Molecular Modeling and Computational Analyses Suggests
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Structural Insight Into Marburg Virus Nucleoprotein-RNA Complex Formation
bioRxiv preprint doi: https://doi.org/10.1101/2021.07.13.452116; this version posted July 13, 2021. The copyright holder for this preprint (which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission. 1 Structural insight into Marburg virus nucleoprotein-RNA complex formation 2 3 Yoko Fujita-Fujiharu1,2,3, Yukihiko Sugita1,2,4, Yuki Takamatsu1,#, Kazuya Houri1,2,3, Manabu 4 Igarashi5, Yukiko Muramoto1,2,3, Masahiro Nakano1,2,3, Yugo Tsunoda1, Stephan Becker6,7, 5 Takeshi Noda1,2,3* 6 7 1 Laboratory of Ultrastructural Virology, Institute for Frontier Life and Medical Sciences, 8 Kyoto University, 53 Shogoin Kawahara-cho, Sakyo-ku, Kyoto 606-8507, Japan 9 2 Laboratory of Ultrastructural Virology, Graduate School of Biostudies, Kyoto University, 53 10 Shogoin Kawahara-cho, Sakyo-ku, Kyoto 606-8507, Japan 11 3 CREST, Japan Science and Technology Agency, 4-1-8 Honcho, Kawaguchi, Saitama 332- 12 0012, Japan 13 4 Hakubi Center for Advanced Research, Kyoto University, Kyoto, Japan. 14 5 Division of Epidemiology, International Institute for Zoonosis Control, Hokkaido University, 15 Sapporo 001-0020, Japan 16 6 Institute of Virology, University of Marburg, 35043 Marburg, Germany. 17 7 German Center for Infection Research (DZIF), Marburg-Gießen-Langen Site, University of 18 Marburg, 35043 Marburg, Germany. 19 20 # present address: Department of Virology I, National Institute of Infectious Diseases, Gakuen 21 4-7-1, Musashimurayama-city, Tokyo 208-0011, Japan 22 *correspondence to: [email protected] 23 24 bioRxiv preprint doi: https://doi.org/10.1101/2021.07.13.452116; this version posted July 13, 2021. -
Α/Β Coiled Coils 2 3 Marcus D
1 α/β Coiled Coils 2 3 Marcus D. Hartmann, Claudia T. Mendler†, Jens Bassler, Ioanna Karamichali, Oswin 4 Ridderbusch‡, Andrei N. Lupas* and Birte Hernandez Alvarez* 5 6 Department of Protein Evolution, Max Planck Institute for Developmental Biology, 72076 7 Tübingen, Germany 8 † present address: Nuklearmedizinische Klinik und Poliklinik, Klinikum rechts der Isar, 9 Technische Universität München, Munich, Germany 10 ‡ present address: Vossius & Partner, Siebertstraße 3, 81675 Munich, Germany 11 12 13 14 * correspondence to A. N. Lupas or B. Hernandez Alvarez: 15 Department of Protein Evolution 16 Max-Planck-Institute for Developmental Biology 17 Spemannstr. 35 18 D-72076 Tübingen 19 Germany 20 Tel. –49 7071 601 356 21 Fax –49 7071 601 349 22 [email protected], [email protected] 23 1 24 Abstract 25 Coiled coils are the best-understood protein fold, as their backbone structure can uniquely be 26 described by parametric equations. This level of understanding has allowed their manipulation 27 in unprecedented detail. They do not seem a likely source of surprises, yet we describe here 28 the unexpected formation of a new type of fiber by the simple insertion of two or six residues 29 into the underlying heptad repeat of a parallel, trimeric coiled coil. These insertions strain the 30 supercoil to the breaking point, causing the local formation of short β-strands, which move the 31 path of the chain by 120° around the trimer axis. The result is an α/β coiled coil, which retains 32 only one backbone hydrogen bond per repeat unit from the parent coiled coil. -
Topography of the Histone Octamer Surface: Repeating Structural Motifs Utilized in the Docking of Nucleosomal
Proc. Natl. Acad. Sci. USA Vol. 90, pp. 10489-10493, November 1993 Biochemistry Topography of the histone octamer surface: Repeating structural motifs utilized in the docking of nucleosomal DNA (histone fold/helix-strand-helix motif/parallel fi bridge/binary DNA binding sites/nucleosome) GINA ARENTS* AND EVANGELOS N. MOUDRIANAKIS*t *Department of Biology, The Johns Hopkins University, Baltimore, MD 21218; and tDepartment of Biology, University of Athens, Athens, Greece Communicated by Christian B. Anfinsen, August 5, 1993 ABSTRACT The histone octamer core of the nucleosome is interactions. The model offers strong predictive criteria for a protein superhelix offour spirally arrayed histone dimers. The structural and genetic biology. cylindrical face of this superhelix is marked by intradimer and interdimer pseudodyad axes, which derive from the nature ofthe METHODS histone fold. The histone fold appears as the result of a tandem, parallel duplication of the "helix-strand-helix" motif. This The determination of the structure of the histone octamer at motif, by its occurrence in the four dimers, gives rise torepetitive 3.1 A has been described (3). The overall shape and volume structural elements-i.e., the "parallel 13 bridges" and the of this tripartite structure is in agreement with the results of "paired ends of helix I" motifs. A preponderance of positive three independent studies based on differing methodolo- charges on the surface of the octamer appears as a left-handed gies-i.e., x-ray diffraction, neutron diffraction, and electron spiral situated at the expected path of the DNA. We have microscopic image reconstruction (4-6). Furthermore, the matched a subset of DNA pseudodyads with the octamer identification of the histone fold, a tertiary structure motif of pseudodyads and thus have built a model of the nucleosome. -
Chapter 6 Protein Structure and Folding
Chapter 6 Protein Structure and Folding 1. Secondary Structure 2. Tertiary Structure 3. Quaternary Structure and Symmetry 4. Protein Stability 5. Protein Folding Myoglobin Introduction 1. Proteins were long thought to be colloids of random structure 2. 1934, crystal of pepsin in X-ray beam produces discrete diffraction pattern -> atoms are ordered 3. 1958 first X-ray structure solved, sperm whale myoglobin, no structural regularity observed 4. Today, approx 50’000 structures solved => remarkable degree of structural regularity observed Hierarchy of Structural Layers 1. Primary structure: amino acid sequence 2. Secondary structure: local arrangement of peptide backbone 3. Tertiary structure: three dimensional arrangement of all atoms, peptide backbone and amino acid side chains 4. Quaternary structure: spatial arrangement of subunits 1) Secondary Structure A) The planar peptide group limits polypeptide conformations The peptide group ha a rigid, planar structure as a consequence of resonance interactions that give the peptide bond ~40% double bond character The trans peptide group The peptide group assumes the trans conformation 8 kJ/mol mire stable than cis Except Pro, followed by cis in 10% Torsion angles between peptide groups describe polypeptide chain conformations The backbone is a chain of planar peptide groups The conformation of the backbone can be described by the torsion angles (dihedral angles, rotation angles) around the Cα-N (Φ) and the Cα-C bond (Ψ) Defined as 180° when extended (as shown) + = clockwise, seen from Cα Not -
Stapled Peptides—A Useful Improvement for Peptide-Based Drugs
molecules Review Stapled Peptides—A Useful Improvement for Peptide-Based Drugs Mattia Moiola, Misal G. Memeo and Paolo Quadrelli * Department of Chemistry, University of Pavia, Viale Taramelli 12, 27100 Pavia, Italy; [email protected] (M.M.); [email protected] (M.G.M.) * Correspondence: [email protected]; Tel.: +39-0382-987315 Received: 30 July 2019; Accepted: 1 October 2019; Published: 10 October 2019 Abstract: Peptide-based drugs, despite being relegated as niche pharmaceuticals for years, are now capturing more and more attention from the scientific community. The main problem for these kinds of pharmacological compounds was the low degree of cellular uptake, which relegates the application of peptide-drugs to extracellular targets. In recent years, many new techniques have been developed in order to bypass the intrinsic problem of this kind of pharmaceuticals. One of these features is the use of stapled peptides. Stapled peptides consist of peptide chains that bring an external brace that force the peptide structure into an a-helical one. The cross-link is obtained by the linkage of the side chains of opportune-modified amino acids posed at the right distance inside the peptide chain. In this account, we report the main stapling methodologies currently employed or under development and the synthetic pathways involved in the amino acid modifications. Moreover, we report the results of two comparative studies upon different kinds of stapled-peptides, evaluating the properties given from each typology of staple to the target peptide and discussing the best choices for the use of this feature in peptide-drug synthesis. Keywords: stapled peptide; structurally constrained peptide; cellular uptake; helicity; peptide drugs 1. -
And Beta-Helical Protein Motifs
Soft Matter Mechanical Unfolding of Alpha- and Beta-helical Protein Motifs Journal: Soft Matter Manuscript ID SM-ART-10-2018-002046.R1 Article Type: Paper Date Submitted by the 28-Nov-2018 Author: Complete List of Authors: DeBenedictis, Elizabeth; Northwestern University Keten, Sinan; Northwestern University, Mechanical Engineering Page 1 of 10 Please doSoft not Matter adjust margins Soft Matter ARTICLE Mechanical Unfolding of Alpha- and Beta-helical Protein Motifs E. P. DeBenedictis and S. Keten* Received 24th September 2018, Alpha helices and beta sheets are the two most common secondary structure motifs in proteins. Beta-helical structures Accepted 00th January 20xx merge features of the two motifs, containing two or three beta-sheet faces connected by loops or turns in a single protein. Beta-helical structures form the basis of proteins with diverse mechanical functions such as bacterial adhesins, phage cell- DOI: 10.1039/x0xx00000x puncture devices, antifreeze proteins, and extracellular matrices. Alpha helices are commonly found in cellular and extracellular matrix components, whereas beta-helices such as curli fibrils are more common as bacterial and biofilm matrix www.rsc.org/ components. It is currently not known whether it may be advantageous to use one helical motif over the other for different structural and mechanical functions. To better understand the mechanical implications of using different helix motifs in networks, here we use Steered Molecular Dynamics (SMD) simulations to mechanically unfold multiple alpha- and beta- helical proteins at constant velocity at the single molecule scale. We focus on the energy dissipated during unfolding as a means of comparison between proteins and work normalized by protein characteristics (initial and final length, # H-bonds, # residues, etc.). -
Effect of Superhelical Structure on the Secondary Structure of DNA Rings
VOL. 5, PP. 691-696 (1967) Effect of Superhelical Structure on the Secondary Structure of DNA Rings DANIEL GLAUBIGER and JOHN E. HEARST, Departnient of Chemistry, University of California, Berkeley, California Synopsis A quantity, called the linking number, is defined, which specifies the total number of t,wists in a circular helix. The linking number is invariant under continuous deforma- tions of the ring and therefore enables one to calculate the influence of superhelical structures on the secondary helix of a circular molecule. The linking number can be determined by projecting the helix into a plane and counting strand crosses in the projection as described. For example, it has been shown that for each 180" twist in a left-handed superhelix, a right-handed 360" twist is removed from the secondary helix, thus allowing local unwinding. Introduction It is of interest to relate superhelical structure of helical molecules to their secondary structure.' By defining a quantity characteristic of two- stranded circular helical niolecules, related to the helical structure, and in- variant under continuous deformations of the molecule, we are able to evaluate the changes in helical structure brought about by the imposition of superhelical configurations on such molecules. The quantity of interest, called the linking number, is related to the number of turns/cycle for a circular helical molecule.* It will be shown that superhelical structures which are made from helical polymers con- tribute to this number and alter the contribution made by the secondary structure of the molecule to this number. This is made manifest as a change in the number of turns/cycle or as a change in the number of turns/ unit length. -
Influence of the Sequence-Dependent Flexure of DNA on Transcription in E.Coli
Volume 17 Number 22 1989 Nucleic Acids Research Influence of the sequence-dependent flexure of DNA on transcription in E.coli Christina M.Collis, Peter L.Molloy, Gerald W.Both and Horace R.Drew* CSIRO Division of Biotechnology, Laboratory for Molecular Biology, PO Box 184, North Ryde, NSW 2113, Australia Received August 11, 1989; Revised and Accepted October 20, 1989 ABSTRACT In order to study the effects of DNA structure on cellular processes such as transcription, we have made a series of plasmids that locate several different kinds of DNA structure (stiff, flexible or curved) near the sites of cleavage by commonly-used restriction enzymes. One can use these plasmids to place any DNA region of interest (e.g., promoter, operator or enhancer) close to certain kinds of DNA structure that may influence its ability to work in a living cell. In the present example, we have placed a promoter from T7 virus next to the special DNA structures; the T7 promoter is then linked to a gene for a marker protein (chloramphenicol acetyl transferase). When plasmids bearing the T7 promoter are grown in cells of E. coli that contain T7 RNA polymerase, the special DNA structures seem to have little or no influence over the activity of the T7 promoter, contrary to our expectations. Yet when the same plasmids are grown in cells of E. coli that do not contain T7 RNA polymerase, some of the DNA structures show a surprising promoter activity of their own. In particular, the favourable flexibility or curvature of DNA, in the close vicinity of potential -35 and -10 promoter regions, seems to be a significant factor in determining where E. -
X-Ray Scattering from the Superhelix in Circular DNA (Supercoiling/Diffraction from Solutions/Specific Linking Difference/Writhe Vs
Proc. Nati Acad. Sci. USA Vol. 80, pp. 741-744, February 1983 Biophysics X-ray scattering from the superhelix in circular DNA (supercoiling/diffraction from solutions/specific linking difference/writhe vs. twist) G. W. BRADY*, D. B. FEIN*, H. LAMBERTSONt, V. GRASSIANt, D. Foost, AND C. J. BENHAMt Institute, Troy, New York 12181; *Center for Laboratories and Research, New York State Department of Health, Albany, New York 12222; tRensselaer Polytechnic and tDepartment of Mathematics, University of Kentucky, Lexington, Kentucky 40506 Communicated by Bruno H. Zimm, October 25, 1982 ABSTRACT This communication presents measurements, creased the lower angle limit of resolution of the instrument made with a newly constructed position-sensitive detector, of the because the inner portion of the scattering curve was super- small-angle x-ray scattering from the first-order superhelix ofna- imposed on a risingbackground resultingfrom parasitic slit scat- tive COP608 plasmid DNA. This instrument measures intensities tering. In consequence, the resulting data could not be de- free of slit effects and provides good resolution in the region of smeared, so a direct comparison with theory was precluded. interest. The reported observations, made both in the presence This paper presents measurements of SAS from the first-or- and in the absence of intercalator, closely fit the scattering pat- der ccc DNA superhelix made with a new position-sensitive terns calculated for noninterwound helical first-order superhel- detector (PSD). The resulting profiles are free of slit effects, ices. These results are consistent with a toroidal helical structure permitting direct and unambiguous comparisons with theory. but not with interwound conformations. -
DNA-Mediated Self-Assembly of Gold Nanoparticles on Protein Superhelix
bioRxiv preprint doi: https://doi.org/10.1101/449561; this version posted October 22, 2018. The copyright holder for this preprint (which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is made available under aCC-BY-NC-ND 4.0 International license. DNA-mediated self-assembly of gold nanoparticles on protein superhelix Tao Zhang∗,y,z and Ingemar Andréy yDepartment of Biochemistry and Structural Biology & Center for Molecular Protein Science, Lund University, P.O. Box 124, SE-221 00 Lund, Sweden zCurrent address: Max-Planck-Institute for Intelligent Systems, Heisenbergstraße 3, D-70569 Stuttgart, Germany E-mail: [email protected] Abstract Recent advances in protein engineering have enabled methods to control the self- assembly of protein on various length-scales. One attractive application for designed proteins is to direct the spatial arrangement of nanomaterials of interest. Until now, however, a reliable conjugation method is missing to facilitate site-specific position- ing. In particular, bare inorganic nanoparticles tend to aggregate in the presence of buffer conditions that are often required for the formation of stable proteins. Here, we demonstrated a DNA mediated conjugation method to link gold nanoparticles with protein structures. To achieve this, we constructed de novo designed protein fibers based on previously published uniform alpha-helical units. DNA modification rendered gold nanoparticles with increased stability against ionic solutions and the use of com- plementary strands hybridization guaranteed the site-specific binding to the protein. The combination of high resolution placement of anchor points in designed protein assemblies with the increased control of covalent attachment through DNA binding 1 bioRxiv preprint doi: https://doi.org/10.1101/449561; this version posted October 22, 2018. -
The Generic Geometry of Helices and Their Close-Packed Structures
Theor Chem Acc (2010) 125:207–215 DOI 10.1007/s00214-009-0639-4 REGULAR ARTICLE The generic geometry of helices and their close-packed structures Kasper Olsen Æ Jakob Bohr Received: 23 May 2009 / Accepted: 9 September 2009 / Published online: 25 September 2009 Ó The Author(s) 2009. This article is published with open access at Springerlink.com Abstract The formation of helices is an ubiquitous 1 Introduction phenomenon for molecular structures whether they are biological, organic, or inorganic, in nature. Helical struc- Helical structures are common in chain molecules such as tures have geometrical constraints analogous to close- proteins, RNA, and DNA, e.g., a-helices and the A, B and Z packing of three-dimensional crystal structures. For helical forms of DNA. In this paper, we consider the packing of packing the geometrical constraints involve parameters idealized helices formed by a continuous tube with the such as the radius of the helical cylinder, the helical pitch purpose to calculate the constraints on such helices which angle, and the helical tube radius. In this communication, arise from close-packing and space filling considerations; the geometrical constraints for single helix, double helix, we consider single helical tubes, as well as sets of two and for double helices with minor and major grooves are identical helical tubes. It is found that the efficiency of the calculated. The results are compared with values from the use of space depends on the helical pitch angle, and the literature for helical polypeptide backbone structures, the optimum helical pitch angle is determined for single and a-, p-, 310-, and c-helices. -
Breaking Non-Native Hydrophobic Clusters Is the Rate-Limiting Step In
Shibasish Chowdhury Wei Zhang Breaking Non-Native Chun Wu Guoming Xiong Hydrophobic Clusters is the Yong Duan Rate-Limiting Step in the Department of Chemistry and Biochemistry, Folding of an Alanine-Based Center of Biomedical Research Excellence, Peptide University of Delaware, Newark, DE 19716 Received 13 March 2002; accepted 29 April 2002 Abstract: The formation mechanism of an alanine-based peptide has been studied by all-atom molecular dynamics simulations with a recently developed all-atom point-charge force field and the Generalize Born continuum solvent model at an effective salt concentration of 0.2M. Thirty-two simulations were conducted. Each simulation was performed for 100 ns. A surprisingly complex folding process was observed. The development of the helical content can be divided into three phases with time constants of 0.06–0.08, 1.4–2.3, and 12–13 ns, respectively. Helices initiate extreme rapidly in the first phase similar to that estimated from explicit solvent simulations. Hydrophobic collapse also takes place in this phase. A folding intermediate state develops in the second phase and is unfolded to allow the peptide to reach the transition state in the third phase. The folding intermediate states are characterized by the two-turn short helices and the transition states are helix–turn–helix motifs—both of which are stabilized by hydrophobic clusters. The equilibrium helical content, calculated by both the main-chain ⌽–⌿ torsion angles and the main-chain hydrogen bonds, is 64–66%, which is in remarkable agreement with experiments. After corrected for the solvent viscosity effect, an extrapolated folding time of 16–20 ns is obtained that is in qualitative agreement with experiments.