Electrostatic interactions in the association of proteins: an analysis of the thrombin-hirudin complex.

The role of electrostatic interactions in stabilization of the thrombin-hirudin complex has been investigated by means of two macroscopic approaches: the modified Tanford-Kirkwood model and the finite-difference method for numerical solution of the Poisson-Boltzmann equations. The electrostatic potentials around the thrombin and hirudin molecules were asymmetric and complementary, and it is suggested that these fields influence the initial orientation in the process of the complex formation. The change of the electrostatic binding energy due to mutation of acidic residues in hirudin has been calculated and compared with experimentally determined changes in binding energy. In general, the change in electrostatic binding energy for a particular mutation calculated by the modified Tanford-Kirkwood approach agreed well with the experimentally observed change. The finite-difference approach tended to overestimate changes in binding energy when the mutated residues were involved in short-range electrostatic interactions. Decreases in binding energy caused by mutations of amino acids that do not make any direct ionic interactions (e.g., Glu 61 and Glu 62 of hirudin) can be explained in terms of the interaction of these charges with the positive electrostatic potential of thrombin. Differences between the calculated and observed changes in binding energy are discussed in terms of the crystal structure of the thrombin-hirudin complex.

The refined 1.9-A X-ray crystal structure of D-Phe-Pro-Arg chloromethylketone-inhibited human alpha-thrombin: structure analysis, overall structure, electrostatic properties, detailed active-site geometry, and structure-function relationships.

Thrombin is a multifunctional serine proteinase that plays a key role in coagulation while exhibiting several other key cellular bioregulatory functions. The X-ray crystal structure of human alpha-thrombin was determined in its complex with the specific thrombin inhibitor D-Phe-Pro-Arg chloromethylketone (PPACK) using Patterson search methods and a search model derived from trypsinlike proteinases of known spatial structure (Bode, W., Mayr, I., Baumann, U., Huber, R., Stone, S.R., & Hofsteenge, J., 1989, EMBO J. 8, 3467-3475). The crystallographic refinement of the PPACK-thrombin model has now been completed at an R value of 0.156 (8 to 1.92 A); in particular, the amino- and the carboxy-termini of the thrombin A-chain are now defined and all side-chain atoms localized; only proline 37 was found to be in a cis-peptidyl conformation. The thrombin B-chain exhibits the characteristic polypeptide fold of trypsinlike serine proteinases; 195 residues occupy topologically equivalent positions with residues in bovine trypsin and 190 with those in bovine chymotrypsin with a root-mean-square (r.m.s.) deviation of 0.8 A for their alpha-carbon atoms. Most of the inserted residues constitute novel surface loops. A chymotrypsinogen numbering is suggested for thrombin based on the topological equivalences. The thrombin A-chain is arranged in a boomeranglike shape against the B-chain globule opposite to the active site; it resembles somewhat the propeptide of chymotrypsin(ogen) and is similarly not involved in substrate and inhibitor binding. Thrombin possesses an exceptionally large proportion of charged residues. The negatively and positively charged residues are not distributed uniformly over the whole molecule, but are clustered to form a sandwichlike electrostatic potential; in particular, two extended patches of mainly positively charged residues occur close to the carboxy-terminal B-chain helix (forming the presumed heparin-binding site) and on the surface of loop segment 70-80 (the fibrin[ogen] secondary binding exosite), respectively; the negatively charged residues are more clustered in the ringlike region between both poles, particularly around the active site. Several of the charged residues are involved in salt bridges; most are on the surface, but 10 charged protein groups form completely buried salt bridges and clusters. These electrostatic interactions play a particularly important role in the intrachain stabilization of the A-chain, in the coherence between the A- and the B-chain, and in the surface structure of the fibrin(ogen) secondary binding exosite (loop segment 67-80).(ABSTRACT TRUNCATED AT 400 WORDS)

Annexin V-crystal structure and its implications on function.

Annexins constitute a family of cytosolic, water soluble proteins, which bind to negatively charged phospholipids in a calcium-dependent manner. They display structural and functional features of both soluble and integral membrane proteins. The annexins face the hydrophilic as well as the hydrophobic phase (Janus-faced proteins) and mediate ion transport in vitro. We present the refined structure and molecular model of annexin V at 2.0 A resolution. The molecule is almost entirely alpha-helical, and each of the four repeats of annexin V is folded into a compact domain of similar structure. The four domains are arranged in an almost planar, cyclic array. In the center of the molecule, one can find a prominent hydrophilic pore, which we associate with the calcium-selective channel found in annexin V. Annexin V has an overall flat, slightly curved shape with two faces, one convex and one concave. The three calcium binding sites Ca1 to Ca3, all located at the convex face of the molecule, are assumed to be phospholipid binding sites, as suggested by their structural similarity to the calcium site of phospholipase A2. Soluble and membrane-bound annexin have closely similar structures, as shown by electron microscopic analysis. Several other observations provide evidence that the membrane-anchoring region of the annexin V molecule is located on the convex face. In the last part of this article, the electrophysiology of the annexins is described. Ion permeation occurs in discrete conductance states and is regulated by voltage across the membrane. A model for the annexin V-membrane interaction, the ion channel formation, and the ion conduction pathway is proposed.

Crystal and molecular structure of human annexin V after refinement. Implications for structure, membrane binding and ion channel formation of the annexin family of proteins.

Two crystal forms (P6(3) and R3) of human annexin V have been crystallographically refined at 2.3 A and 2.0 A resolution to R-values of 0.184 and 0.174, respectively, applying very tight stereochemical restraints with deviations from ideal geometry of 0.01 A and 2 degrees. The three independent molecules (2 in P6(3), 1 in R3) are similar, with deviations in C alpha positions of 0.6 A. The polypeptide chain of 320 amino acid residues is folded into a planar cyclic arrangement of four repeats. The repeats have similar structures of five alpha-helical segments wound into a right-handed compact superhelix. Three calcium ion sites in repeats I, II and IV and two lanthanum ion sites in repeat I have been found in the R3 crystals. They are located at the convex face of the molecule opposite the N terminus. Repeat III has a different conformation at this site and no calcium bound. The calcium sites are similar to the phospholipase A2 calcium-binding site, suggesting analogy also in phospholipid interaction. The center of the molecule is formed by a channel of polar charged residues, which also harbors a chain of ordered water molecules conserved in the different crystal forms. Comparison with amino acid sequences of other annexins shows a high degree of similarity between them. Long insertions are found only at the N termini. Most conserved are the residues forming the metal-binding sites and the polar channel. Annexins V and VII form voltage-gated calcium ion channels when bound to membranes in vitro. We suggest that annexins bind with their convex face to membranes, causing local disorder and permeability of the phospholipid bilayers. Annexins are Janus-faced proteins that face phospholipid and water and mediate calcium transport.

Role of electrostatic interaction in the stability of the hexamer of constitutive phycocyanin from Fremyella diplosiphon.

The role of electrostatic interactions between the charges carried by the titratable groups in the different aggregates of constitutive phycocyanin from Fremyella diplosiphon has been studied by using a simple theoretical approach based on the modified Tanford-Kirkwood model. The electrostatic potential has also been calculated by means of a numerical solution of the linearized Poisson-Boltzmann equations using the finite-differences technique. The pH dependence of the electrostatic contribution to free energy suggests an electrostatic stabilization of the alpha- and beta-subunits as well as of the (alpha beta)-monomer over a broad pH interval. The charge distributions in the individual alpha- and beta-subunits produce electrostatic complementarity and promote the assembly of the subunits to the (alpha beta)-monomer, as well as of the monomers to the larger trimeric and hexameric aggregates. Trimer-trimer electrostatic interactions exhibit strong pH dependence, predicting an association/dissociation equilibrium with a midpoint at pH 6. The electrostatic trimer-trimer interactions correspond to the steric fit, suggesting that electrostatic interactions may initially help to orient the trimers during aggregation. The distribution of the electrostatic potential of the monomers and of the higher aggregates suggests that it plays an important role also in phycocyanin-linker protein binding.

Electrostatic effects in a large enzyme complex: subunit interactions and electrostatic potential field of the icosahedral beta 60 capsid of heavy riboflavin synthase.

The role of the electrostatic interactions in the stability of the icosahedral beta 60 capsid of heavy riboflavin synthase from Bacillus subtilis has been investigated using an approach based on the theory of Kirkwood and Tanford. The pH dependence of the electrostatic subunit interactions agrees well with experimental data. The electrostatic subunit interaction energy has a pronounced minimum at pH 8.2 for both the ligated and ligand-free capsid. The latter is characterized by a reduction of the magnitude and the pH range of the electrostatic attraction. It is found that only 8 charged groups, which form one cluster and two ion pairs, provide a significant contribution to the capsid stability. The analysis has shown that the aggregation/disaggregation equilibrium seems to be regulated by electrostatic interactions between beta-subunits forming dimers, which connect the relatively stable pentamers in the beta-60 capsid. The release of the ligand causes a reduction of the electrostatic attraction of the dimers, which may induce disaggregation of the capsid. The electrostatic potential field due to the titratable groups and alpha-helix macrodipoles has been calculated on the basis of the Coulomb relation. Two different values of the dielectric constant have been used for the protein and the surrounding solvent, respectively. The electrostatic potential shows a radially polar distribution with a positive pole at the inner capsid wall and a negative pole outside the capsid. An interesting feature of the electrostatic field is the formation of positive potential "channels" that coincide with the channels constituted by the pentameric and trimeric beta-subunit aggregates. It is supposed that the electrostatic potential field plays a role in enzyme-substrate recognition.

[Theoretical studies of the electrostatic interactions in aspartic proteinases, intramolecular interactions in pepsin and penicillopepsin]. / Teoreticheskie issledovaniia élektrostaticheskikh vzaimodeistvii v aspartatnykh proteinazakh, vnutrimolekuliarnye vzaimodeistviia v pepsine i penitsillopepsine.

A semi-empirical approach has been used to estimate the intramolecular electrostatic interactions in pepsin and penicillopepsin. The pH-dependence of the free energy electrostatic term was calculated, and the pH-dependence of the domain interactions has been estimated. As it was shown, the contribution of electrostatic interactions is rather small for the stabilization of the native structure. At the same time the electrostatic repulsion between domains increases with the increase of pH. The later can be the cause of the alkaline denaturation of pepsin and domain mobility.

The 2.0 A X-ray crystal structure of chicken egg white cystatin and its possible mode of interaction with cysteine proteinases.

The crystal structure of chicken egg white cystatin has been solved by X-ray diffraction methods using the multiple isomorphous replacement technique. Its structure has been refined to a crystallographic R value of 0.19 using X-ray data between 6 and 2.0A. The molecule consists mainly of a straight five-turn alpha-helix, a five-stranded antiparallel beta-pleated sheet which is twisted and wrapped around the alpha-helix and an appending segment of partially alpha-helical geometry. The 'highly conserved' region from Gln53I to Gly57I implicated with binding to cysteine proteinases folds into a tight beta-hairpin loop which on opposite sides is flanked by the amino-terminal segment and by a second hairpin loop made up of the similarly conserved segment Pro103I - Trp104I. These loops and the amino-terminal Gly9I - Ala10I form a wedge-shaped 'edge' which is quite complementary to the 'active site cleft' of papain. Docking experiments suggest a unique model for the interaction of cystatin and papain: according to it both hairpin loops of cystatin make major binding interactions with the highly conserved residues Gly23, Gln19, Trp177 and Ala136 of papain in the neighbourhood of the reactive site Cys25; the amino-terminal segment Gly9I - Ala10I of bound cystatin is directed towards the substrate subsite S2, but in an inappropriate conformation and too far away to be attacked by the reactive site Cys25. As a consequence, the mechanism of the interaction between cysteine proteinases and their cystatin-like inhibitors seems to be fundamentally different from the 'standard mechanism' defined for serine proteinases and most of their protein inhibitors.