Protein—surface interactions in the presence of polyethylene oxide

Abstract The protein resistance character of polyethylene oxide (PEO) chains terminally attached to a hydrophobic solid substrate is theoretically studied. Steric repulsion, van der Waals attraction, and hydrophobic interaction free energies are considered. The results are dependent on the chain length and surface density of PEO. The protein approaches the PEO surface by diffusion and is affected by the van der Waals attraction between the PEO surface and protein through water. Further approach of the protein initiates the compression of PEO chains, which induces a steric repulsion effect; an additional van der Waals attraction becomes important between the substrate and protein through the water solvated PEO layer. The van der Waals component with the substrate decreases with increasing surface density and chain length of terminally attached PEO chains. Other synthetic polymers were also studied, indicating that the protein resistance character is related to the refractive index, with PEO having the lowest refractive index of the common water-soluble synthetic polymers. The osmotic and elastic constants of steric repulsion for terminally attached PEO were estimated as ∼0.007 and 0.02, respectively, from literature data for PEO adsorbed to mica. The steric repulsion free energy and the combined steric repulsion and hydrophobic interaction free energies were calculated as a function of surface density and chain length of PEO. The free energy calculations as a function of surface density and chain length of PEO reveal that a high surface density and long chain length of terminally attached PEO should exhibit optimal protein resistance, with the attainment of high surface density of PEO being more important than long chain length. These theoretical results should be helpful in the design and development of materials resistant to protein adsorption.

[1]  G. Hadziioannou,et al.  A simple model for forces between surfaces bearing grafted polymers applied to data on adsorbed block copolymers , 1988 .

[2]  T. Tadros,et al.  Forces between graft copolymers adsorbed to mica surfaces , 1988 .

[3]  P. Luckham,et al.  Forces between two adsorbed poly(ethylene oxide) layers in a good aqueous solvent in the range 0-150 nm , 1984 .

[4]  C. Toprakcioglu,et al.  Forces between surfaces bearing terminally anchored polymer chains in good solvents , 1988, Nature.

[5]  T. Okano,et al.  Surfaces and Blood Compatibility Current Hypotheses , 1987 .

[6]  P. Gennes Scaling Concepts in Polymer Physics , 1979 .

[7]  Per Stenius,et al.  Direct measurement of temperature-dependent interactions between non-ionic surfactant layers , 1986 .

[8]  C. Toprakcioglu,et al.  Direct measurement of the interaction between mica surfaces with adsorbed diblock copolymer in a good solvent , 1988 .

[9]  Joseph D. Andrade,et al.  Protein—surface interactions in the presence of polyethylene oxide: II. Effect of protein size , 1991 .

[10]  J. Israelachvili,et al.  Measurement of the hydrophobic interaction between two hydrophobic surfaces in aqueous electrolyte solutions , 1984 .

[11]  F. E. Bailey,et al.  Poly(ethylene oxide) , 1976 .

[12]  H. Tadokoro,et al.  Structural studies on polyethers, [‐(CH2)m‐O‐]n. II. Molecular structure of polyethylene oxide , 1964 .

[13]  P. Gennes Polymers at an interface. 2. Interaction between two plates carrying adsorbed polymer layers , 1982 .

[14]  Interaction of hydrophobized filaments in aqueous electrolyte solutions , 1988 .

[15]  R. H. Boyd,et al.  A Dielectric Study of the Effects of Melting on Molecular Relaxation in Poly(ethylene oxide) and Polyoxymethylene , 1971 .

[16]  C. Toprakcioglu,et al.  Interactions between surfaces bearing end-adsorbed chains in a good solvent , 1990 .

[17]  B. Derjaguin,et al.  The modern state of the macroscopic theory of molecular forces and the results of its experimental verification for thin interlayers , 1987 .

[18]  D. F. Evans,et al.  Attractive forces between uncharged hydrophobic surfaces: direct measurements in aqueous solution. , 1985, Science.

[19]  J. H. Lee,et al.  Protein-resistant surfaces prepared by PEO-containing block copolymer surfactants. , 1989, Journal of biomedical materials research.

[20]  Hiroyuki Tadokoro,et al.  Structural Studies of Polyethers, (-(CH2)m-O-)n. X. Crystal Structure of Poly(ethylene oxide) , 1973 .

[21]  J. Eriksson,et al.  Salt effects on the cloud point of the poly(ethylene oxide)+ water system , 1984 .

[22]  P. Claesson,et al.  Direct measurements of steric interactions between mica surfaces covered with electrostatically bound low-molecular-weight polyethylene oxide , 1987 .

[23]  R. C. Weast CRC Handbook of Chemistry and Physics , 1973 .

[24]  H. Christenson,et al.  Very long range attractive forces between uncharged hydrocarbon and fluorocarbon surfaces in water , 1988 .

[25]  T. Kotaka,et al.  Dielectric Relaxations in Poly(ethylene oxide): Dependence on Molecular Weight , 1981 .

[26]  J. Israelachvili Intermolecular and surface forces , 1985 .

[27]  P. Luckham,et al.  Interactions between smooth solid surfaces in solutions of adsorbing and nonadsorbing polymers in good solvent conditions , 1985 .

[28]  P. G. de Gennes,et al.  Polymer solutions near an interface. Adsorption and depletion layers , 1981 .

[29]  S. Granick,et al.  Forces between surfaces of block copolymers adsorbed on mica , 1986 .

[30]  R. Kjellander,et al.  Water structure and changes in thermal stability of the system poly(ethylene oxide)–water , 1981 .

[31]  Y. Okahata,et al.  Viscoelastic properties of lipid surfactant/polymer composite films , 1988 .

[32]  P. Luckham,et al.  Forces between two adsorbed polyethylene oxide layers immersed in a good aqueous solvent , 1982, Nature.

[33]  J. Klein Forces between mica surfaces bearing adsorbed macromolecules in liquid media , 1983 .

[34]  J. Proust,et al.  Effects of a non-adsorbing polymer on colloid stability : force measurements between mica surfaces immersed in dextran solution , 1985 .