Elsevier

Biomaterials

Volume 26, Issue 11, April 2005, Pages 1231-1236
Biomaterials

Coil dimensions of the mussel adhesive protein Mefp-1

https://doi.org/10.1016/j.biomaterials.2004.04.032Get rights and content

Abstract

To obtain a better understanding of factors controlling cross-linking rates of Mussel adhesive proteins, we study the conformation of the Mussel Adhesive Protein Mefp-1. The dimensions of Mefp-1 in solution are determined by dynamic light scattering. Under physiological conditions, the hydrodynamic radius RH of Mefp-1 is found to be 10.5±1.1 nm. Measured Mefp-1 dimensions are compared with theoretical dimensions of Mefp-1 in random coil conformations. We have strong indications that Mefp-1, under dilute and physiological conditions, has a self-avoiding random walk conformation with helix-like deca-peptide segments. With a number of segments of approximately 90, the segment length is found to be 2.7 nm.

Introduction

Mussels like the common blue mussel Mytilus edulis are able to glue themselves underwater to a variety of (hydrophilic) surfaces by using a mix of proteins. Until now, six adhesive proteins, varying in type and molecular weight, have been isolated from the phenolic glands of the blue mussel's foot [1]. They are indicated by Mefp-1 to 6, the abbreviation of M. edulis foot protein. Common for all these proteins is the presence of Dopa (3,4-dihydroxyphenylalanine).

Already in an early stage, the potential of mussel adhesive proteins (MAPs) as high performance medical adhesive was recognised [2], [3], [4]. However, because the yield from extraction is low, several attempts have been made to produce large amounts of proteins using molecular biology based methods [5], [6] or to make synthetic mimics of MAPs, which resulted in various peptide-based products [7], [8], [9], [10]. More recently, the focus has changed to the use of various polymer backbones to which Dopa groups are attached [11], [12], [13], [14].

The main challenge in these bio-mimetic approaches is to sufficiently simplify the structure to enable easy-to-use synthesis routes, while keeping the essential elements of the MAPs. An additional problem is that by mimicking one molecule, it is not taken into account that the mussel uses a mix of proteins, with different molecular weights and amino acid composition.

In mussel adhesion, the interplay between the rate of deposition and the cross-linking rates determines the properties of the adhesive bond [15]. Cross-linking rates determine curing times. Especially in medical applications these must be well controlled.

The kinetics of reactions of macromolecules bearing reactive groups are unusual in many respects. They not only depend on the chemical reaction rates, but also on the dynamics and the conformation of the macromolecules. Important parameters are, for example, solvent quality, molecular weight and chain stiffness [16]. Therefore, in the design of synthetic mimics of MAP, information of the conformation of MAPs and the effect of molecular weight on cross-linking rates are indispensable.

In a previous paper, we determined the reaction rates of Dopa groups in the mussel adhesive protein Mefp-1 [17]. In this paper, we determine the chain stiffness under physiological conditions. The possible conformation of Mefp-1 is discussed by comparing the experimental results with literature data.

Section snippets

Mefp-1

Mefp-1 has a molecular weight of 115 kDa based on mass spectroscopy [18] and of 130 kDa on the basis of gel chromatography [19]. It is mainly composed of a repeating uniform deca-peptide. One Mefp-1 molecule contains 71 deca-peptides and 12 hexa-peptides of comparable composition, as shown in Fig. 1. The distribution of the deca- and hexa-peptides over the Mefp-1 backbone is illustrated in Fig. 2. The total number of amino acids is 897.

Looking at the molecular structure of Mefp-1, several

Coil dimensions

In the cross-linking kinetics for random coiled molecules, the reaction rate depends on the reactivity of the groups and the conformation of the coil. For example, in dilute systems in a good solvent the effective rate constant for a reactive group connected to a chain segment with length A is given by [16]k≃k0A3Ñ−vgin which k0 is the reactivity of a single segment, Ñ an effective chain length, related to the location on, and number of segments (N) in the chain [16], [17]. The exponent ν=35.

Experimental

The samples of Mefp-1 had a purity of 95% and were delivered in 1% citric acid at concentrations of 1.3 mg/ml. These stock solutions were stored in the dark at 4°C. To prevent oxidation of DOPA groups, a 50 mmol l(+)-ascorbic acid (Fluka) buffer in millipore water was used. NaCl was added for the desired ionic strength and the pH was set at 3.8. The DLS apparatus was equipped with a JDS Uniphase 633 nm 35-mW laser, an ALV sp-125 s/w 93 goniometer, a fibre detector and a Perkin Elmer photon counter

Results

First, measurements were performed with Mefp-1 concentrations varying from 0.013 to 0.13 mg/ml. No considerable effect of the Mefp-1 concentration on the measured dimensions was detected. Therefore, in further analysis, there was no need for extrapolations to zero concentration, and all subsequent measurements were done with Mefp-1 concentrations of 0.13 mg/ml. In Fig. 3 the thus obtained hydrodynamic radii of Mefp-1 are plotted as a function of the inverse ionic strength, enabling an

Analysis and discussion

Sedimentation studies on Mefp-1, performed by Deacon et al. [22], resulted in a frictional ratio f/f0 of 3.2±0.3 at pH=4.5 and ionic strength of 0.1 m, with f0 as the friction coefficient of the dehydrated protein, and a partial specific volume of dehydrated Mefp-1 of 0.75 ml/g. This frictional ratio corresponds with an RH (of the hydrated coil) of 10±1.0 nm and agrees well with our DLS results.

Conclusions

The experimentally obtained hydrodynamic radius of Mefp-1 of 10.5±1 nm can be explained by two different models. Assuming that Mefp-1 is a fully random protein, it can be described as a random polymer in θ-conditions, which is also called a Gaussian chain. If it is assumed that within the deca-peptide segment there is some helical-like structure present, the found hydrodynamic radius can only be explained by assuming good solvent conditions. The reactivity of the Dopa groups and the hydrophilic

Acknowledgements

The authors thank M. Qvist (Biopolymer Products AB, Alingsås, Sweden) who kindly supplied the Mefp-1 samples and the Dutch Technology Foundation STW for their financial support.

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