To make globular proteins suitable for application in adhesives, the specif
ic bonds and interactions which shape their structure have to broken. Only
then, a layer of relatively large, flexible and interwoven polymer chains,
which are firmly attached to the solid surface by adsorption, can be create
d. Such a network layer is essential to save the adhesive bond under an app
lied force, because it can distribute the concentration of stresses generat
ed at the interface into the bulk. Unfolding and swelling of a protein can
be achieved by changing the solvent quality. For the globular whey protein
beta-lactoglobulin, the optimal conditions for unfolding and swelling is fo
und with 98% formic acid as a solvent. In formic acid, beta-lactoglobulin l
ooses its amphoteric character (it is protonated, probably for approximate
to 20%). In addition, formic acid is less polar than water and thus a bette
r solvent for the apolar parts of the protein. The swelling and unfolding b
ehaviour of beta-lactoglobulin is studied by viscosity and CD-spectroscopy
measurements. For the interpretation of the results we apply the Kuhn forma
lism that the conformation of a protein can be described in terms of a stat
istical chain which consists of segments of an average persistence length (
P) over bar. The statistical segment length (P) over bar, which varies with
the experimental conditions, is directly related to the adsorption energy
required for a strong adhesion between coil and surface. It determines the
depletion energy kT (P) over bar(-2) m(-2) which must be overcome by specif
ic attraction between side groups of the protein chain and the surface. For
beta-lactoglobulin in 98% formic acid, we find a (P) over bar value of app
roximate to 2.2 nm, pointing at a relatively flexible chain, The minimum ne
t adsorption energy kT (P) over bar(-2) is then approximate to 1 mJ m(-2) a
relatively small value to be exceeded. Preliminary results of destructive
adhesion tests on beech wood lap-shear Joints reveal promising tensile stre
ngths of approximate to 2.9 +/- 1.1 N mm(-2), indeed. (C) 2000 Elsevier Sci
ence B.V. All rights reserved.