Molecular structure of flavocytochrome b2 at 2.4 A resolution

The crystal structure of flavocytochrome b2 has been solved at 3.0 A resolution by the method of multiple isomorphous replacement with anomalous scattering. Area detector data from native and two heavy-atom derivative crystals were used. The phases were refined by the B.C. Wang phase-filtering procedure utilizing the 67% (v/v) solvent content of the crystals. A molecular model was built first on a minimap and then on computer graphics from a combination of maps both averaged and not averaged about the molecular symmetry axis. The structure was extended to 2.4 A resolution using film data recorded at a synchrotron and refined by the Hendrickson-Konnert procedure. The molecule, a tetramer of Mr 230,000, is located on a crystallographic 2-fold axis and possesses local 4-fold symmetry. Each subunit is composed of two domains, one binding a heme and the other an FMN prosthetic group. In subunit 1, both the cystochrome and the flavin-binding domain are visible in the electron density map. In subunit 2 the cytochrome domain is disordered. However, in the latter, a molecule of pyruvate, the product of the enzymatic reaction, is bound at the active site. The cytochrome domain consists of residues 1 to 99 and is folded in a fashion similar to the homologous soluble fragment of cytochrome b5. The flavin binding domain contains a parallel beta 8 alpha 8 barrel structure and is composed of residues 100 to 486. The remaining 25 residues form a tail that wraps around the molecular 4-fold axis and is in contact with each remaining subunit. The FMN moiety, which is located at the C-terminal end of the central beta-barrel, is mostly sequestered from solvent; it forms hydrogen bond interactions with main- and side-chain atoms from six of the eight beta-strands. The interaction of Lys349 with atoms N-1 and O-2 of the flavin ring is probably responsible for stabilization of the anionic form of the flavin semiquinone and hydroquinone and enhancing the reactivity of atom N-5 toward sulfite. The binding of pyruvate at the active site in subunit 2 is stabilized by interaction of its carboxylate group with the side-chain atoms of Arg376 and Tyr143. Residues His373 and Tyr254 interact with the keto-oxygen atom and are involved in catalysis. In contrast, four water molecules occupy the substrate-binding site in subunit 1 and Tyr143 forms a hydrogen bond to the ordered heme propionate group. Otherwise the two flavin-binding domains are identical within experimental error.(ABSTRACT TRUNCATED AT 400 WORDS)     

P.versicolor龙虾D-甘油醛-3-磷酸脱氢酶的X射线晶体学研究——分子置换法结构测定

由P.versicolor龙虾尾肌提取的HOIO-D-甘油醛-3-磷酸脱氢酶(GAPDH),已长出可供Χ射线衍射用的晶体。初步Χ射线晶体学研究确定:此酶晶体属於C2空间群,不对称单位内含有半个分子,分子坐落在二重轴上。以Homarus Amercanus龙虾GAPDH结构为模型结构,应用分子置换技术进行了低分辨率Χ射线结构分析,结果表明:分子内亚基排列具有222对称性,分子Q轴平行于晶体学二重轴b,分子P和R轴分别平行于晶体学a和c轴。按分子置换法推出的结构模型算得5A分辨率的晶体学R因子为0.46。并获得了一套5A。分辨率的电子密度图。此酶的几种同晶型晶体,特别是荧光NAD衍生物晶体的较高分辨率的结构分析工作正在进行中。     

Structure of yeast hexokinase. 3. Low resolution structure of a second crystal form showing a different quaternary structure, heterologous interaction of subunits and substrate binding

A 7 Å resolution electron density map of a second crystal form (called BII) of yeast hexokinase B has been obtained. This crystal form, unlike the first crystal form (BI), binds nucleotide and sugar substrates. While the overall tertiary structure of each subunit appears to be largely the same in both crystal forms, the quaternary structure of the dimer is completely different in the two crystals. The two subunits in the crystallographic asymmetric unit of form BII are related by a molecular screw axis; that is, the two subunits are related by a 160 ° rotation and a 13 Å translation of one subunit relative to the other along the symmetry axis resulting in non-equivalent environments for the two chemically identical subunits. A deep cleft divides each subunit into two domains or lobes of roughly equal size. The helical regions which are clearly visible as rods of electron density in this map constitute at least 40 to 50% of the polypeptide chain and 70 to 80% of one of the lobes. At this resolution the molecule does not appear to be homologous in detail to other kinases such as phosphoglycerate kinase and adenylate kinase. Sugar substrates and inhibitors bind deeply in the cleft which separates the two lobes and produce substantial alterations in the protein structure.     

3D domain swapping modulates the stability of members of an icosahedral virus group

BACKGROUND: Rice yellow mottle virus (RYMV) is a major pathogen that dramatically reduces rice production in many African countries. RYMV belongs to the genus sobemovirus, one group of plant viruses with icosahedral capsids and single-stranded, positive-sense RNA genomes. RESULTS: The structure of RYMV was determined and refined to 2.8 A resolution by X-ray crystallography. The capsid contains 180 copies of the coat protein subunit arranged with T = 3 icosahedral symmetry. Each subunit adopts a jelly-roll beta sandwich fold. The RYMV capsid structure is similar to those of other sobemoviruses. When compared with these viruses, however, the betaA arm of the RYMV C subunit, which is a molecular switch that regulates quasi-equivalent subunit interactions, is swapped with the 2-fold-related betaA arm to a similar, noncovalent bonding environment. This exchange of identical structural elements across a symmetry axis is categorized as 3D domain swapping and produces long-range interactions throughout the icosahedral surface lattice. Biochemical analysis supports the notion that 3D domain swapping increases the stability of RYMV. CONCLUSIONS: The quasi-equivalent interactions between the RYMV proteins are regulated by the N-terminal ordered residues of the betaA arm, which functions as a molecular switch. Comparative analysis suggests that this molecular switch can also modulate the stability of the viral capsids.     

The optimization of protein-solvent interactions: thermostability and the role of hydrophobic and electrostatic interactions.

Protein-solvent interactions were analyzed using an optimization parameter based on the ratio of the solvent-accessible area in the native and the unfolded protein structure. The calculations were performed for a set of 183 nonhomologous proteins with known three-dimensional structure available in the Protein Data Bank. The dependence of the total solvent-accessible surface area on the protein molecular mass was analyzed. It was shown that there is no difference between the monomeric and oligomeric proteins with respect to the solvent-accessible area. The results also suggested that for proteins with molecular mass above some critical mass, which is about 28 kDa, a formation of domain structure or subunit aggregation into oligomers is preferred rather than a further enlargement of a single domain structure. An analysis of the optimization of both protein-solvent and charge-charge interactions was performed for 14 proteins from thermophilic organisms. The comparison of the optimization parameters calculated for proteins from thermophiles and mesophiles showed that the former are generally characterized by a high degree of optimization of the hydrophobic interactions or, in cases where the optimization of the hydrophobic interactions is not sufficiently high, by highly optimized charge-charge interactions.     

Structure of yeast hexokinase. II. A 6 angstrom resolution electron density map showing molecular shape and heterologous interaction of subunits

An electron density map of yeast hexokinase has been calculated at 6 Å resolution using six heavy atom derivatives. The map shows each of the enzyme's two 51,000 molecular weight subunits to consist of two separate lobes connected by a narrow bridge of density. Furthermore, these two subunits are related to each other in the asymmetric unit of the crystal by a quasi-2-fold rather than a true 2-fold axis. That is, they are related by a rotation of 180 ° plus a relative translation of 3.6 Å along the symmetry axis. This gives rise to a heterologous subunit interaction and a possibility of non-identical structure and function for these chemically identical subunits. The molecule is quite asymmetric, having dimensions of 150 Å × 45 Å × 55 Å. Each subunit is about 80 Å × 40 Å × 50 Å.A portion of an electron density map at 3 Å resolution has been also calculated, based on phases from two heavy atom derivatives. Polypeptide backbone and side chains are visible in this map.     

High resolution X-ray structure of yeast hexokinase,an allosteric protein exhibiting a non-symmetric arrangement of subunits

The structure determination of yeast hexokinase has been extended to 3.5 Å resolution for the dimer and to 2.7 Å resolution for the monomer using multiple isomorphous replacement. The electron density maps of both the monomer and dimer crystal forms have been substantially improved by an averaging procedure. From these maps the course of the polypeptide backbone and some aspects of the dimer interaction have been established.The hexokinase subunit arrangement is contrary to a major tenet of the Monod et al. (1965) theory of allosteric proteins which postulated that only symmetric or isologous interactions of subunits would occur in oligomeric proteins. One subunit of the dimer is related to the other by a 156 ° rotation about and a 13.8 Å translation along a molecular screw axis. In the hexokinase dimer the set of residues in one subunit that is interacting with the other subunit is different from the set of residues in the second subunit that is interacting with the first subunit. This heterologous or non-symmetric interaction of subunits is associated with some small differences in the structure of the two subunits, particularly at the subunit interface, and accounts for some of this enzyme's non-symmetric interactions with substrates and activators. Indeed, the non-symmetric subunit association may play an important role in the control of this enzyme's activity.The overall structure of hexokinase is considerably different than the known structures of the other enzymes in the glycolytic pathway. Although there is a striking similarity between the domain of hexokinase that binds AMP and the domain of lactate dehydrogenase that binds NAD, the former structure contains both antiparallel and parallel β-pleated strands, while the latter contains only parallel β-structure. In an attempt to assess the significance of this structural similarity, the structure of the nucleotide binding domains of hexokinase and lactate dehydrogenase are compared to a portion of carboxypeptidase A. The observed similarities among these structures suggests that a central β-pleated sheet flanked by α-helices is a common supersecondary structure that probably arose by convergent as well as divergent evolution. Thus, there appears to be no compelling evidence at this time to support the hypothesis that a part of hexokinase has evolved from the same gene as the dinucleotide binding domain of lactate dehydrogenase.     

Structure of the detergent phase and protein-detergent interactions in crystals of the wild-type (strain Y) Rhodobacter sphaeroides photochemical reaction center

Rhodobacter sphaeroides (strain Y) reaction center (RC) crystals were grown in the presence of n-octyl beta-glucoside (beta-OG). In order to determine the structure of the detergent phase in these crystals, low-resolution neutron diffraction experiments were performed at different contrasts obtained by varying the H2O/D2O ratio in the solvent. From the contrast variation data and from the RC atomic coordinates determined by X-ray diffraction [Arnoux, B., Ducruix, A., Reiss-Husson, F., Lutz, M., Norris, J., Schiffer, M., & Chang, C. H. (1989) FEBS Lett. 258, 47-50], a model was obtained for the structure of the detergent phase in the crystal. The detergent forms a ring-shaped micelle surrounding the most hydrophobic part of the transmembrane alpha helices of the RC. Each detergent ring is connected to two next-neighbor rings by intermicellar bridges. The detergent phase is organized thus in infinite zigzag chains parallel to the b axis of the P2(1)2(1)2(1) unit cell. The main interactions between beta-OG molecules and the RC molecules are hydrophobic and are localized at the level of the transmembrane alpha helices. This interaction replaces the phospholipid-protein interaction existing in vivo in the membrane and, to some extent, also the light harvesting complex-protein interaction. Secondary hydrophilic interactions are found between a few of the charged residues of the H subunit and the hydrophilic surface of the detergent ring from a neighboring RC molecule. A comparison with a previous study on Rhodopseudomonas viridis crystals [which grow in the presence of lauryldimethylamine N-oxide (LDAO) and belong to a different space group] [Roth, M., Lewit-Bentley, A., Michel, H., Deisenhofer, J., Huber, R., & Oesterhelt, D. (1989) Nature 340, 659-661] shows a quasi identity of shape and position of the beta-OG and LDAO rings around the transmembrane alpha helices. The secondary interactions, involving in both cases the external surface of the H subunit, differ because of the different molecular packing in the two space groups. The role and structural requirements of the detergent in the crystallization process are discussed.     

X-ray structure of lipoamide dehydrogenase from Azotobacter vinelandii determined by a combination of molecular and isomorphous replacement techniques

The crystal structure of lipoamide dehydrogenase from Azotobacter vinelandii has been determined by a combination of molecular replacement and isomorphous replacement techniques yielding eventually a good-quality 2.8 A electron density map. Initially, the structure determination was attempted by molecular replacement procedures alone using a model of human glutathione reductase, which has 26% sequence identity with this bacterial dehydrogenase. The rotation function yielded the correct orientation of the model structure both when the glutathione reductase dimer and monomer were used as starting model. The translation function could not be solved, however. Consequently, data for two heavy-atom derivatives were collected using the Hamburg synchotron facilities. The derivatives had several sites in common, which was presumably a major reason why the electron density map obtained by isomorphous information alone was of poor quality. Application of solvent flattening procedures cleaned up the map considerably, however, showing clearly the outline of the lipoamide dehydrogenase dimer, which has a molecular weight of 100,000. Application of the "phased translation function", which combines the phase information of both isomorphous and molecular replacement, led to an unambiguous determination of the position of the model structure in the lipoamide dehydrogenase unit cell. The non-crystallographic 2-fold axis of the dimer was optimized by several cycles of constrained-restrained least-squares refinement and subsequently used for phase improvement by 2-fold density averaging. After ten cycles at 3.5 A, the resolution was gradually extended to 2.8 A in another 140 cycles. The 2.8 A electron density distribution obtained in this manner was of much improved quality and allowed building of an atomic model of A. vinelandii lipoamide dehydrogenase. It appears that in the orthorhombic crystals used each dimer is involved in contacts with eight surrounding dimers, leaving unexplained why the crystals are rather fragile. Contacts between subunits within one dimer, which are quite extensive, can be divided into two regions separated by a cavity. In one of the contact regions, the level of sequence identity with glutathione reductase is very low but it is quite high in the other. The folding of the polypeptide chain in each subunit is quite similar to that of glutathione reductase, as is the extended conformation of the co-enzyme FAD.(ABSTRACT TRUNCATED AT 400 WORDS)     

Crystal structure of the 30 S ribosomal subunit from Thermus thermophilus: purification, crystallization and structure determination.

We describe the crystallization and structure determination of the 30 S ribosomal subunit from Thermus thermophilus. Previous reports of crystals that diffracted to 10 A resolution were used as a starting point to improve the quality of the diffraction. Eventually, ideas such as the addition of substrates or factors to eliminate conformational heterogeneity proved less important than attention to detail in yielding crystals that diffracted beyond 3 A resolution. Despite improvements in technology and methodology in the last decade, the structure determination of the 30 S subunit presented some very challenging technical problems because of the size of the asymmetric unit, crystal variability and sensitivity to radiation damage. Some steps that were useful for determination of the atomic structure were: the use of anomalous scattering from the LIII edges of osmium and lutetium to obtain the necessary phasing signal; the use of tunable, third-generation synchrotron sources to obtain data of reasonable quality at high resolution; collection of derivative data precisely about a mirror plane to preserve small anomalous differences between Bijvoet mates despite extensive radiation damage and multi-crystal scaling; the pre-screening of crystals to ensure quality, isomorphism and the efficient use of scarce third-generation synchrotron time; pre-incubation of crystals in cobalt hexaammine to ensure isomorphism with other derivatives; and finally, the placement of proteins whose structures had been previously solved in isolation, in conjunction with biochemical data on protein-RNA interactions, to map out the architecture of the 30 S subunit prior to the construction of a detailed atomic-resolution model.     

The absence of tertiary interactions in a self-assembled DNA crystal structure

DNA is a highly effective molecule for controlling nanometer-scale structure. The convenience of using DNA lies in the programmability of Watson-Crick base-paired secondary interactions, useful both to design branched molecular motifs and to connect them through sticky-ended cohesion. Recently, the tensegrity triangle motif has been used to self-assemble three-dimensional crystals whose structures have been determined; sticky ends were reported to be the only intermolecular cohesive elements in those crystals. A recent communication in this journal suggested that tertiary interactions between phosphates and cytosine N(4) groups are responsible for intermolecular cohesion in these crystals, in addition to the secondary and covalent interactions programmed into the motif. To resolve this issue, we report experiments challenging this contention. Gel electrophoresis demonstrates that the tensegrity triangle exists in conditions where cytosine-PO(4) tertiary interactions seem ineffective. Furthermore, we have crystallized a tensegrity triangle using a junction lacking the cytosine suggested for involvement in tertiary interactions. The unit cell is isomorphous with that of a tensegrity triangle crystal reported earlier. This structure has been solved by molecular replacement and refined. The data presented here leave no doubt that the tensegrity triangle crystal structures reported earlier depend only on base pairing and covalent interactions for their formation.     

Crystallographic study of turkey egg-white lysozyme and its complex with a disaccharide

The crystal structure of turkey egg-white lysozyme, determined by the molecular replacement method at 5 Å resolution (Bott & Sarma, 1976) has now been refined to 2.8 Å resolution and a model has been built to fit the electron density. A comparison of the co-ordinates with those of hen lysozyme indicate a rootmean-square deviation of 1.6 Å for all the main-chain and side-chain atoms. A significant difference is observed in the region of residues 98 to 115 of the structure. The molecules are packed in this crystal form with the entire length of the active cleft positioned in the vicinity of the crystallographic 6-fold axis and is not blocked by neighboring molecules. A difference electron density map calculated between crystals of turkey lysozyme soaked in a disaccharide of N-acetyl glucosamine—N-acetyl muramic acid and the native crystals showed a strong positive peak at subsite C, a weak positive peak at subsite D and two strong peaks that correspond to the subsite E and a new subsite F′. This new site F′ is different from the subsite F predicted for the sixth saccharide from model building in hen lysozyme. The interactions between the saccharides bound at subsites E and F′ and the enzyme molecules are discussed.     

Structure of satellite tobacco necrosis virus after crystallographic refinement at 2.5 Å resolution

The structure of the protein subunit of satellite tobacco necrosis virus has been solved at 3.7 Å resolution. We have now crystallographically refined the original model and extended the resolution to 2.5 Å in order to get a model accurate enough to explain the details of the subunit interactions. The refinement was done with a novel method utilizing the icosahedral symmetry of the virus particle.The final model shows a complicated network of interactions, involving salt linkages, hydrogen bonds and hydrophobic contacts. In addition, we have located three different metal ion sites in the protein shell, linking the protein subunits together. These sites are probably occupied by calcium ions. One site is found in a general position near the icosahedral 3-fold axis of the virus. The ligands form an octahedral arrangement, with two main chain carbonyl oxygens (O-61 and O-64), one carboxylate oxygen (OD1 from Asp194) of the same subunit and a second carboxylate oxygen (OE1 of Glu25) from a 3-fold related subunit. Two water molecules complete the octahedral arrangement. A second site is on the icosahedral 3-fold axis and is liganded by the carboxylate oxygens of the 3-fold related Asp55 residues. The third metal ion site is found on the 5-fold axis, liganded by the five carbonyl oxygens of Thr138 and two water molecules.We are unable to locate the first 11 N-terminal amino acid residues, which point into the virus interior. No interpretable density for RNA has been found, indicating that the nucleic acid of the virus does not have a unique orientation in the crystal.     

Structure of tropomyosin at 9 angstroms resolution.

We have used molecular replacement followed by a highly parameterized refinement to determine the structure of tropomyosin crystals to a resolution to 9 A. The shape, coiled-coil structure and interactions of the molecules in the crystals have been determined. These crystals have C2 symmetry with a = 259.7 A, b = 55.3 A, c = 135.6 A and beta = 97.2 degrees. Because of the unusual distribution of intensity in X-ray diffraction patterns from these crystals, it was possible to solve the rotation problem by inspection of qualitative aspects of the diffraction data and to define unequivocally the general alignment of the molecules along the (332) and (3-32) directions of the unit cell. The translation function was then solved by a direct search procedure, while electron microscopy of a related crystal form indicated the probable location of molecular ends in the asymmetric unit, as well as the anti-parallel arrangement. The structural model we have obtained is much clearer than that obtained previously with crystals of extraordinarily high solvent content and shows the two alpha-helices of the coiled coil over most of the length of the molecules and establishes the coiled-coil pitch at 140(+/- 10) A. Moreover, the precise value of the coiled-coil pitch varies along the molecule, probably in response to local variations in the amino acid sequence, which we have determined by sequencing the appropriate cDNA. The crystals are constructed from layers of tropomyosin filaments. There are two molecules in the crystallographic asymmetric unit and the molecules within a layer are bent into an approximately sinusoidal profile. Molecules in consecutive layers in the crystal lie at an angle relative to one another as found in crystalline arrays of actin and myosin rod. There are three classes of interactions between tropomyosin molecules in the spermine-induced crystals and these give some insights into the molecular interactions between coiled-coil molecules that may have implications for assemblies such as muscle thick filaments and intermediate filaments. In interactions within a layer, the geometry of coiled-coil contacts is retained, whereas in contacts between molecules in adjacent layers the coiled-coil geometry varies and these interactions instead appear to be dominated by the repeating pattern of charged zones along the molecule.     

The molecular and crystal structure of dextrans: a combined electron and X-ray diffraction study. II. A low temperature, hydrated polymorph

The crystal and molecular structure of a dextran hydrate has been determined through combined electron and X-ray diffraction analysis, aided by stereochemical model refinement. A total of 65 hk0 electron diffraction intensities were measured on frozen single crystals held at the temperature of liquid nitrogen, to a resolution limit of 1.6 A. The X-ray intensities were measured from powder patterns recorded from collections of the single crystals. The structure crystallizes in a monoclinic unit cell with parameters a = 25.71 A, b = 10.21 A, c (chain axis) = 7.76 A and beta = 91.3 degrees. The space group is P2(1) with b axis unique. The unit cell contains six chains and eight water molecules, with three chains of the same polarity and four water molecules constituting the asymmetric unit. Along the chain direction the asymmetric unit is a dimer residue; however, the individual glucopyranose residues are very nearly related by a molecular 2-fold screw axis. The conformation of the chain is very similar to that in the anhydrous structure, but the chain packing differs in the two structures in that the rotational positions of the chains about the helix axes (the chain setting angles) are considerably different. The chains still pack in the form of sheets that are separated by water molecules. The difference in the chain setting angles between the anhydrous and hydrate structures corresponds to the angle between like unit cell axes observed in the diffraction diagrams recorded from hybrid crystals containing both polymorphs. Despite some beam damage effects, the structure was determined to a satisfactory degree of agreement, with the residuals R'(electron diffraction) = 0.258 and R(X-ray) = 0.127.     

Control of crystal forms of apoferritin by site-directed mutagenesis

Surface charges of protein molecules are not only important to biological functions but also crucial to the molecular assembly responsible for crystallization. Appropriate alteration in the surface charge distribution of a protein molecule induces new molecular alignment in the proper direction in the crystal and, hence, controls the crystal form. Apoferritin molecules are known to crystallize in two- and three-dimensional forms in the presence of cadmium ions, which bridge neighboring protein molecules. Here we report a controlled transformation of the apoferritin 2-D crystal by site-directed mutagenesis. In mutant apoferritin, two amino acid residues binding a cadmium-ion through their negative charge, were replaced by one type of nonionic amino acid residues. The amino acid residues, Asp-84 and Gln-86 in the sequence of recombinant (i.e., wild-type) horse L -apoferritin, were replaced by Ser. The wild-type apoferritin yielded a hexagonal lattice 2-D crystal in the presence of cadmium ions. In contrast, the mutant apoferritin yielded two types of oblique crystals independent of the presence of cadmium ions. Image reconstruction of electron micrographs of the mutant crystals made clear that the mutant apoferritin molecules oriented themselves with the 2-fold symmetry axis perpendicular to the crystal plane in both crystals, while the wild-type apoferritin molecules oriented themselves with the 3-fold symmetry axis perpendicular to the crystal plane. The changes of crystal forms and molecular orientation in the 2-D crystals were well explained by a change of the electrostatic interactions induced by the mutagenesis. © 1995 Wiley-Liss, Inc.     

Model-building studies of Inovirus: genetic variations on a geometric theme

Inovirus (filamentous bacteriophage) is a simple system for studying the rules by which protein primary structure (amino acid sequence) controls secondary and higher order structure, and thereby function. The virus occurs naturally as a number of different strains with similar secondary and higher order structure, but the protein subunit that assembles to form the virion coat has quite different primary structures in different virus strains. Despite these differences in primary structure, the subunits of all strains have much the same size, about 50 residues, which are distributed by type in much the same way into three domains of primary structure: a collection of acidic residues in the N-terminal region, a hydrophobic domain of about 19 residues near the middle, and a collection of basic residues near the C-terminus. Each subunit can be closely approximated by an alpha-helix with its long axis roughly parallel to the fibre axis, sloping from large to small radius in the virion and interleaving between subunits in the next turn or level. The acidic residues near the N-terminus of the subunit face outwards on the virion surface, and explain the low isoelectric point of the virion; the basic residues near the C-terminus face inwards, where they neutralize the charge on the DNA at the core of the virion; and the hydrophobic central domain is involved in interactions which bind neighbouring subunits. Detailed X-ray fibre diffraction analysis of one strain gives the subunit structure. Comparative model-building studies of different strains illustrate the common structural principles.     

Analysis of maize alcohol dehydrogenase by native-SDS two dimensional electrophoresis and autoradiography

Summary Alcohol dehydrogenase isozyme proteins were characterized by visualization on two dimensional polyacrylamide gels. Native first dimension electrophoresis separates isozymes by size and charge, while preserving enzyme activity and subunit interactions. SDS electrophoresis in the second dimension breaks subunit interactions and separates polypeptides primarily by molecular weight. Results revealed that ADH2 monomers are larger in molecular weight than ADH1 monomers. An EMS induced Adhl mutant was found to produce ADH1 monomers of reduced molecular weight. Autoradiography revealed that only a few proteins (five or six) including ADH1 and ADH2 actively incorporate labelled amino acids after prolonged anaerobiosis.