended in an aqueous medium propagated the need to use a different
experimental medium to determine the same. Magnetic Suspension Balances
(MSB) is able to perform kinetic and equilibrium measurements and solubility
data (e.g. absorption and adsorption isotherms) can be examined gravimetrically
with high accuracy [25].
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4.2 MSB EXPERIMENTAL APPARATUS AND PROCEDURE
A schematic of the MSB is shown in Fig. 6
Fig. 6 Magnetic Suspension Balance [25]
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The MSB consists of a sorption chamber that is used to expose the sample to
gas at elevated temperatures and pressures, and a microbalance, which is
isolated from the sample and exists at ambient conditions. An electromagnet
connected to the microbalance is adjusted so that a permanent magnet
connected to a rod–rod–basket assembly and located within the sorption
chamber is kept in suspension. Thus, the microbalance measures a weight that
is proportional to the electromagnetic force, which keeps the rod–rod–basket
assembly in suspension [25].
In a typical experiment, the polymer is placed in a sample basket as powder or is
directly attached as a film (i.e., PSF) to the hook of the rod–rod assembly. After
closing the sorption chamber the polymer is degassed by evacuating the sorption
chamber at 10−2 Torr until the weight measured by the microbalance remains
unchanged over time. A heating circulator is used to control the temperature of
the chamber, which is measured with a calibrated platinum resistance
thermometer to an accuracy of ± 0.5 °C. The sample weight, read from the
microbalance under vacuum and at temperature T, is recorded as ws(vac,T).[25]
The electromagnetic force measured by the microbalance increases to keep the
rod–rod–basket assembly in suspension. In this manner, the mass of the gas
absorbed by the polymer is measured directly by monitoring the increase of the
electromagnetic force. Eventually, the equilibrium sorption (the solubility) is
reached and the weight of the sample stops increasing. At this final saturation
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stage, the weight reading from the microbalance at pressure P and temperature
T is recorded as ws (P, T).
The mass of the gas dissolved in the polymer, wfl (P, T) is calculated using the
following equation:
wfl(P,T)=ws(P,T)−ws(vac,T)+ρfl(P,T)(Vr–b+Vp+Vsw) [25]
where ρfl(P,T) is the density of the gas at P and T, Vr–b and Vp the volumes of the
rod–basket assembly and of the original polymer, respectively, and Vsw is the
volume change of the original polymer due to swelling. The last term of the above
equation, ρfl(P,T)(Vr–b + Vp + Vsw), represents the buoyancy force caused by the
compressed gas, which lifts the rod–rod–basket assembly and thus decreases
the electromagnetic force necessary to keep the rod–rod–basket assembly in
suspension [25]. The density of CO2, ρfl(P,T) is calculated from the Bender EoS
[26], which is accurate for the purposes of this work.
4.3 MSB EXPERIMENTAL RESULTS AND DISCUSSIONS
Multiple experiments were conducted at different pressure and temperature sets
for pre-weighed EPP beads dispersed in water. The aim was to attain
experimental data to support claims for determining an optimum pressure-
temperature combination wherein peak solubility of CO2 could be achieved in
EPP beads dispersed in water.
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Similar results to PVT were attained for solubility data of CO2 in EPP beads
dispersed in water. Lack of apparatus capability to retain water during the
saturation phase was a major deterrent for the inconclusive results. The
conclusion in short though was that once again the apparatus needed to be
modified to adapt to the experimental set of conditions required. These
modifications exceeded the current project scope and have been delegated as
part of future work.
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CHAPTER 5
5.1 AUTOCLAVE APPRATUS SETUP:
A pre-designed autoclave was initially selected as the pressure chamber for bead
expansion. Additional features like pressure gauge (Range: 0 – 1000 psi) and
four 250 W cartridge heaters from McMaster Carr (machined and embedded into
the chamber along the periphery) were added for experimentation. A side
discharge valve from Swagelok was appended to provide rapid discharge of gas
after saturation and provide conditions for bead expansion and foaming. A safety
feature in the form of an 8” x 8” x 11” plexiglass cuboid with a 1” Diameter orifice
was affixed at the end of the valve outlet for secure release of steam-gas mixture
from the chamber. An additional cylindrical Stainless Steel (SS-316) vessel was
machined in the UofT Machine Shop to create a medium for holding water and
EPP bead mixture.
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Fig. 3 Initial Chamber With Side Discharge Valve
A temperature controller unit was designed with an 8-pin SS (Solid State) relay,
20 Amp General purpose fuse and micro-controller (from Love Controls) to
provide a closed loop feedback system for temperature control. The circuit
diagram for the controller was illustrated below:
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Fig. 4 Temperature Controller Circuit Diagram
5.2 PROCEDURE
The expanded beads are prepared from resin particles by the dispersion method
in which the resin particles are dispersed in a dispersing medium, such as water,
in an autoclave together with a physical blowing agent and heated under a
pressure to a temperature higher than the softening point of the resin particles to
impregnate the resin particles with the blowing agent. The resulting dispersion is
discharged from a the autoclave into a lower pressure atmosphere while
maintaining the pressure within the autoclave at a pressure higher than the vapor
pressure of the blowing agent, so that the resin particles are foamed and
L N
L
L
N
Relay
Controller
Fuse
N L Heater
AC Supply
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expanded to obtain the expanded beads. Because of the surface tension of the
dispersing medium acting on the softened resin particles during the impregnation
with the blowing agent, the resin particles are smooth and rounded. The diameter
of the resin particles increases as a result of the gas absorption and the
expanded bead attain a greater diameter than their raw material resin particles
[27].
Various experiments were conducted at different temperatures and various
saturation times. 50 Grams of unexpanded particles formed of the SEP-550
polymer were charged into an autoclave and was mixed with 500 ml of water to
form dispersion. The dispersion was heated to foaming temperature of 150 C. A
blowing agent (carbon dioxide) was then fed to the autoclave until the pressure
within the autoclave had the value of 600 psi and the dispersion was maintained
at that condition for 60 min. Then the autoclave was opened to discharge the gas
and the dispersion was recovered after opening the autoclave. The same set of
experiment was conducted albeit with the saturation time now at 120 min. Similar
experiments were conducted for another a couple of temperature – saturation
time combinations (viz.) 155 C and 160 C, both @ 60 mins and 120 mins.
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5.3 INITIAL RESULTS AND DISCUSSIONS
Fig. 4 Results from initial experiments
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Initial experimental data was directed towards attaining an optimum temperature
– saturation time blend to enable maximum expansion ratio for the polymeric
material. All initial observations consisted of low to negligible expansion ratios
and involved substantial agglomeration of the beads.
The conjoint beads made it very arduous to estimate the exact expansion of each
individual pellet. The following possibilities were researched and looked into in an
attempt to resolve the agglomeration issue:
� Pre-coating the beads before the foaming
� Setting a stirrer in the chamber.
• Adding a suspension stabilizer to the dispersion with the following ratios:
o Water: 220 parts
o PP pellets: 100 parts
o Suspension stabilizer: 0.2 parts (ex. Sodium dodecylbezene
suffocate, aluminum sulfate
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The addition of suspension stabilizer was determined to be the most economic
and likely possible alternative as the pre-coating of beads was not only
expensive but also could impact the gas absorption capabilities of the polymer
bead. The addition of stirrer would involve a complete re-design of the entire
autoclave chamber and involve additional financial costs.
.
Fig. 6 2nd generation of Chamber setup
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Fig. 7 2nd generation of Chamber
5.4 2nd GENERATION CHAMBER RESULTS AND DISCUSSIONS
A new chamber was designed with bottom discharge option for both gas and
liquid together with the pallets. After conducting some test experiments with the
same conditions previously used except adding the stirring with the help of a
100RPM motor, the following observations have been noted.
Molten Pellets Stuck Inside Chamber
• Low Stirring RPM – Not enough force to eject polymer beads out of the
chamber
• Insufficient discharge port Diameter
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• Temperature is too high
Some simulation experiments were performed using a glass beaker of same size
of chamber and magnetic stirrers of different diameters and lengths to observe
the effect of increased speed of stirring, a better vortex was formed which was
required in order to provide enough force to push the beads out of the chamber.
Results showed that stirring speed and structure of the stirrer have significant
effects on the water vortex
5.5 CHAMBER AND PROPELLER MODIFICATIONS
New propeller was designed in order to get enough vortex to push the beads out.
Different propellers were tested and a 3 fin 2.5” diameter propeller was acquired
for future experiment. The previous rotary seal failed as we raised the stirring
speed to above 100rpm
New rotary seals were purchased which can be operated under the following
conditions
• Pressure = 2000 psi (max)
• Speed = 1500 – 1750 rpm
• Temperature = 200 C
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This requires increase of hardness of the shaft (55-65Rc) and with 8-12 mils
plunge-ground finished and a retainer ring to hold the seal in place will be
applied.
Fig. 8 Modification of shaft of propeller
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Fig. 9 Modification to the propeller
Fig. 10 New high speed motor
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