polymer processing module 3b. module 3b spring 20012isat 430 dr. ken lewis introduction processing...
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Polymer Processing
Module 3b
Spring 2001 2ISAT 430 Dr. Ken Lewis Module 3B
Introduction
Processing Methods and Operations Choice is dictated by the product desired and
the quantity desired.» Fiber, film, sheet, tube» Cup, bucket, car bumper, chair.
Fiber manufacture is different, it is continuous. Large quantities usually use extrusion or
injection molding Smaller quantities use compression molding or
transfer molding
Spring 2001 3ISAT 430 Dr. Ken Lewis Module 3B
Extrusion
This process is fundamental to both metals and ceramics as well as polymers.
Definition Extrusion is a compression process
» Material is forced to flow through a die orifice» Cross-sectional shape determined by the shape of
the orifice» Product is long and continuous
Spring 2001 4ISAT 430 Dr. Ken Lewis Module 3B
Extrusion2
Rarely used for thermosetting polymers
Products» Tubing, pipes, and hose» Window and door moldings» Sheet and film» Continuous filaments (as we saw in module 3A)» Coated electrical wire and cable.
Spring 2001 5ISAT 430 Dr. Ken Lewis Module 3B
Extrusion3
The extruder consists basically of a hopper and a barrel and a screw.
Spring 2001 6ISAT 430 Dr. Ken Lewis Module 3B
Extruder
The die is not part of the extruder
Usually ~ 1 – 6 in. dia.
Up to 60 rpm
Flight clearance of only 0.002 in.
Spring 2001 7ISAT 430 Dr. Ken Lewis Module 3B
Extruder
Feed section Compact to a solid mass Pre heat
Compression or plastication section Melting progresses, degassing
occurs Metering section
Internal heating from viscous flow
Pressure is developed to extrude the material through the die
Spring 2001 8ISAT 430 Dr. Ken Lewis Module 3B
Extruder2
The screw is a tight fit in the barrel.
Note how the channel depth. changes in the plastication
section. Is constant in the metering
section.
Channel depth
These section lengths will change depending on the polymer being processed.
Compression section Short for materials that melt
suddenly (nylon) Long for gradually softening
materials (polyvinyl chloride)
Spring 2001 9ISAT 430 Dr. Ken Lewis Module 3B
Channel depth
Pressure applied to polymer melt is a function of the channel depth, dc. Feed section dc is relatively large
» Allows lots of granular polymer to be added to barrel
Compression section dc gets smaller» Applies additional pressure to metering section
Metering section dc is smallest
Can be carefully designed, but… In general, industry uses general kind of “off the
shelf” extruders.
Spring 2001 10ISAT 430 Dr. Ken Lewis Module 3B
Screw details
Helical flights with space between them Carries the polymer. Flight land is hardened
and barely clears the barrel.
The Pitch (distance the flight travels in one complete rotation) is usually about equal to the diameter.
pitchtan
DA
Spring 2001 11ISAT 430 Dr. Ken Lewis Module 3B
Melt Flow in the Extruder
OK, the screw turns, the flights advance, WHY DOES THE POLYMER ADVANCE?
Why doesn’t it just slip and slide back?
DRAG FLOW Friction between the fluid and the two
opposing surfaces» The stationary barrel» The moving channel of the turning screw» RECALL…
xv y
Y
x
zy
0v
Spring 2001 12ISAT 430 Dr. Ken Lewis Module 3B
Melt Flow in the Extruder Qdr, the volumetric drag flow rate.
If we assume that the velocity v is ½ the flight velocity (the moving plate velocity)
xv y
Y
x
zy
0v
0.5drQ vwd
•Where:
•v = velocity of the plate (m/s)
•D = distance between the plates (m)
•W = width of the plates(m)
Spring 2001 13ISAT 430 Dr. Ken Lewis Module 3B
Melt Flow in the Extruder
Most analyses of extruders unroll the helical shaped channel Leads to a rectangular
channel covered by an infinite plate moving at constant velocity
The fluid motion (or flow) in the channel can be decomposed A cross flow in the x – y
plan An axial flow in the z
direction.
Spring 2001 14ISAT 430 Dr. Ken Lewis Module 3B
Melt Flow in the Extruder
The axial flow in the z direction is responsible for the pumping
The cross flow does most of the mixing.
Spring 2001 15ISAT 430 Dr. Ken Lewis Module 3B
Extruder Mixing & Melting
The happenings in the channel are complex. Near the leading edge
the polymer has experienced the longest residence time.
Mixing is poor» Flow is laminar» Zero turbulence
Polymer cooking can be a problem.
Direction of travel.
Spring 2001 16ISAT 430 Dr. Ken Lewis Module 3B
Extruder transport
0.5drQ vwd
•Where:
•v = velocity of the plate (m/s)
•D = distance between the plates (m)
•W = width of the plates(m)
Using the unrolled screw model, we can show that:
cosv DN A
cd d
tan cosc fw w D A w A
or
2 20.5 sin cosdr cQ D Nd A A
We have assumed:
wf is negligible
Note:
sintan
cosA
AA
Spring 2001 17ISAT 430 Dr. Ken Lewis Module 3B
Extruder transport – back pressure.
This is the maximum possible output for an extruder.
Conveyance of the polymer through Smaller and smaller cross sections the screen pack and die…
Creates a back pressure, Qbp.
2 20.5 sin cosdr cQ D Nd A A
3 2sin12c
bp
Dd A dpQ
dl
Spring 2001 18ISAT 430 Dr. Ken Lewis Module 3B
Extruder transport – back pressure
The back pressure is a function of Barrel dimensions The polymer viscosity The flight angle The pressure gradient dp/dl…
The pressure gradient dp/dl Is a function of the screw shape, the barrel
size, the flight angel. If we assume the pressure profile is linear
along the barrel, then dp/dl becomes p/L
3 2sin12c
bp
Dd A dpQ
dl
Spring 2001 19ISAT 430 Dr. Ken Lewis Module 3B
Extruder transport3 2sin
12c
bp
Dd A dpQ
dl
Then:
3 2sin12
cbp
p Dd AQ
L
•Where:
•p = the head pressure (Mpa)
•L = length of the barrel (m)
Spring 2001 20ISAT 430 Dr. Ken Lewis Module 3B
Back Pressure Flow
A misnomer It is not back pressure flow It is resistance to forward flow
So what is the net flow?
net dr bpQ Q Q 3 2
2 2 sin0.5 sin cos
12c
net c
p Dd AQ D Nd A A
L
Qnet is what finally comes out of the die!
Spring 2001 21ISAT 430 Dr. Ken Lewis Module 3B
Back Pressure
There is some (hopefully) negligible slippage of fluid between the flight and the barrel wall.
Back pressure reduces flow but causes plastication. In the limit, the back pressure can stop the flow
0e dr bpQ Q Q
dr bpQ Q
And the maximum pressure becomes:
max 2
6 cot
c
DNL Ap
d
Spring 2001 22ISAT 430 Dr. Ken Lewis Module 3B
The Net Flow
There are a lot of parameters in the above equation (relation)
They are of two types
Those we control (design parameters)
Those we don’t control (operating parameters)
3 22 2 sin
0.5 sin cos12
cnet c
p Dd AQ D Nd A A
L
Spring 2001 23ISAT 430 Dr. Ken Lewis Module 3B
Design Parameters
These we control at conception time and are fixed thereafter. Barrel diameter Flight or Helix angle Channel depth dc
Barrel length L
Spring 2001 24ISAT 430 Dr. Ken Lewis Module 3B
Operating Parameters
These we can fiddle with to optimize the process. Rotational speed, N The head pressure (change the die, slow the
screw, change the temperature) The hidden variable … TEMPERATURE. The viscosity
» But only to the extent that the shear rate and temperature will allow!
Spring 2001 25ISAT 430 Dr. Ken Lewis Module 3B
Extruder Characteristics
For a given extruder:
2 20.5 sin coscdrQ D Nd A A N
3 2sin
12c
bp
p Dd A pQ
L
or
e
pQ N
Spring 2001 26ISAT 430 Dr. Ken Lewis Module 3B
Extruder Characteristics
Extrusion PressurePmax
Extruder CharacteristicCurve
Increasing N orincreasing viscosityE
xtruder Flow Rate
Flow up with Increasing N Decreasing p Increasing
Ignores non-Newtonian flow behavior
Ignores friction
e
pQ N
Spring 2001 27ISAT 430 Dr. Ken Lewis Module 3B
Extruder Characteristicse
pQ N
Usual Recommended
Cescr Ce
scr
Output in Kg/h 0.006 2.2 0.006 2.3
Output in lb/h 16 2.2 20 2.35
A useful estimate of extruder capacity with a L/D = 24 is:
scre eQ C D
Actual output may ± 20% (good for back of envelope calculations)
Spring 2001 28ISAT 430 Dr. Ken Lewis Module 3B
A screw extruder has D = 75 mm, dc = 5 mm, A = 17.5°. It rotates at 100 rpm. The plastic has a density of 1 gm/cc.
What is the output for zero back pressure?
22 60min0.5 75 100 5 sin 17.5 cos 17.5
mindr
revQ mm mm
hr
33
3 3
1238,822,278.3 238.8
10 10dr
mm cm gm kg kgQ
hr mm cm gm hr
What is the output expected for normal conditions?
2.30.006 75 123dr
kgQ
hr
Spring 2001 29ISAT 430 Dr. Ken Lewis Module 3B
Die Characteristics
Flow through a die generates back pressure For a simple cylindrical flow channel the flow
rate is given by the famous Hagen – Poiseuille equation:
4
128d
cl
p DQ
L
D = diameter
= melt viscosity [=]
Spring 2001 30ISAT 430 Dr. Ken Lewis Module 3B
Die characteristics
So flow increases with p Look at the power of the die diameter! This gives the linear die characteristic
curve. Note: some people write the above
equation as:
4
128d
cl
p DQ
L
c sQ K p
Spring 2001 31ISAT 430 Dr. Ken Lewis Module 3B
Die characteristics
Where Ks is called the die shape factor Still just equation for laminar flow through
a pipe.
4
128d
cl
p DQ
L
c sQ K p
Spring 2001 32ISAT 430 Dr. Ken Lewis Module 3B
Extrusion PressurePmax
Extruder CharacteristicCurve
Die characteristiccurve
IncreassingL, n,decreasingD
Increasing N orincreasing viscosityE
xtruder Flow Rate
OperatingPoint
Extrusion Curve
Spring 2001 33ISAT 430 Dr. Ken Lewis Module 3B
Operating Point
The values of Q and p where the curves intersect is the extruder operating point.
Note the shape factor Ks is the slope of the die characteristic curve.
Extrusion PressurePmax
Extruder CharacteristicCurve
Die characteristiccurve
IncreassingL, n,decreasingD
Increasing N orincreasing viscosityE
xtruder Flow Rate
OperatingPoint
Spring 2001 34ISAT 430 Dr. Ken Lewis Module 3B
example
Consider an extruder with the following properties: D = 3.0 in L = 75 in N = 1 rev/sec dc = 0.25 in A = 20°
Let the melt have a shear viscosity of = 125 lb-sec/in2 = 103.4 Pa sec
Spring 2001 35ISAT 430 Dr. Ken Lewis Module 3B
example2
Knowing the above characteristics, calculate Qmax and pmax.
2 20.5 sin cosdr cQ D Nd A A
22max 0.5 3 1 0.25 sin 20cos 20
secdr
revQ Q in in
3
max 3.568sec
inQ
Spring 2001 36ISAT 430 Dr. Ken Lewis Module 3B
example3
Knowing the above characteristics, calculate Qmax and pmax.
max 2
6 cot
c
DNL Ap
d
2
max 2
sec cos 206 3 1 75 0.015
sec sin 20
0.25
rev lbfin in
inp
in
max 22796.59
lbfp
in
Spring 2001 37ISAT 430 Dr. Ken Lewis Module 3B
example4
These two values define the abscissa and the ordinate for the extruder characteristic.
If we have a circular die with a diameter Dd = 0.25 in, and a length Ld = 1.0 in
What’s the shape factor for the die?
3
max 3.568sec
inQ max 2
2796.59lbf
pin
Spring 2001 38ISAT 430 Dr. Ken Lewis Module 3B
If we have a circular die with a diameter Dd = 0.25 in, and a length Ld = 1.0 inWhat’s the shape factor for the die?
4
128d
sd
DK
L
4
2
0.25sec
128 0.015 1.0s
inK
lbfin
in
5
0.0063916secs
inK
lbf
remember c sQ K p
Spring 2001 39ISAT 430 Dr. Ken Lewis Module 3B
example5
Now we can find the operating point for the extruder. We can express the extruder characteristic as the straight
line between Qmax and pmax.
maxmax
maxx
QQ Q p
p 3.57 0.0012765xQ p
And from the die equation 0.0063916xQ p
Setting these equal provides the operating point 465.6p psi
3
2.98secx
inQ
Spring 2001 40ISAT 430 Dr. Ken Lewis Module 3B
Extruder Characteristic
0.000
1.000
2.000
3.000
4.000
5.000
6.000
7.000
0 500 1000 1500 2000 2500 3000
Pressure (psi)
Flo
w R
ate
(in
3/se
c)
Q ex
Q die
Spring 2001 41ISAT 430 Dr. Ken Lewis Module 3B
Dies
The polymer is extruded past the breaker plate into the die. Our previous example assumed a cylindrical
die Dies come in many flavors.
The die must take into account several factors Die swell bambooing
Spring 2001 42ISAT 430 Dr. Ken Lewis Module 3B
Die Swell
On the left is a cylindrical die and on the right is an annular die. Note the Barus bulge Due to release of stored elastic energy obtained in the
die and the radical change in velocity of material close to the die walls.
Spring 2001 43ISAT 430 Dr. Ken Lewis Module 3B
Die Swell
Note that as soon as the polymer has left the die, its surface is free Stress free Polymer will relax unless it is kept under tension.
Spring 2001 44ISAT 430 Dr. Ken Lewis Module 3B
Surface Fracture
At high shear rates The polymer in the middle of the round channel is
quiescent while the material near the walls is in high shear.
The energy stored is high enough that upon emerging from the die, the polymer fractures in trying the equilibrate the stresses.
Spring 2001 45ISAT 430 Dr. Ken Lewis Module 3B
Effect of Die Swell
Knowing that die swell will occur is important After the polymer leaves the die it is rapidly
cooling and becoming fixed in shape For each polymer, if we know
» Viscosity» Temperature» Shear rate
We can account for the die swell in the shape of our die
Spring 2001 46ISAT 430 Dr. Ken Lewis Module 3B
Die shapes
The dies The finished shapes
Spring 2001 47ISAT 430 Dr. Ken Lewis Module 3B
Pipe extrusion
The central mandrel is supported by spider legs These disrupt the flow of
polymer The polymer rejoins
itself because » the flow rate is low » The conditions haven’t
changed (temperature) To minimize the effect of
the spiders, the mandrel is tapered.
Spring 2001 48ISAT 430 Dr. Ken Lewis Module 3B
Pipe extrusion To control the pipe size,
other means are used.
Internal sizing mandrel
External sizing using air pressure
External sizing usingvacuum
Spring 2001 49ISAT 430 Dr. Ken Lewis Module 3B
Tubing Die
Note the expansion to the spider legs and the reduction afterwards.
If the extrusion is too rapid, the spider leg openings will not heal.
Spring 2001 50ISAT 430 Dr. Ken Lewis Module 3B
Wire Coating Die
The wire runs straight through
Polymer comes in vertically into a distribution cavity
Used for wire diameters of 1 mm up to submarine cables with diameters of 150 mm.
Spring 2001 51ISAT 430 Dr. Ken Lewis Module 3B
Wire Coating Die2
Note here the wire is helping draw the polymer from the die!
The taught wire provides rigidity during cooling
The product is usually cooled by passing it through a liquid bath
These system roll, making coated wire at speeds up to10,000 ft/min.
Injection Molding
Spring 2001 53ISAT 430 Dr. Ken Lewis Module 3B
Injection Molding
Polymer is heated, mixed, the then forced to flow into a mold cavity
Similar to extrusion Hopper, barrel, screw
Screw rotation is the principal motion only in one part of the cycle Mixes, compacts, plasticizes, and heats Pressures may reach 10 – 20 MPa (1450 –
2900 psi)
Spring 2001 54ISAT 430 Dr. Ken Lewis Module 3B
Injection Molding2
In the injecting stage, the screw is driven axially by a piston to generate the working pressure 150 – 250 MPa (21,756 – 36,260 psi)
Spring 2001 55ISAT 430 Dr. Ken Lewis Module 3B
Spring 2001 56ISAT 430 Dr. Ken Lewis Module 3B
Injection Molding Sequences
(1) Close the mold (2) Inject the melt
(3) Retract the screw (4) Open mold – eject part
Spring 2001 57ISAT 430 Dr. Ken Lewis Module 3B
Two Plate Mold The mold here is closed The mold is position
between two platens One stationary One moveable
Note the water channels for quickly cooling the mold and its polymer load.
Sprue: channel from die nozzle
Into the mold
Runner: channel from SprueInto the cavity
Gates: restrict the polymer
Flow into the cavity
Spring 2001 58ISAT 430 Dr. Ken Lewis Module 3B
Two Plate Mold2
The mold here is open The ejector pins push
the rather fragile plastic from the mold cavity
The sprue and runners are waste..
Spring 2001 59ISAT 430 Dr. Ken Lewis Module 3B
Two Plate Mold3
Cooling system Usually water passages in the mold itself
Gas vents Usually about 0.001 in deep and 0.5 wide. Allows the air to escape when the cavity is
filling Too small to let the viscous polymer follow.
Spring 2001 60ISAT 430 Dr. Ken Lewis Module 3B
Two Plate Mold - Parts
Cavities (shape the part) Distribution channels (get the polymer to
the cavity) Ejection system (safely remove the part) Cooling system (change the polymer from
soup to part) Gas venting facility ( allow the cavity to fill)
Thermoforming
Spring 2001 62ISAT 430 Dr. Ken Lewis Module 3B
Thermoforming
A flat thermoplastic sheet is softened and deformed into the desired shape. Used for large items
» Bathtubs» Skylights» Freezer interior walls» Bumpers
Two steps» Heating» Deforming / forming
Spring 2001 63ISAT 430 Dr. Ken Lewis Module 3B
Thermoforming
Three major types of thermoforming
Vacuum» Pressure limit of 1 atmosphere
Pressure » Higher allowable pressures
Mechanical
Spring 2001 64ISAT 430 Dr. Ken Lewis Module 3B
Vacuum Thermoforming
Spring 2001 65ISAT 430 Dr. Ken Lewis Module 3B
Pressure Thermoforming
Spring 2001 66ISAT 430 Dr. Ken Lewis Module 3B
Mechanical Thermoforming
In (1) the polymer is pre stretched In (2) the polymer is draped over the positive mold and
pressure applied to force it in place
Spring 2001 67ISAT 430 Dr. Ken Lewis Module 3B
Mechanical Thermoforming2
In (1) the polymer is pre heated In (2) the polymer is forced into place in the negative mold.
Spring 2001 68ISAT 430 Dr. Ken Lewis Module 3B
Product design Considerations
In general Strength
» Plastics are not metals» Should not be used in strength or creep critical applications.
Impact resistance» Good, better than many ceramics
Service temperature» Much less than metals or ceramics
Degradation» Radiation» Oxygen or ozone» Solvents
Corrosion resistance» Better than metals
Spring 2001 69ISAT 430 Dr. Ken Lewis Module 3B
Extrusion Considerations
Desirable product traits Wall thickness should be uniform Hollow sections seriously complicate the
extrusion process Corners
» Avoid as they cause uneven polymer flow and are stress concentrators
Spring 2001 70ISAT 430 Dr. Ken Lewis Module 3B
Molded Part Considerations
Economic production Injection molding minimum ~10,000 parts Vacuum etc. usually around ~1,000 parts.
Part complexity Possible, just makes the mold more
complicated Wall thickness
Wasteful and can warp during shrinkage Use ribs for stiffness
Spring 2001 71ISAT 430 Dr. Ken Lewis Module 3B
Molded Part Considerations2
Corner radii and/or fillets Sharp corners are stress concentrators, bad
Holes OK but complicate the mold
Draft (the taper of the cavity) Should be there to allow easy mold removal Recommended drafts
» Thermosets: ½° - 1°» Thermoplastics: 1/8° - ½°
Spring 2001 72ISAT 430 Dr. Ken Lewis Module 3B
Molded Part Considerations3
Tolerances Shrinkage will occur but is predictable The more generous the tolerances the
easier the manufacture. Typical dimension tolerances are:
» +/- 0.006 – 0.010 inches
Typical hole tolerances are:» +/- 0.003 – 0.005 inches