Mechanical properties of two polymers in
a blend or alloy would depend upon their compatibility
or the level of interfacial forces. High adhesion
can only be obtained if the interface can
sustain sufficient stress to induce dissipative
forms of deformation such as flow, yield or
crazing in the polymer. Under most circumstances,
such deformation modes can only be obtained
when the interface is coupled with a sufficient
density of covalent bonds, together with perhaps
some toughening effects due to surface roughness.
Most thermoplastics gain their strength from
entanglement between the chains. The polymer
chains form an entangled network that cannot
pull apart when the material is in the glassy
or semi-crystalline state. Instead, under
stress, the whole network deforms and then
strain hardens as the chains become stretched.
Fracture requires scission of these covalently
bonded chains. To form strong polymer-polymer
adhesion it is necessary for the network to
be continuous across the interface. This continuity
can be formed by:
* Inter diffusion of chains if the two polymers
are sufficiently miscible
* Use of coupling chains placed at the interface
* Chemical reaction to form coupling chains
at the interface
Di block copolymers are used commercially
for the coupling between phases within polymer
blends.
The form of coupling has been found to depend
on the molecular weight of the coupling chains.
Short chains can pull out of the bulk material
at a force that increases with the length
of the pulled-out section. As the length of
the chains increases to somewhere between
one and four times, the length required to
from an entanglement in the melt, the force
required for pullout, becomes greater than
the force to break chains, so they fail by
scission. The extent of adhesion is strongly
affected by the molecular failure mechanism
as tough interfaces are normally only obtained
when the failure is by scission. Scission
failure alone does not ensure a tough interface.
A common technique to couple two bulk polymers
is to introduce into one or both of the materials
a small percentage of chemically modified
chains that can react with the other polymer
to form coupling chains at the interface.
A classic example of this technique is the
introduction into Polypropylene of some Maleic
anhydride grafted Polypropylene chains to
induce coupling with a Polyamide such as Nylon
6. The maleic anhydride functionality can
react with hydroxyl end groups on the Polyamide
chain to form a graft or block copolymer at
the interface. The molecular mechanism of
interfacial failure can again be either pullout
or scission of these coupling chains. Pullout
at low force can occur if either one of the
blocks in the copolymer formed at the interface
is rather short or if there are too many coupling
chains at the interface.
In the Polyamide-Polypropylene example, where
typically there are very few grafts per Polypropylene
chain, pullout is only expected if the grafted
Polypropylene chain is rather short which
can easily happen as the grafting process
tends to cause scission. The Polyamide chain
is typical of bulk material and so has a molecular
weight well above the entanglement molecular
weight to give the material a useful cohesive
toughness.
In other systems, when multiple grafts are
possible on a single chain, then the coupling
chains can become so densely packed at the
interface that they exclude other chains and
so cannot entangle well with the bulk material,
causing pullout failure. This situation has
been observed when the chains themselves were
long enough to entangle.
Coupling by chain inter diffusion can occur
if the two polymeric materials are miscible
in each other, or at least sufficiently miscible
to form a broad interface. Welding is the
most common form of inter diffusion but chain
inter diffusion is also important in solvent
bonding.