Effect of nucleotides on the oligomeric state of human lactoferrin

Lactoferrin (LF) is a multifunctional acute-phase protein involved in nonspecific defense against bacteria, viruses, and cancer diseases and is present in human barrier fluids, blood, and milk. Small-angle X-ray scattering (SAXS) and light scattering (LS) demonstrated for the first time that LF occurs in the form of oligomers, with a high monomer unit number in the solution. The degree of LF oligomerization depends on the LF concentration and the storage period of non-frozen neutral LF solutions. The average inertial radius of scattering particles (R _g) reaches 100–450 Å at LF concentrations comparable with those in human milk, while R _g of LF monomers is 26.7 Å. LF forms complexes with various nucleotides and hydrolyzes them. The addition of ATP or AMP to LF solutions accelerates LF oligomerization and increases R _g to 600–700 Å, regardless of the initial degree of LF oligomerization. According to the different models (sphere, plate, and cylinder) of LF aggregates, its complexes with such R _g presumably contain several tens to thousands of LF monomers. The possible role of oligomeric complexes in multiple biological functions of LF is discussed.     

DNA and oligosaccharides stimulate oligomerization of human milk lactoferrin

Lactoferrin (LF) is a Fe³⁺-transferring glycoprotein and is contained in human barrier fluids, blood, and milk. LF is an acute phase protein, is involved in nonspecific defense, and displays a unique set of biological functions. Small-angle X-ray scattering and light scattering experiments demonstrated that DNA and oligosaccharides added to LF with various levels of initial oligomerization increased the oligomerization rate. Almost complete dissociation into monomers was observed when 1 M NaCl was added to LF oligomers obtained in the presence of DNA, oligosaccharides, and nucleotides, previously identified as oligomerization effectors. LF complexes obtained with different oligomerization effectors differed in stability. Incubation with 50 mM MgCl₂ completely destructed LF complexes formed in the presence of ATP and oligosaccharides but only partly destructed AMP- and d(pT)₁₀-dependent complexes, which was followed by the formation of new complexes with a higher salt stability. A possible role of oligomerization in various LF functions is discussed.     

Small-angle X-ray scattering of D-Ribulose-1,5-diphosphate carboxylase from Dasycladus clavaeformis roth (Ag.) in solution

D-Ribulose-1,5-diphosphate carboxylase from $\text{Dasycladus}$ was purified, and the gross dimensions were obtained by means of small-angle X-ray scattering measurements in solution. Dissolved single crystals of this enzyme (called “fraction I protein”) gave the same hydrodynamic parameters as the purified form. The molecular weight was found to be 535,000, and a radius of gyration of R_g = 45.5 Å was determined. The experimental scattering curves revealed a geometrical particle of D-Ribulose-1,5-diphosphate carboxylase with gross dimensions of that of a hollow sphere with outer radius of 56 Å and inner radius of 12 Å. Determinations of the diffusion coefficients lead to the conclusion that the enzyme has a spherical shape of almost uniform density.     

Characterization of group C meningococcal polysaccharide by light-scattering spectroscopy. III. Determination of molecular weight, radius of gyration, and translational diffusional coefficient.

Group-specific polysaccharides isolated by means of a cetavlon procedure are immunogenic in man and induce protective immunity against meningococcal meningitis. Minute quantities of the polymers in solution can act as vaccines. We now report the first characterization of a fractionated (C-1) group C polysaccharide in 0.4KM KCl and 0.05M sodium acetate by means of light-scattering spectroscopy. Independent measurements of refractive index increments, absolute scattered intensities, angular scattering intensities and line widths as a function of scattering angles and delay times at different concentrations using incident wavelengths of 632.8 nm from a He–Ne laser and of 488 nm from an argon–ion laser yield information on aggregation properties, molecular weight (M_r), radius of gyration 〈r⁰_g〉^1/2_z, translational diffusion coefficient 〈D〉⁰_z, and second virial coefficients A₂ and B₂ of C-1 polysaccharide. At relatively high ionic strength (0.04M KCl + 0.05M sodium acetate), we obtain for the C-1 polysaccharide in solution M_r = 5.15 × 10⁵, 〈r²_g〉^1/2_z = 345 Å, A₂ = 1.25 × 10^?4 ml/g, 〈D〉 = 1.16 × 10^?7 cm²/sec with a corresponding Stokes radius of 240 Å and B₂ = 4.4 ml/g. A₂ and B₂ are the second virial coefficients from intensity- and diffusion-coefficient measurements. The C-1 polysaccharide aggregates in solution and behaves hydrodynamically like random coils. Viscosity and sedimentation studies further confirm our conclusions that the fractioned C-1 polysaccharide aggregates in solution and EDTA can partially break up those aggregates. However, the system remains polydisperse even after adding an excess amount of EDTA. The weight-average molecular weight of the C-1 polysaccharide in solution depends upon ionic strength and exhibits a minimum at ～0.2M KCl. Finally, viscosity, light-scattering, and sedimentation results all show that the aggregated macromolecular system behaves like random-coiled polymers with no measurable shape factors.     

The molecular structure and solution conformation of an acidic heteropolysaccharide from Auricularia auricula-judae

A water soluble acidic heteropolysaccharide named WAF was isolated from Auricularia auricula‐judae by extracting with 0.9% NaCl solution. By using gas chromatography, gas chromatography‐mass spectrometry, and NMR, its chemical structure was determined to be composed of a backbone of α‐(1→3)‐linked D ‐mannopyranose residues with pendant side groups of β‐D ‐xylose, β‐D ‐glucose, or β‐D ‐glucuronic acid at position O6 or O2. Six fractions prepared from WAF with a weight‐average molecular mass (M_w) between 5.9 × 10⁴ and 64.7 × 10⁴ g/mol were characterized with laser light scattering and viscometry in 0.1M NaCl at 25°C. The dependence of intrinsic viscosity ([η]) and radius of gyration (R_g) on M_w for this polysaccharide were found to be [η] = 1.79 × 10^?3M_w^0.96 cm³ g^?1 and R_g = 6.99 × 10^?2 M_w^0.54 nm. The molar mass per unit contour length (M_L) and the persistence length (L_p) were estimated to be 1124 nm^?1 and 11 nm, respectively. The WAF exhibited a semirigid character typical of linear polysaccharides. Molecular modeling was then used to predict the ordered and disordered states of WAF; the simulated M_L and L_p were however much smaller than the experimental values. Taken altogether, the results suggested that WAF formed a duplex in solution. © 2010 Wiley Periodicals, Inc. Biopolymers 95: 217–227, 2011.     

Effect of the cations sodium,potassium and calcium on the interaction of hyaluronate chains: a light scattering and viscometric study

Light scattering and viscometric studies have been carried out on two preparations, A and B, of rooster comb hyaluronate. Sedimentation rate studies have also been performed with A. Light scattering measurements in 0.2 m KCl for preparation A gave a molecular weight of 3.3 × 10⁶ and for B, 1.0 × 10⁶. In (0.1–0.3) M NaCl similar measurements gave a particle weight for A of (4.4–6.4 × 10⁶ and for B (1.7–2.8 × 10⁶. In 0.066 m CaCl₂ molecular weight values of 9.5 × 10⁶ for A and 1.7 × 10⁶ for B were obtained. Thus in the presence of Na⁺ and Ca²⁺ ions aggregates of chains persisted into dilute solution. Measurements by light scattering on A and B in 4 m guanidinium chloride gave values in the same range as those obtained in 0.2 m KCl. Sedimentation rate studies on A gave values of 10.3 Svedbergs in 0.2 m KCl and 12.2 Svedbergs in 0.2 m NaCl and 0.066m CaCl₂. The shear dependence of the viscosity was studied using a conicylindrical viscometer at shear rates between 0.5 and 20 s^?1. Preparation A in 0.2 m KCl and NaCl yielded values for (ν_sp/cc→0 of 5000 and 7100 ml g^?1 respectively in keeping with the tendency to aggregate. The behaviour for preparation B was similar. In 0.066 m CaCl₂ there was a marked dependence of viscosity on shear speed below 10 s^?1 for all concentrations and the value of (ν_sp/c)→0 at 0 s^?1 for preparation A was 7700 ml g^?1 while at a shear rate of 8 s^?1 (ν_sp/c)c→0 ? 5000 ml g ^?1. Similar effects were found for preparation B and the data suggest associations of chains disruptable by weak shear forces. The increase in viscosity with concentration in the presence of 0.066 m CaCl₂ was much less than in the presence of KCl or NaCl, suggesting that the Ca²⁺ had a marked effect on the ”rigidity’ of the molecules in solution. A viscometric titration experiment with Ca^2? showed that a level of 0.02 m CaCl₂ in 0.2 m NaCl was sufficient to produce the change in viscosity presented above and that significant perturbations of the viscosity were present at 0.005?0.01 m CaCl₂.     

X-ray evidence of a native state with increased compactness populated by tryptophan-less B. licheniformis β-lactamase

β‐lactamases confer antibiotic resistance, one of the most serious world‐wide health problems, and are an excellent theoretical and experimental model in the study of protein structure, dynamics and evolution. Bacillus licheniformis exo‐small penicillinase (ESP) is a Class‐A β‐lactamase with three tryptophan residues located in the protein core. Here, we report the 1.7‐Å resolution X‐ray structure, catalytic parameters, and thermodynamic stability of ESP^ΔW, an engineered mutant of ESP in which phenylalanine replaces the wild‐type tryptophan residues. The structure revealed no qualitative conformational changes compared with thirteen previously reported structures of B. licheniformis β‐lactamases (RMSD = 0.4–1.2 Å). However, a closer scrutiny showed that the mutations result in an overall more compact structure, with most atoms shifted toward the geometric center of the molecule. Thus, ESP^ΔW has a significantly smaller radius of gyration (R_g) than the other B. licheniformis β‐lactamases characterized so far. Indeed, ESP^ΔW has the smallest R_g among 126 Class‐A β‐lactamases in the Protein Data Bank (PDB). Other measures of compactness, like the number of atoms in fixed volumes and the number and average of noncovalent distances, confirmed the effect. ESP^ΔW proves that the compactness of the native state can be enhanced by protein engineering and establishes a new lower limit to the compactness of the Class‐A β‐lactamase fold. As the condensation achieved by the native state is a paramount notion in protein folding, this result may contribute to a better understanding of how the sequence determines the conformational variability and thermodynamic stability of a given fold.     

On the subunit structure of crotoxin: hydrodynamic and shape properties of crotoxin, phospholipase A and crotapotin.

This paper reports physical-chemical properties of the subunit structure of crotoxin, phospholipase A and crotapotin. The native crotoxin has a sedimentation coefficient of 3S and a radius of gyration of R_g = 16.5 Å and a molecular weight of 30,900. Dissociation of the 3S particle results in two proteins of unequal size with sedimentation coefficients of 1.5 S (crotapotin) and 1S (phospholipase A). These dissociated species and the reconstituted complex were investigated by means of hydrodynamic methods including small angle X-ray scattering. The actual frictional ratios were obtained indicating that crotoxin is a sphere with a Stokes' radius of R_o = 22.5 Å and an axial ratio of 1:3, whereas phospholipase A, depending on the degree of association, has a radius of gyration of R_g = 32.4 Å and a high axial ratio of 1:14 for the monomer. Crotapotin has a radius of gyration of R_g = 12.4 Å, indicating an oblate ellipsoid of revolution of an axial ratio of 1:4. Evidently, the crotoxin complex consists of one highly asymmetric molecule (phospholipase A) and an oblate ellipsoid (crotapotin), which reconstitutes to a spherical 3S-particle (crotoxin).     

A structural mechanism for dimeric to tetrameric oligomer conversion in Halomonas sp. nucleoside diphosphate kinase

Nucleoside diphosphate kinase (NDK) is known to form homotetramers or homohexamers. To clarify the oligomer state of NDK from moderately halophilic Halomonas sp. 593 (HaNDK), the oligomeric state of HaNDK was characterized by light scattering followed by X‐ray crystallography. The molecular weight of HaNDK is 33,660, and the X‐ray crystal structure determination to 2.3 and 2.7 Å resolution showed a dimer form which was confirmed in the different space groups of R3 and C2 with an independent packing arrangement. This is the first structural evidence that HaNDK forms a dimeric assembly. Moreover, the inferred molecular mass of a mutant HaNDK (E134A) indicated 62.1–65.3 kDa, and the oligomerization state was investigated by X‐ray crystallography to 2.3 and 2.5 Å resolution with space groups of P2₁ and C2. The assembly form of the E134A mutant HaNDK was identified as a Type I tetramer as found in Myxococcus NDK. The structural comparison between the wild‐type and E134A mutant HaNDKs suggests that the change from dimer to tetramer is due to the removal of negative charge repulsion caused by the E134 in the wild‐type HaNDK. The higher ordered association of proteins usually contributes to an increase in thermal stability and substrate affinity. The change in the assembly form by a minimum mutation may be an effective way for NDK to acquire molecular characteristics suited to various circumstances.     

Light scattering and viscosity study of heat aggregation of insulin

Aggregation behavior and hydrodynamic parameters of insulin have been determined from static and dynamic light scattering experiments and intrinsic viscosity measurements carried out at pH 4.0, 7.5, and 9.0 in the temperature range 20–40°C in aqueous solutions. The protein aggregated extensively at elevated temperatures in the acidic solutions. Intermolecular interactions were found to be attractive and to increase with temperature. The measured intrinsic viscosity [η], diffusion coefficient D₀, molecular weight M, and radius of gyration R_g exhibited the universal behavior: M[η] = (2.4 ± 02) × 10⁻²⁷ (R_e,η/R_e,D)³(D_0η/T)⁻³ and (D₀√n)₋₁ ≃ (√6 πη₀ζβ/k_BT) [1 + 0.201)(v/β³)√n], where n is the number of segments in the polypeptide. The effective hydrodynamic radii deduced from [η], (R_e, η) and the same deduced from D₀, (R_e,D) showed a constant ratio, (R_e,η/R_e,D = 1.1 ± 0.1). R_e,D/R_g = ξ was found to be (0.76 ± 0.07). From the known solvent viscosity η₀, the segment length β was deduced to be (10 ± 1) Å. The excluded volume was deduced to be (5 Å)³ regardless of pH. The Flory-Huggins interaction parameter was found to be χ = 0.45 ± 0.04, independent of pH and temperature. © 1998 John Wiley & Sons, Inc. Biopoly 45: 1–8, 1998     

Chaperone‐client interactions between Hsp21 and client proteins monitored in solution by small angle X‐ray scattering and captured by crosslinking mass spectrometry

The small heat shock protein (sHsp) chaperones are important for stress survival, yet the molecular details of how they interact with client proteins are not understood. All sHsps share a folded middle domain to which is appended flexible N‐ and C‐terminal regions varying in length and sequence between different sHsps which, in different ways for different sHsps, mediate recognition of client proteins. In plants there is a chloroplast‐localized sHsp, Hsp21, and a structural model suggests that Hsp21 has a dodecameric arrangement with six N‐terminal arms located on the outside of the dodecamer and six inwardly‐facing. Here, we investigated the interactions between Hsp21 and thermosensitive model substrate client proteins in solution, by small‐angle X‐ray scattering (SAXS) and crosslinking mass spectrometry. The chaperone‐client complexes were monitored and the R_g‐values were found to increase continuously during 20 min at 45°, which could reflect binding of partially unfolded clients to the flexible N‐terminal arms of the Hsp21 dodecamer. No such increase in R_g‐values was observed with a mutational variant of Hsp21, which is mainly dimeric and has reduced chaperone activity. Crosslinking data suggest that the chaperone‐client interactions involve the N‐terminal region in Hsp21 and only certain parts in the client proteins. These parts are peripheral structural elements presumably the first to unfold under destabilizing conditions. We propose that the flexible and hydrophobic N‐terminal arms of Hsp21 can trap and refold early‐unfolding intermediates with or without dodecamer dissociation.     

Temperature effects on the hydrodynamic radius of the intrinsically disordered N‐terminal region of the p53 protein

Intrinsically disordered proteins (IDPs) are often characterized in terms of the hydrodynamic radius, R_h. The R_h of IDPs are known to depend on fractional proline content and net charge, where increased numbers of proline residues and increased net charge cause larger R_h. Though sequence and charge effects on the R_h of IDPs have been studied, the temperature sensitivity has been noted only briefly. Reported here are R_h measurements in the temperature range of 5–75°C for the intrinsically disordered N‐terminal region of the p53 protein, p53(1–93). Of note, the R_h of this protein fragment was highly sensitive to temperature, decreasing from 35 Å at 5°C to 26 Å at 75°C. Computer generated simulations of conformationally dynamic and disordered polypeptide chains were performed to provide a hypothesis for the heat‐induced compaction of p53(1–93) structure, which was opposite to the heat‐induced increase in R_h observed for a model folded protein. The simulations demonstrated that heat caused R_h to trend toward statistical coil values for both proteins, indicating that the effects of heat on p53(1–93) structure could be interpreted as thermal denaturation. The simulation data also predicted that proline content contributed minimally to the native R_h of p53(1–93), which was confirmed by measuring R_h for a substitution variant that had all 22 proline residues changed for glycine. Proteins 2014; 82:668–678. © 2013 Wiley Periodicals, Inc.     

Ions and osmolality on post‐thaw sperm motility activation of the endangered Brycon insignis (Characiformes)

The aim of this study was to evaluate the effects of osmolality and the presence of ions on the activation of post‐thaw sperm motility of Brycon insignis. Sperm was frozen under a standardized methodology for this species. In experiment 1, 11 solutions were prepared with reverse osmosis (RO) water (～0 mOsm/kg) and glucose or NaCl adjusted to an osmolality of 50, 100, 150, 200 and 250 mOsm/kg. In experiment 2, six solutions were prepared with RO and adjusted to ~100 mOsm/kg with one of the following chemicals: NaHCO₃, sodium citrate (Na₃C₆H₅O₇), NaCl, KCl, CaCl₂ or glucose (as ion‐free control). Post‐thaw sperm of both experiments was evaluated for motility rate, velocities (curvilinear = VCL, among others) and beat‐cross frequency (BCF). In experiment 1, sperm motility rate and velocities were higher (p < 0.05) when triggered in solutions at osmolalities from 0 to 200 mOsm/kg (62–80% motility; 139–167 µm/s) than that at 250 mOsm/kg (36–44% motility; 94–99 µm/s VCL). BCF was not affected by osmolality and varied from 19 to 24 Hz in all samples. In experiment 2, samples activated in NaHCO₃, citrate, NaCl and KCl solutions yielded higher motility rates (76–85%) and BCF (24–25 Hz) compared to those activated in CaCl₂ (50%; 14 Hz). Samples activated in ion‐free control solution yielded higher motility rate (87%) than those activated in NaHCO₃ and in CaCl₂. Curvilinear velocity was higher in samples activated in NaHCO₃, citrate, KCl and control solutions (144–160 µm/s) than in those activated in CaCl₂ (104 µm/s); samples activated in NaCl yielded intermediate VCL values (127 µm/s). Post‐thaw sperm achieves maximum motility rate and velocities when activated in solutions composed of sodium citrate, NaCl, KCl or glucose. Thus, post‐thaw sperm motility of B. insignis can be triggered in ionic and non‐ionic solutions at osmolality between 0 and 200 mOsm/kg. The use of solutions containing calcium, however, should be avoided.     

Small-angle x-ray scattering of bovine nasal cartilage proteoglycan in solution

The proteoglycan subunit (PGS) from bovine nasal cartilage was examined in water and in 0.15 N LiCl by small-angle x-ray scattering (SAXS). The molecular weight of 2.5 × 10⁶ and the radius of gyration, R_g = 493 Å, in 0.15 N LiCl, obtained by SAXS, are in good agreement with values reported by others for similar preparations. Values of the radius of gyration of the cross section, mass per unit length, and persistence length of the PGS are also reported. The low value of intrinsic viscosity ([η]) found in 0.15 N LiCl, and a comparison of the experimental distance distribution function to that of the theoretical distance distribution function for sphere, suggest that the PGS in salt solution approaches spherical symmetry. The much higher value of [η] in water suggests a prolate ellipsoid of low axial ratio.     

The association behavior of beta-lactamases in polyethylene glycol solution

The β-lactamases (EC 3.5.2.6) from Bacillus licheniformis 749/C, Enterobacter cloacae P99, and TEM plasmid RP4 are studied in 10–14% (w/v) polyethyleneglycol (PEG) 8000 solutions at pH 6.5 by x-ray scattering and in 18% PEG by equilibrium sedimentation. Although all three enzymes crystallize with twofold crystal symmetry from PEG 8000, it is not possible in this study to prove that dimerization occurs; however, both techniques give evidence for association above 1% (w/v) protein concentration. For the B. lichen., P99, and TEM enzymes, a dimerization of at most 0, 5, and 10% (v/v), respectively, account for the variation of radii of gyration R_g with concentration, after accounting for the effects of nonideality. Apparent R_g were 3–5% smaller in PEG solution than in PEG-free solution. Enhanced ordering of the molecules in PEG solution or the presence of a PEG-depleted hydration shell around the enzymes can account for the observation of reduced R_g values. Accordingly, values of the partial specific volume (defined at constant chemical potential of PEG) indicate considerable PEG exclusion and are consistent with the ability of high M_r PEGs to induce crystallization of these enzymes.     

Studies on deoxyribonucleoprotein structure. Small-angle X-ray scattering in solutions of various ionic strengths.

The cross-sectional radius of gyration of the deoxyribonucleoprotein (DNP) threads was measured by small-angle X-ray scattering in a wide range of ionic strengths (from 0.0005 to 2 M NaCl). For DNP in a solution of low ionic strength, this value is 30 Å. The increase of ionic strength results in partial deproteinization of DNP, while the cross-sectional radius of gyration varies from 25 Å for DNP in 0.7 M NaCl to 10 Å for DNP in 2 M NaCl. It is suggested that gradual deproteinization by the increase of NaCl concentration causes conformational changes, which are associated with the alteration of the DNP superstructure. The data are interpreted on the basis of the superhelical model of DNA packing in DNP; however, the coexistence of superhelical and unfolded regions in the DNP structure is also a possibility.     

Conformation of <Emphasis Type="Italic">Thermus thermophilus</Emphasis> ribosomal protein S1 in solution at different ionic strengths

Small-angle x-ray and neutron scattering were used to study the structure of the ribosomal protein S1 (61 kDa) from Thermus thermophilus in solution at low and moderate ionic strength (0 and 100 mM NaCl). The protein was found to be globular in both cases. Modeling of the S1 structure comprising six homologous domains on the basis of the NMR data for one domain showed that the best fit to scattering data was provided by compact domain packing. The calculated gyration radius was 28–29 Å, as typical of globular proteins about 60 kDa. The protein was prone to self-association, forming mainly dimers and trimers at moderate ionic strength and higher compact associates at low ionic strength. Neutron scattering assays in heavy water at 100 mM NaCl revealed markedly elongated associates. The translational diffusion coefficient calculated for S1 at 100 mM NaCl from dynamic light scattering was markedly lower than the one expected for its globular monomer (D _20,w = (2.7 ± 0.1)·10^?7 versus (5.8–6.0)·10^?7 cm² s^?1), confirming protein association under equilibrium conditions.     

Preliminary x-ray analysis of Escherichia coli GMP synthetase: Determination of anomalous scattering factors for a cysteinyl mercury derivative

We have initiated a project to determine the three-dimensional structure of GMP synthetase (GMPS) from Escherichia coli. GMPS catalyzes the conversion of XMP to GMP in the final step of de novo guanine nucleotide biosynthesis, and is a member of the glutamine amidotransferase family: a group of enzymes responsible for the assimilation of nitrogen into compounds such as amino acids, purine and pyrimidine bases, amino sugars, and antibiotics. The E. coli guaA gene encoding GMPS was cloned into a tac expression vector, overexpressed, and its gene product purified. Conditions for the growth of protein crystals were developed using recombinant GMPS in the presence of MgCl₂, ATP, and XMP. The crystals are monoclinic, space group P2₁, with cell parameters of a = 156.0 Å, b = 102.0 Å, c = 78.8 Å, β= 96.7°. Diffraction data to 2.8 Å spacings were collected on a Xuong-Hamlin area detector with an overall R_sym of 5.2%. Both the volume of the unit cell and the peaks in the self-rotation function are consistent with one GMPS tetramer of D₂ symmetry in the crystallographic asymmetric unit. Previously, GMPS has been observed only as a dimer in solution. GMPS was covalently modified with p-chloromercuribenzylsulfonic acid (PCMBS), and its X-ray fluorescence spectrum was measured through the L_III absorption edge of mercury Anomalous scattering factors for cysteinyl mercury were derived from this spectrum, and the feasibility of structure determination by multi-wavelength anomalous diffraction was evaluated. The optimal MAD dispersive signal is 4.5% of |F|, and the optimal MAD Bijvoet signal is 7.5% of |F| at a concentration of approximately 1 mercury per 10-kDa protein. The anomalous scattering factors tabulated here should be transferable to cysteinyl mercury in other proteins. © 1994 John Wiley & Sons, Inc.     

Conformation of mucous glycoproteins in aqueous solvents

Light-scattering techniques have been used to measure the z-average radius of gyration R_g z-average translational diffusion coefficient D_t and weight–average molecular weight M_w of porcine submaxillary mucin (PSM) in solution. PSM isolated at low shear in the presence of protease inhibitors has a M_w about twice as large as a sample prepared without these precautions. The former sample has a M_w of 17 × 10⁶ in 0.1M NaCl, which decreases to 8 × 10⁶ in 6M guanidine hydrochloride (GdnHCl) and then to 2 × 10⁶ on addition of 0.1M mercaptoethanol to the 6M GdnHCl solution. The R_g or D values obtained for PSM in this work superimpose with those of other authors for different mucin glycoproteins, leading to linear log–log relationships to the molecular weight of the protein core. Comparison of these results with those in the literature for denatured proteins suggest that mucins are linear random coils in which the protein core is stiffened by the presence of the oligosaccharide side chains. The length of the oligosaccharides and the nature of the solvent have little effect on the extension of the protein core. This suggests that the stiffness of the protein core is maintained by steric repulsion of the residues at the beginning of the oligosaccharide chains.     

Refined structures of mouse P‐glycoprotein

The recently determined C. elegans P‐glycoprotein (Pgp) structure revealed significant deviations compared to the original mouse Pgp structure, which suggested possible misinterpretations in the latter model. To address this concern, we generated an experimental electron density map from single‐wavelength anomalous dispersion phasing of an original mouse Pgp dataset to 3.8 Å resolution. The map exhibited significantly more detail compared to the original MAD map and revealed several regions of the structure that required de novo model building. The improved drug‐free structure was refined to 3.8 Å resolution with a 9.4 and 8.1% decrease in R_work and R_free, respectively, (R_work = 21.2%, R_free = 26.6%) and a significant improvement in protein geometry. The improved mouse Pgp model contains ～95% of residues in the favorable Ramachandran region compared to only 57% for the original model. The registry of six transmembrane helices was corrected, revealing amino acid residues involved in drug binding that were previously unrecognized. Registry shifts (rotations and translations) for three transmembrane (TM)4 and TM5 and the addition of three N‐terminal residues were necessary, and were validated with new mercury labeling and anomalous Fourier density. The corrected position of TM4, which forms the frame of a portal for drug entry, had backbone atoms shifted >6 Å from their original positions. The drug translocation pathway of mouse Pgp is 96% identical to human Pgp and is enriched in aromatic residues that likely play a collective role in allowing a high degree of polyspecific substrate recognition.