Alkyl ketene dimers are widely used in sizing treatment of paper products.
It is known that a good sizing effect can only be developed after the sized
paper is cured at elevated temperatures. It is generally accepted that AKD
re-distributes on the surface of the fibres during curing. The mechanism t
hat dominates the re-distribution of AKD during curing is not fully underst
ood and contradictory opinions can be found in the literature. There have b
een speculations in the literature that AKD undergoes a spontaneous 'flow-l
ike' spreading during curing leading to the development of an adequate sizi
ng effect of paper. Other studies have suggested that AKD melt does not und
ergo a spontaneous spreading on the surface of smooth cellulose films. Some
authors stressed that the vaporisation/deposition of AKD also plays a sign
ificant role in AKD sizing. The re-distribution of AKD in the curing proces
s of papermaking is complicated and may involve the spreading of AKD melt,
which is driven by the surface tension and/or the capillary forces, and the
evaporation/re-deposition of AKD vapour. In this work, we examined the mec
hanism of AKD re-distribution on a smooth hydrophilic surface. By excluding
the influence of porosity, this study allows us to focus on the effect of
interfacial energetics on the possible spreading of AKD and the development
of a sizing effect. Glass was used to provide the model for this study. AF
M and XPS were used to monitor the spreading of AKD on the glass surface be
fore and after curing. The Wilhelmy method was used to monitor the developm
ent of a sizing effect on the glass surfaces. Our results show that AKD wax
does not undergo a macroscopic 'flow-like' spreading on the glass surface
at a temperature well above the AKD melting point within the time scale of
the experiment. A sizing effect developed more rapidly on areas of the glas
s surface which were covered with AKD than on areas that were initially not
covered by AKD, since in the latter case sizing develops purely via exposu
re of the glass surface to AKD vapour. This implies that the distribution o
f AKD on the glass surface is likely to be very uneven on a microscopic sca
le. However, such an uneven distribution of AKD does not affect the develop
ment of a good macroscopic sizing effect on the glass surface. (C) 2001 Els
evier Science B.V. All rights reserved.