Jr. Lu et al., STRUCTURAL CONFORMATION OF LYSOZYME LAYERS AT THE AIR WATER INTERFACESTUDIED BY NEUTRON REFLECTION/, Journal of the Chemical Society. Faraday transactions (Print), 94(21), 1998, pp. 3279-3287
Citations number
29
Categorie Soggetti
Chemistry Physical","Physics, Atomic, Molecular & Chemical
The adsorption of chicken egg white lysozyme at the air/water interfac
e has been studied by specular neutron reflection. The variation of th
e total thickness of the lysozyme layer at the surface of water under
varying solution conditions has been determined. The use of mixed H2O
and D2O allowed the determination of the extent of immersion of the la
yer in water at all concentrations. The measured layer thickness combi
ned with the globular dimensions of lysozyme suggests that the adsorbe
d lysozyme molecules retain their globular structure with no significa
nt denaturation. Measurements were made over a lysozyme concentration
range of 9 x 10(-4) g dm(-3) to 4 g dm(-3) at pH 7 and at an ionic str
ength of 0.02 M. The thickness of the layer was determined by measurin
g neutron reflectivities in null reflecting water (NRW) where the sign
al is only from the adsorbed protein layer. Below 0.1 g dm(-3) the sur
face coverage increases with bulk concentration but the thickness of t
he layer is constant at 30 +/- 3 Angstrom, suggesting that lysozyme is
adsorbed sideways-on. As the bulk concentration increases, the layer
thickness gradually increases to a value of 47 +/- 3 Angstrom(2) at a
bulk concentration of 1 g dm(-3), suggesting that the molecules switch
from sideways-on to longways-on orientations. The area per molecule a
t 1 g dm(-3) was found to be 950 +/- 50 Angstrom(2) which is close to
the limit of 30 x 30 Angstrom(2) for a saturated layer of longways-on
molecules. The extent of mixing of the layer with water was determined
directly by measuring reflectivity profiles in mixed H2O and D2O. A t
wo layer model was found to be appropriate with an upper layer in air
and a lower layer fully immersed in water. The thickness of the layer
in air was found to vary from 15 +/- 5 Angstrom at the lowest bulk con
centration to 9 +/- 3 Angstrom at the highest concentration studied. T
he results show that as the total layer thickness increases with bulk
concentration the fraction of the layer immersed in water increases fr
om 50 to 85%. At the highest concentration of 4 g dm(-3) the adsorbed
layer is better described by a two layer model consisting of a close p
acked top layer of thickness 47 +/- 3 Angstrom and a loosely packed su
blayer of 30 +/- 3 Angstrom.