Life: Self-Directing with Unlimited Variability on Self-Speeding

Abstract

The crystal structure of the deoxyoctamer d(G-G-^Br U-A-^BrU-A-C-C) was refined to a resolution of 1.7Å using combined diffractometer and synchrotron data. The analysis was carried out independently in two laboratories using different procedures. Although the final results are identical the comparison of the two approaches highlights potential problems in the refinement of oligonucleotides when only limited data are available.

As part of the analysis the positions of 84 solvent molecules in the asymmetric unit were established. The DNA molecule is highly solvated, particularly the phosphate-sugar backbone and the functional groups of the bases. The major groove contains, in the central ^BrU-A-^BrU-A region, a ribbon of water molecules forming closed pentagons with shared edges. These water molecules are linked to the base O and N atoms and to the solvent chains connecting the O-1 phosphate oxygen atoms on each strand. The minor groove is also extensively hydrated with a continuous network in the central region and other networks at each end. The pattern of hydration is briefly compared with that observed in the crystal structure of a B-dodecamer.     

Ordered water structure around a B-DNA dodecamer: A quantitative study

The crystal structure of the double-helical B-DNA dodecamer of sequence C-G-C-G-A-A-T-T-C-G-C-G has been solved and refined independently in three forms: (1) the parent sequence at room temperature; (2) the same sequence at 16 K; and (3) the 9-bromo variant C-G-C-G-A-A-T-T^BrC-G-C-G at 7 °C in 60% (v/v) 2-methyl-2.4-pentanediol. The latter two structures show extensive hydration along the phosphate backbone, a feature that was invisible in the native structure because of high temperature factors (indicating thermal or static disorder) of the backbone atoms. Sixty-five solvent peaks are associated with the phosphate backbone, or an average of three per phosphate group. Nineteen other molecules form a first shell of hydration to base edge N and O atoms within the major groove, and 36 more are found in upper hydration layers. The latter tend to occur in strings or clusters spanning the major groove from one phosphate group to another. A single spermine molecule also spans the major groove. In the minor groove, the zig-zag spine of hydration that we believe to be principally responsible for stabilizing the B form of DNA is found in all three structures. Upper level hydration in the minor groove is relatively sparse, and consists mainly of strings of water molecules extending across the groove, with few contacts to the spine below. Sugar O-1′ atoms are closely associated with water molecules, but these are chiefly molecules in the spine, so the association may reflect the geometry of the minor groove rather than any intrinsic attraction of O-1′ atoms for hydration. The phosphate O-3′ and O-5′ atoms within the backbone chain are least hydrated of all, although no physical or steric impediment seems to exist that would deny access to these oxygen atoms by water molecules.     

Hydration of transfer RNA molecules: a crystallographic study

Four crystal structures of transfer RNA molecules were refined at 3 A resolution with the inclusion of the solvent molecules found in the difference maps: yeast tRNA-phe in the orthorhombic form, yeast tRNA-phe in the monoclinic form and yeast tRNA-asp in the A and B forms. Over 100 solvent molecules were located in each tRNA crystal. Several hydration schemes are found repeatedly in the 4 crystals. The tertiary interactions in the corner of the L-shaped molecule attract numerous solvent molecules which bridge the ribose hydroxyl O(2') atoms, base exocyclic atoms and phosphate anionic oxygen atoms. Conservation of bases leads to conservative localized hydration patterns. Several solvent molecules are found stabilizing unusual base pairs like the G-U pairs and those involving the pseudouridine base. Water bridges between the O(2') and the exocyclic atom O2 of pyrimidines or the N3 atom of purines are common. Water bridges occur frequently between successive anionic oxygen atoms of each strand as well as between N7 or other exocyclic atoms of successive bases in the major groove. Magnesium ions or spermine molecules are found to bind in the major groove of tRNA helices without specific interactions.     

Refined atomic model of the four-layer aggregate of the tobacco mosaic virus coat protein at 2.4-A resolution.

Previous x-ray studies (2.8-A resolution) on crystals of tobacco mosaic virus coat protein grown from solutions containing high salt have characterized the structure of the protein aggregate as a dimer of a bilayered cylindrical disk formed by 34 chemically identical subunits. We have determined the crystal structure of the disk aggregate at 2.4-A resolution using x-ray diffraction from crystals maintained at cryogenic temperatures. Two regions of interest have been extensively refined. First, residues of the low-radius loop region, which were not modeled previously, have been traced completely in our electron density maps. Similar to the structure observed in the virus, the right radial helix in each protomer ends around residue 87, after which the protein chain forms an extended chain that extends to the left radial helix. The left radial helix appears as a long alpha-helix with high temperature factors for the main-chain atoms in the inner portion. The side-chain atoms in this region (residues 90-110) are not visible in the electron density maps and are assumed to be disordered. Second, interactions between subunits in the symmetry-related central A pair have been determined. No direct protein-protein interactions are observed in the major overlap region between these subunits; all interactions are mediated by two layers of ordered solvent molecules. The current structure emphasizes the importance of water in biological macromolecular assemblies.     

Stabilization of Z-DNA by demethylation of thymine bases: 1.3-A single-crystal structure of d(m5CGUAm5CG)

Methylation of cytosine bases at the C5 position has been known to stabilize Z-DNA. We had previously predicted from calculations of solvent-accessible surfaces that the methyl group at the same position of thymine has a destabilizing effect on Z-DNA. In the current studies, the sequence d(m5CGUAm5CG) has been crystallized and its structure solved as Z-DNA to 1.3-A resolution. A well-defined octahedral hexaaquomagnesium complex was observed to bridge the O4 oxygens of the adjacent uridine bases at the major groove surface, and four well-structured water molecules were found in the minor groove crevice at the d(UA) dinucleotide. These solvent interactions were not observed in the previously published Z-DNA structure of the analogous d(m5CGTAm5CG) sequence. A comparison of the thymine and uridine structures supports our prediction that demethylation of thymine bases helps to stabilize Z-DNA. A comparison of this d(UA)-containing Z-DNA structure with the analogous d(TA) structure shows that access of the O4 position is hindered by the C5 methyl of thymine due to steric and hydrophobic inhibition. In the absence of the methyl group, a magnesium-water complex binds to and slightly affects the structure of the Z-DNA major groove surface. This perturbation of the solvent structure at the major groove surface is translated into a much larger 1.41-A widening of the minor groove crevice, thereby allowing the specific binding of two water molecules at well-defined sites of each internal d(UA) base pair. Possible mechanisms by which modifications at the major groove surface of Z-DNA can affect the solvent properties of the minor groove crevice are discussed.     

Absence of minor groove monovalent cations in the crosslinked dodecamer C-G-C-G-A-A-T-T-C-G-C-G.

The structure of a crosslinked B -DNA dodecamer of sequence C-G-C-G-A-A-T-T-C-G-C-G has been solved to a resolution of 1.43 A. The dithiobis-propane crosslink, -CH2-CH2-CH2-S-S-CH2-CH2-CH2-, bridges N7 atoms of adenine bases 6 and 18 in the two central base-pairs within the major groove. The crosslink is sufficiently long that no bending is induced in the helix, which is essentially isostructural with the native unlinked dodecamer at 1.9 A. A constellation of solvent peaks tentatively fitted as a spermine molecule in that earlier analysis is now seen at higher resolution to be a well-defined octahedral magnesium hexahydrate complex in the major groove. One end of the duplex curves around that complex to produce a roll-bend near base-pairs 3-5, and an overall bend in helix axis, as has long been noted. Two other magnesium complexes connect the helices and help to knit the crystal lattice together. No evidence exists for partial sodium or potassium ion substitution for solvent water molecules within the minor groove spine of hydration, as had been suggested previously: not coordination geometry and environment, nor B values, nor calculated valence values, nor difference map analyses. Indeed, the very numbers that have been claimed in support of partial substitution by sodium or potassium ions are reproduced with the present crystals, which by chemical analysis contains only one trace sodium ion per 160 bp, and one potassium ion per 41 bp. In contrast, our crystals contain one Mg2+ per base-pair, meaning that phosphate group charge neutrality is accomplished by divalent cations, not monovalent ions. Three of these magnesium cations per duplex are localized and visible in the X-ray analysis, and nine are disordered and invisible. Hence although binding of monovalent cations within the minor groove of A -tracts on occasion may be a consequence of groove narrowing, it cannot be the cause of that narrowing. Cations, contrary to what has been claimed, are not in charge.     

Structure, dynamics and hydration of the nogalamycin-d(ATGCAT)2Complex determined by NMR and molecular dynamics simulations in solution.

The structure of the 1:1 nogalamycin:d(ATGCAT)2 complex has been determined in solution from high-resolution NMR data and restrained molecular dynamics (rMD) simulations using an explicit solvation model. The antibiotic intercalates at the 5'-TpG step with the nogalose lying along the minor groove towards the centre of the duplex. Many drug-DNA nuclear Overhauser enhancements (NOEs) in the minor groove are indicative of hydrophobic interactions over the TGCA sequence. Steric occlusion prevents a second nogalamycin molecule from binding at the symmetry-related 5'-CpA site, leading to the conclusion that the observed binding orientation in this complex is the preferred orientation free of the complication of end-effects (drug molecules occupy terminal intercalation sites in all X-ray structures) or steric interactions between drug molecules (other NMR structures have two drug molecules bound in close proximity), as previously suggested. Fluctuations in key structural parameters such as rise, helical twist, slide, shift, buckle and sugar pucker have been examined from an analysis of the final 500 ps of a 1 ns rMD simulation, and reveal that many sequence-dependent structural features previously identified by comparison of different X-ray structures lie within the range of dynamic fluctuations observed in the MD simulations. Water density calculations on MD simulation data reveal a time-averaged pattern of hydration in both the major and minor groove, in good agreement with the extensive hydration observed in two related X-ray structures in which nogalamycin is bound at terminal 5'-TpG sites. However, the pattern of hydration determined from the sign and magnitude of NOE and ROE cross-peaks to water identified in 2D NOESY and ROESY experiments identifies only a few "bound" water molecules with long residence times. These solvate the charged bicycloaminoglucose sugar ring, suggesting an important role for water molecules in mediating drug-DNA electrostatic interactions within the major groove. The high density of water molecules found in the minor groove in X-ray structures and MD simulations is found to be associated with only weakly bound solvent in solution.     

Visualisation of extensive water ribbons and networks in a DNA minor-groove drug complex.

The crystal structure is reported of a complex between an ethyl derivative of the minor-groove drug furamidine and the dodecanucleotide duplex d(CGCGAATTCGCG)2, which has been refined to 1.85 A resolution and an R factor of 16.6% for data collected at -173 degreesC. An exceptionally large number (220) of water molecules have been located. The majority of these occur in the first coordination shell of solvation. There are extensive networks of connected waters, both in the major and minor grooves. In particular, there are 21 water molecules associated with the minor-groove drug, via hydrogen bonds from the four charged nitrogen atoms. One cluster of four waters is situated in the groove itself; the majority are on the outer edge of the groove, and serve to bridge between the outward-directed drug nitrogen atoms and backbone phosphate oxygen atoms. These bridges are both intra- and inter-strand, with the net effect that the outer edge of the drug molecule is covered by ribbons of water molecules.     

Water spines and networks in G-quadruplex structures

Quadruplex DNAs can fold into a variety of distinct topologies, depending in part on loop types and orientations of individual strands, as shown by high-resolution crystal and NMR structures. Crystal structures also show associated water molecules. We report here on an analysis of the hydration arrangements around selected folded quadruplex DNAs, which has revealed several prominent features that re-occur in related structures. Many of the primary-sphere water molecules are found in the grooves and loop regions of these structures. At least one groove in anti-parallel and hybrid quadruplex structures is long and narrow and contains an extensive spine of linked primary-sphere water molecules. This spine is analogous to but fundamentally distinct from the well-characterized spine observed in the minor groove of A/T-rich duplex DNA, in that every water molecule in the continuous quadruplex spines makes a direct hydrogen bond contact with groove atoms, principally phosphate oxygen atoms lining groove walls and guanine base nitrogen atoms on the groove floor. By contrast, parallel quadruplexes do not have extended grooves, but primary-sphere water molecules still cluster in them and are especially associated with the loops, helping to stabilize loop conformations.     

A high angle neutron fibre diffraction study of the hydration of the A conformation of the DNA double helix.

A high angle neutron fibre diffraction study of the distribution of water around the A-form of DNA has been performed using the diffractometer D19 at the Institut Laue-Langevin, Grenoble. These experiments have exploited the ability to replace H2O surrounding the DNA by D2O so that isotopic difference Fourier maps can be computed in which peaks are identified with the distribution of water in the unit cell. All peaks of significant height have been accounted for by four families of water molecules whose positions and occupancies have been determined using least squares refinement. The coordinates of the water peaks making up each family do not deviate significantly from a regular helical arrangement with the same parameters as the DNA. Two of these families are of particular interest. The first consists of water molecules in the major groove linking successive charged phosphate oxygens along the polynucleotide chains. The second is associated with bases in the major groove and forms a central core of density along the helix axis. These two families provide a layer of hydration lining the interior wall of the major groove leaving a central channel to accommodate cations. The relationship between these observations and conformational stability is discussed.     

The hydration of the neurotransmitter acetylcholine in aqueous solution

Neutron diffraction augmented with hydrogen isotope substitution has been used to examine the water structure around the acetylcholine molecular ion in aqueous solution. It is shown that the nearest-neighbor water molecules in the region around the trimethylammonium headgroup are located either in a ring around the central nitrogen atom or between the carbon atoms, forming a sheath around the onium group. Moreover the water molecules in this cavity do not bond to the onium group but rather form hydrogen bonds with water molecules in the surrounding aqueous environment. Given that in the bound state the onium headgroup must be completely desolvated, the absence of bonding between the onium headgroup and the surrounding water solvent may be selectively favorable to acetylcholine-binding in the receptor site. Away from the headgroup, pronounced hydrogen-bonding of water to the carbonyl oxygen is observed, but not to the ether oxygen in the acetylcholine chain.     

The structure of sitting-atop complexes of metalloporphyrins studied by theoretical methods

The metallation of tetrapyrroles is believed to proceed via a sitting-atop (SAT) complex, in which some of the pyrrole nitrogen atoms are still protonated and the metal ion resides above the ring plane. No crystal structure of such a complex has been presented, but NMR and extended X-ray absorption fine structure (EXAFS) data has been reported for Cu(2+) in acetonitrile. We have used density functional calculations to obtain reasonable models for SAT complexes of porphyrins with Mg(2+), Fe(2+), and Cu(2+). The results show that there are many possible SAT complexes with 1-5 solvent molecules, one or two metal ions, and cis or trans protonation of the porphyrin ring. Many of these have similar energies and their relative stabilities vary with the metal ion. A complex with two cis pyrrolenine nitrogens atoms and 2-4 solvent molecules coordinated to Cu(2+) fits the NMR and EXAFS data best. However, we cannot fully exclude the possibility that what is observed is rather a mixture of a doubly protonated porphyrin and the copper porphyrin. Mg(2+) has a lower affinity for porphyrin and stronger affinity for water, so a complex with five water molecules and only one bond to porphyrin seems to be most stable. For Fe(2+), a cis structure with two first-sphere water molecules and four interactions to the porphyrin seems to be most likely.     

Crystal structure of the B-DNA hexamer d(CTCGAG): model for an A-to-B transition.

The crystal structure of the B-DNA hexamer d(CTCGAG) has been solved at 1.9 A resolution by iterative single isomorphous replacement, using the brominated derivative d(CG5BrCGAG), and refined to an R-factor of 18.6% for 120 nonhydrogen nucleic acid atoms and 32 water molecules. Although the central four base pairs form a typical B-form helix, several parameters suggest a transition to an A-like conformation at the termini. Based on this observation, a B-to-A transition was modeled, maintaining efficient base stacking across the junction. The wide minor groove (approximately 6.9 A) is reminiscent of that in the side-by-side double drug-DNA complexes and hosts a double spine of hydration. The global helix axes of the pseudo-continuous helices are at an acute angle of 60 degrees. The pseudocontinuous stacking is reinforced by the minor groove water structure extending between the two duplexes. The crossover point of two pairs of stacked duplexes is at the stacking junction, unlike that observed in the B-DNA decamers and dodecamers. This arrangement may have implications for the structure of a four-way DNA junction. The duplexes are arranged around a large (approximately 20 A diameter) channel centered on a 6(2) screw axis.     

Crystal and molecular structure of the ammonium salt of the dinucleoside monophosphate d(CpG)

The crystal and molecular structure of the ammonium salt of deoxycytidylyl-(3'-5')-deoxyguanosine has been determined from 0.85 A resolution single crystal X-ray diffraction data. The crystals obtained by acetone diffusion technique at -20 degrees C, are orthorhombic, P212121, a = 12.880(2), b = 17444(2) and c = 27.642(2) A. The structure was solved by high resolution Patterson and Fourier methods and refined to R = 0.136. There are two d(CpG) molecules in the asymmetric unit forming a mini left handed Z-DNA helix. This is in contrast to the earlier reported forms of d(CpG) where the molecules form self base paired duplexes. There are two ammonium ions in the asymmetric unit. The major groove NH+4 ion interacts with N7 of guanines through water bridges besides making H-bonded interactions directly with the phosphate oxygen atoms. A second NH+4 ion is found in the minor groove interacting directly with the phosphate oxygen atoms. Symmetry related molecules pack in such a way that the cytosine base stacks on cytosine and guanine base on guanine. Our structure demonstrates that alternating d(CpG) sequences have the ability to adopt the left handed Z-DNA structure even at the dimer level i.e., in a sequence which is only two base pairs long.     

X-ray analyses of aspartic proteinases. The three-dimensional structure at 2.1 A resolution of endothiapepsin

The molecular structure of endothiapepsin (EC 3.4.23.6), the aspartic proteinase from Endothia parasitica, has been refined to a crystallographic R-factor of 0.178 at 2.1 A resolution. The positions of 2389 protein non-hydrogen atoms have been determined and the present model contains 333 solvent molecules. The structure is bilobal, consisting of two predominantly beta-sheet domains that are related by an approximate 2-fold axis. Of approximately 170 residues, 65 are topologically equivalent when one lobe is superimposed on the other. Twenty beta-strands are arranged as five beta-sheets and are connected by regions involving 29 turns and four helices. A central sheet involves three antiparallel strands from each lobe organized around the dyad axis. Each lobe contains a further local dyad that passes through two sheets arranged as a sandwich and relates two equivalent motifs of four antiparallel strands (a, b, c, d) followed by a helix or an irregular helical region. Sheets 1N and 1C, each contain two interpenetrating psi structures contributed by strands c,d,d' and c',d',d, which are related by the intralobe dyad. A further sheet, 2N or 2C, is formed from two extended beta-hairpins from strands b,c and b',c' that fold above the sheets 1N and 1C, respectively, and are hydrogen-bonded around the local intralobe dyad. Asp32 and Asp215 are related by the interlobe dyad and form an intricate hydrogen-bonded network with the neighbouring residues and comprise the most symmetrical part of the structure. The side-chains of the active site aspartate residues are held coplanar and the nearby main chain makes a "fireman's grip" hydrogen-bonding network. Residues 74 to 83 from strands a'N and b'N in the N-terminal lobe form a beta-hairpin loop with high thermal parameters. This "flap" projects over the active site cleft and shields the active site from the solvent region. Shells of water molecules are found on the surface of the protein molecule and large solvent channels are observed within the crystal. There are only three regions of intermolecular contacts and the crystal packing is stabilized by many solvent molecules forming a network of hydrogen bonds. The three-dimensional structure of endothiapepsin is found to be similar to two other fungal aspartic proteinases, penicillopepsin and rhizopuspepsin. Even though sequence identities of endothiapepsin with rhizopuspepsin and penicillopepsin are only 41% and 51%, respectively, a superposition of the three-dimensional structures of these three enzymes shows that 237 residues (72%) are within a root-mean-square distance of 1.0 A.     

Analysis of solvent structure in proteins using neutron D2O-H2O solvent maps: pattern of primary and secondary hydration of trypsin.

A method of determining the water structure in protein crystals is described using neutron solvent difference maps. These maps are obtained by comparing the changes in diffracted intensities between two data sets, one in which H2O is the major solvent constituent, and a second in which D2O is the solvent medium. To a good first approximation, the protein atom contributions to the scattering intensities in both data sets are equal and cancel, but since H2O and D2O have very different neutron-scattering properties, their differences are accentuated to reveal an accurate representation of the solvent structure. The method also employs a series of density modification steps that impose known physical constraints on the density distribution function in the unit cell by making real space modifications directly to the density maps. Important attributes of the method are that (1) it is less subjective in the assignment of water positions than X-ray analysis; (2) there is threefold improvement in the signal-to-noise ratio for the solvent density; and (3) the iterative density modification produces a low-biased representation of the solvent density. Tests showed that water molecules with as low as 10% occupancy could be confidently assigned. About 300 water sites were assigned for trypsin from the refined solvent density; 140 of these sites were defined in the maps as discrete peaks, while the remaining were found within less-ordered channels of density. There is a very good correspondence between the sites in the primary hydration layer and waters found in the X-ray structure. Most water sites are clustered into H-bonding networks, many of which are found along intermolecular contact zones. The bound water is equally distributed between contacting apolar and polar atoms at the protein interface. A common occurrence at hydrophobic surfaces is that apolar atoms are circumvented by one or more waters that are part of a larger water network. When the effects on surface accessibility by neighboring molecules in the crystal lattice are taken into consideration, only about 29% of the surface does not interface ordered water. About 25% of the ordered water is found in the second hydration sphere. In many instances these waters bridge larger clusters of primary layer waters. It is apparent that, in certain regions of the crystal, the organization of ordered water reflects the characteristics of the crystal environment more than those of trypsin's surface alone.     

1H NMR relaxometric characterization of bovine lactoferrin

Lactoferrin (Lf) is a mammalian iron binding protein present in external secretions and in polymorphonuclear leukocytes. Its role in host defense mechanisms related to the non-immune defense system has been definitively established. Lf has two identical iron-binding sites, far from each other (44.3 A) and magnetically non-interacting. Fe(III) ions are six-coordinated, with four donor atoms provided by protein sidechains (two Tyr, one His, one Asp) and two oxygen atoms from a bridged HCO(3)(-). This set of ligands provides an ideal coordination scheme for stable and reversible iron binding. Nuclear magnetic relaxation dispersion (NMRD) profiles of Lf are consistent with a closest distance for a single water hydrogen atom of 3.1 A. By looking at the X-ray structure of Lf (PDB ID code: 1BLF) we can locate two water oxygens at 3.95 and 4.27 A from each Fe(III), respectively. Temperature dependence data suggest that an important contribution to the overall paramagnetic contribution to the solvent water relaxation rate arises from one or more second sphere water molecules in slow exchange with the bulk. A decreasing value of the exchange rate is obtained, ranging from 1.2 to 0.7 micros in the observed temperature range (25-65 degrees C), with an activation enthalpy of 7.3+/-0.8 kJ mol(-1). The low exchange rate obtained from NMRD data can be explained by the observation that both water molecules are bound to several polar groups of the protein backbone and side chains. By increasing the pH from 6.5 to 12 two distinct titrations are observed, consistent with sequential removal of both water molecules.     

Amphipathic structure of theonellapeptolide-Id, a hydrophobic tridecapeptide lactone from the Okinawa marine sponge Theonella swinhoei

Theonellapeptolide-Id (TNLP), a cyclic tridecapeptide lactone, was crystallized from dimethylformamide-water solution. In the asymmetric unit, two peptide molecules were combined with solvent molecules, and the total molecular weight was over 3000 Dalton. The crystal structure including solvent molecules was finally determined at 0.80 A resolution using synchrotron radiation. The conformations of two independent molecules were similar to each other and were also similar to the previously reported structure (Doi, Ishida, Kobayashi, Deschamps and Flippen-Anderson, 1999, Acta Crystallogr Sect C, 55, 796-798). About 13 hydrated water molecules were found at disordered 19 sites; they were located at a certain region to avoid contact with aliphatic side-chains of peptolide in the crystal. The spatial disposition of the solvent molecules and peptides subsequently caused the formation of the amphipathic layer.     

Structure and refinement at 1.8 A resolution of the aspartic proteinase from Rhizopus chinensis

The structure of rhizopuspepsin (EC 3.4.23.6), the aspartic proteinase from Rhizopus chinensis, has been refined to a crystallographic R-factor of 0.143 at 1.8 A resolution. The positions of 2417 protein atoms have been determined with a root-mean-square (r.m.s.) error of 0.12 A. In the final model, the r.m.s. deviation from ideality for bond distances is 0.010 A, and for angle distances it is 0.034 A. During the course of the refinement, a calcium ion and 373 water molecules, of which 17 are internal, have been located. The active aspartate residues, Asp35 and Asp218, are involved in similar hydrogen-bonding interactions with neighboring residues and with several water molecules. One water molecule is located between the two carboxyl groups of the catalytic aspartate residues in a tightly hydrogen-bonded position. The refinement resulted in an unambiguous interpretation of the highly mobile "flap", a beta-hairpin loop region that projects over the binding pocket. Large solvent channels are formed when the molecules pack in the crystal, exposing the binding pocket and making it easily accessible. Intermolecular contacts involve mainly solvent molecules and a few protein atoms. The three-dimensional structure of rhizopuspepsin closely resembles other aspartic proteinase structures. A detailed comparison with the structure of penicillopepsin showed striking similarities as well as subtle differences in the active site geometry and molecular packing.