Solid Conveying Function
Initial Forwarding and
Compaction of Pellets
Once polymer pellets enter into the screw channel
through the feed throat of an extruder, they drop to the bottom of the barrel
because of gravity. The advancing flight pushes the pellets forward along the
barrel as illustrated in Fig. 2.4. When the screw channel is not full under the
hopper, the pellets do not make full contact with the screw surface and the
screw cannot grab the pellets to rotate with it. The pellets are efficiently
pushed forward by the advancing flight until the screw channel becomes full.
The initial forwarding mechanism is the same as that of screw conveyors such as
the grain feeders used by farmers.
The screw surface becomes hot because of the heat
conducted from the melt, and the screw tip at the die end is heated to the same
temperature as the melt. The screw surface under the hopper is cooled
continuously by the incoming stream of cold feed pellets in a steady-state
operation. Thus the screw surface in this section stays below the melting point
of the pellets in a steady-state operation, and the rubbing force of the
pellets on the screw surface is controlled by the external friction of the
pellets. Low external friction coefficient of the pellets on the screw surface
allows easy sliding of the pellets on the screw, resulting in fast forwarding
and compaction. However, the barrel surface immediately after the feed throat
is usually set well above the melting point of the pellets, and the rubbing
force of the pellets on the barrel surface is controlled by the viscosity of
the polymer. High polymer viscosity gives high rubbing force on the barrel,
resulting in fast forwarding and compaction.
The ratio of the viscosity on the barrel surface to
the external friction coefficient of the polymer, (η/μe), may be used as a
parameter to indicate the initial forwarding and compaction characteristics of
the pellets.
If the screw surface under the hopper becomes hot
and pellets stick on the screw surface, the pellets stuck on the screw will
rotate with the screw, reducing the screw channel area and the output rate.
Then the output rate slowly decreases with time after startup. Such phenomenon
is called “feed bridging”. Thefeed bridging problem often occursonrestart after
an interrupted operation because the screw surface under the hopper becomes hot
during screw stoppage. Sticking of polymer pellets on screw surface must be
avoided in the first several L/D of a screw to avoid feed bridging. If the
sticking problem occurs, the screw over the first several L/D should be bored
out and cooled by water or other suitable cooling medium.
The screw channel quickly becomes full, usually
after 3–5 L/D from the hopper, and the pellets start to be compacted into a solid bed, developing pressure. High internal friction
between the pellets is desirable to transfer the screw torque to the pellets
for compaction. Spherical pellets like ball bearings with a low internal
friction slide past each other and are not compacted easily. Soft pellets are
compacted easily along the screw. Harder pellets
are more difficult to compact, and full compaction
is achieved farther away from the hopper.
The air between the pellets also goes into the screw
with the pellets. It is remarkable that all the air is squeezed out of the
screw as the pellets are compacted. There must be continuous flow paths for the
air to flow backward from the compacting solid bed to the hopper. If the flow
paths are blocked by penetrating melt, the air becomes entrapped in the melt
and the entrapped air mixed in the melt is extruded. The air entrapment problem
is common for hard polymers and powder feeds.
The initial forwarding and compaction rate of a
screw usually increases proportional to the screw speed. At present, there is
no mathematical model that can be used to predict the forwarding and compaction
rate.
Preferred conditions for a high rate of the initial
forwarding and compaction are:
• High
rubbing force on the barrel
– High
viscosity of the polymer
– Barrel
temperature near the melting point of the polymer
– Grooved
barrel surface
• Low
rubbing force on the screw
– Low
external friction coefficient of the polymer
– Low
screw surface temperature far below the melting point of the polymer
– Polished
screw surface
– Low
friction coating on the screw surface
• High
melting point
• High
bulk density
• Soft
pellets for easy compaction
• Shape
and size favorable for high internal friction
2.2.2 Solid
Bed Conveying
Polymer pellets inside a screw channel are compacted
into a solid bed (or a solid plug) after 3–5 L/D from the hopper by the pushing
force of the screw, as discussed in the previous section. For most polymers
which are rigid at the feed temperature, the solid bed moves down the screw
channel as a rigid body. Once the solid bed is fully compacted after 5–7 L/D,
it is very strong under compression, like a rock, and it cannot be easily
compressed or sheared. But, it can be easily split or broken up by tensile force
because the pellets in the solid bed are not fused together. It will be
important to remember various solid bed characteristics when the screw
mechanisms are studied later, in more detail.
This case occurs if the barrel and screw surfaces
are kept below the melting point of the polymer. However, the entire barrel,
starting from the first zone next to the hopper, is usually heated well above
the melting point of the polymer. The screw also becomes hot because of the
heat conducted from the melt. The tip of the screw reaches the melt temperature
unless the screw is bored to the tip and cooled. The screw temperature
increases quickly along the screw and reaches the melting point after 5–7 L/D
from the hopper. Thus the screw temperature, where the solid bed is formed, is
usually well above the melting point. Because a polymer melts quickly upon
touching a hot metal surface above its melting point, the solid bed melts on
all barrel and screw surfaces. The solid bed becomes surrounded by the melt,
The rotating screw grabs the solid bed and makes the
solid bed rotate with it. As the rotating solid bed rubs on the stationary
barrel, the barrel exerts a breaking force on the solid bed and makes the solid
bed slide slightly on the screw surface. Therefore, the solid bed rotates at a
slightly lower speed than the screw. If the barrel is removed or lubricated,
the solid bed rotates with the screw at the same speed. The difference between
the rotational speeds of the screw and the solid bed results in the solid
conveying rate according to the helical geometry of the screw channel.
The slippage of the solid bed on the screw, that is,
the solid bed conveying rate down the screw channel is controlled by the
difference between two forces exerted on the solid bed by
the rotating screw and the stationary barrel. The
pressure inside the screw channel usually increases along the screw because the
forwarding force accumulates along the screw. The increased pressure along the
screw channel pushes the solid bed backward toward the hopper. The only driving
force for solid bed conveying is the rubbing force exerted on the solid bed by
the stationary barrel, resisting the solid bed rotation. The opposing forces
are the rubbing force exerted on the solid bed by the rotating screw and the
increased pressure along the screw channel. A high rubbing force on the barrel
and a low rubbing force on the screw are desirable for a high solid conveying
rate. It is common practice to highly polish the screw surface in order to minimize
the rubbing force on the screw. The barrel surface near the hopper can be
grooved and/or cooled by water to increase the rubbing force on the barrel.
The rubbing force on the barrel or screw surface may
be frictional or viscous in nature, depending on the temperature condition of
the metal surface. If the metal surface is at a temperature above the melting
point of the polymer, the polymer melts as shown in Fig. 2.6, and the rubbing
force is viscous in nature. Because the first barrel zone temperature next to
the hopper is usually set well above the melting point of the polymer in most
cases, the rubbing force on the barrel is viscous in nature and the pressure
builds up linearly along the screw channel, as discussed in Chapter 4. A
polymer with a high viscosity gives a high solid conveying rate in this case.
If the metal surface is at a temperature below the
melting point of the polymer, the solid bed does not melt, as shown in Fig.
2.5, and the rubbing force is frictional in nature. The barrel is readily
heated above the melting point of the polymer
in operation by the heat generated from the frictional force of the solid bed
unless it is cooled efficiently. The barrel section next to the hopper may be
grooved and intensely water-cooled, in order to keep the barrel surface below
the melting point of the polymer. Then, the rubbing force on the barrel is
frictional in nature and the pressure increases exponentially along the screw
channel, as discussed in Chapter 4. Extremely high internal pressures over 69
MPa (10,000 psi) can be developed in this case. However, a grooved barrel
without intense water-cooling does not keep the barrel surface below the
melting point of the polymer,
and such high pressures are not developed. Even if water-cooling is not applied,
a grooved barrel increases the solid conveying rate by increasing the rubbing
force on the barrel [3].
Elastomeric polymers with a low melting or fusion
temperature, such as thermoplastic elastomers, present a unique solid conveying
problem. The pellets of these polymers can fuse together upon compression,
forming an elastic band in the feeding section. The elastic band stretches by
screw rotation and the stretched elastic band wraps around the screw, tightly
holding onto the screw and thus stopping solid conveying. If such a “feed
binding” problem occurs, the output rate is very low and increases only
slightly with increasing screw speed.
The mass solid conveying rate of a screw is equal to
[(the sliding velocity of the solid bed on the screw surface) × (the screw
channel cross-sectional area perpendicular to the screw flight) × (the bulk
density of the solid bed)]. The mathematical solid conveying
models presented in Chapter 4 are used to calculate
the solid conveying rate. The solid conveying rate usually increases nearly
proportional to the screw speed. The mass output rate of an extruder is equal
to the mass solid conveying rate, because an extruder is a continuous pump.
Preferred conditions for a high conveying rate of
the solid bed are:
• Large screw
channel area
• High
rubbing force on the barrel
– High
viscosity of the polymer
– Barrel
temperature near the melting point of the polymer
– Grooved
barrel surface
• Low
rubbing force on the screw
– Screw
temperature significantly higher than the melting point of the polymer
– Highly
polished screw surface
– Low
friction coating on the screw surface
• Small
screw surface area in comparison to the barrel area
– Low
screw channel depth to width ratio
– Large
flight radius on the screw root
• Low
pressure increase along the screw channel
– Long
feeding section
– No or
low reduction of the channel area along the screw