Solid-State NMR Study Reveals Collagen I Structural Modifications

Total Page:16

File Type:pdf, Size:1020Kb

Solid-State NMR Study Reveals Collagen I Structural Modifications Solid-state NMR Study Reveals Collagen I Structural Modifications of Amino Acid Side Chains upon Fibrillogenesis Paulo de Sa Peixoto, Guillaume Laurent, Thierry Azais, Gervaise Mosser To cite this version: Paulo de Sa Peixoto, Guillaume Laurent, Thierry Azais, Gervaise Mosser. Solid-state NMR Study Reveals Collagen I Structural Modifications of Amino Acid Side Chains upon Fibrillogenesis. Journal of Biological Chemistry, American Society for Biochemistry and Molecular Biology, 2013, 288 (11), pp.7528-7535. 10.1074/jbc.M112.390146. hal-01461409 HAL Id: hal-01461409 https://hal.archives-ouvertes.fr/hal-01461409 Submitted on 2 Oct 2018 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Copyright Solid-state NMR study reveals Collagen I structural modifications of amino acid side chains upon fibrillogenesis. Paulo De Sa Peixoto, Guillaume Laurent, Thierry Azaïs, Gervaise Mosser. Laboratoire de Chimie de la Matière Condensée de Paris, UMR7574-UPMC/CNRS/Collège de France, UPMC, 4 place Jussieu, 75005 PARIS, France. Running Title : fibrillogenesis of Collagen I studied by solid-state NMR To whom correspondence should be addressed: Gervaise Mosser, Laboratoire de Chimie de la Matière Condensée de Paris, UMR7574 UPMC/CNRS/Collège de France, 75005 Paris, France. E-mail: [email protected]. Tel: +33 144276553, Fax: +33 144276539. Key-Words: Collagen I; solid-state NMR; fibrillogenesis; random coiled side-chain chemical shift; imino acids Background : Collagen fibrillogenesis is a amino acids residues. Moreover, based on a fundamental process both in vivo and in 13C quantitative spectrum we estimate the vitro. percentage of residues implicated in each Results : Fibrillogenesis increases the equilibrium. Our data indicate that fibril heterogeneity of conformations of side formation greatly affects hydroxyproline and proline prolyl pucker ring conformation. chains amino acids, impacting 40% of Finally, we discuss the implication of these iminoacids. structural data and propose a model in which Conclusion : A temperature-induced- the attractive force of fibrillogenesis comes attractive force component comes from from a structural reorganization of 10% to significant amount of the collagen amino 15% of the amino acids. These results allow acids. us to further understand collagen's self- Significance: Brings new perspectives to assembling process and fibrillar structure. studies of collagen assembly and ____________________________________ interactions with other matrix molecules. Collagen I, the most abundant protein in human body, is a very long (300 nm) and thin (1.5 nm) SUMMARY protein. It is formed by three left-handed In vivo, collagen I, the major structural polypeptide chains super-coiled into a right- protein in human body, is found assembled handed helix. These polypeptide chains, into fibrils. In the present work, we study a composed of about 1040 amino acids each (1), high concentrated collagen sample in its are formed almost exclusively by repeats of soluble, fibrillar and denatured states using 1 13 three amino acid units -(Gly-X-Y) - where Gly one and two dimensional { H}- C solid-state n 13 is a glycine and X and Y can be any other amino NMR spectroscopy. We interpret C acid but often, in mammals, X is a proline and Y chemical shifts variations in terms of dihedral is a hydroxyproline (2). The collagen molecule angle conformation changes. Our data show has propensity to self-associate into fibrils that that fibrillogenesis increases the side chain further organize into hierarchical architectures and backbone structural complexity. both in vivo and in vitro (3, 4). Within those Nevertheless, only three to five rotameric units, collagen molecules are arranged equilibria are found for each amino acid longitudinally and laterally so as forming a residue indicating a relatively low structural crystal-like period called “D period” of 67 nm heterogeneity of collagen upon fibrillogenesis. evidenced both by X-ray diffraction (XRD) and Using side chain statistical data we calculate electron microscopy studies (5,6). So far, the equilibrium constants for a great number of 1 highest resolution obtained on the whole molecule by XRD is 5-11 Å (lateral and axial EXPERIMENTAL PROCEDURES resolution respectively) (5). High-resolution Sample purification and fibrillogenesis local structural data were obtained on several Collagen was prepared as already described (6). crystals of collagen-like peptide. However, due Collagen concentration was assessed by to the limited number of these crystals (~20 hydroxyproline titration (16) and purity was resolved structures currently in the PDB) data determined by SDS-PAGE electrophoresis. collected are far from representing the great Collagen stock solution (500 mM CH3COOH, diversity of -(Gly-X-Y)n- sequences present in pH=2.5) was dialyzed against HCl (3 mM, collagen I (7). 1H NMR has only shown pH=2.5) and concentrated to 410 mg.mL-1 by a moderate potential to solve collagen-like peptide centrifugation-filtration process using PES tubes structure because of many overlaps of the of 30 KDa cut-off (3000 g at 10°C, variable resonances (8). Moreover, up to now 13C NMR angle centrifuge EPENDORF 5702R™). The pH experiments did not display a sufficient spectral was further increased by exposing the acidic resolution to allow a clear distinction among the sample to ammonia vapors (30 w %) at 20°C for different amino acid carbon resonances (9, 10). 7 minutes. 2D solid state NMR spectra were NMR studies using specific residue labeling recorded 6 hours after the sample exposition to have given valuable information on dynamics ammonia and acquired during 6 hours. The (11, 12, 13). In order to deduce the backbone stability of the sample was checked by recording conformation, Saito H. et al have compared 13C 1D 13C spectra prior and after each 2D 1H-13C chemical shifts of fibrillar collagen with those experiments. The spectra were similar for each obtained on small triple helical peptides (9). condition. Finally, the “basic-pH” sample was Torchia et al. have compared native and centrifuged-filtrated in order to collect enough denatured resonances of collagen fragment CB2 liquid (~150 µl) to measure the pH with a pH (14). More recently, Zhu et al. have studied paper. The resulting pH was 8.5 ± 0.5. structural modifications of bovine cortical bone Denaturation of the sample was obtained by induced by dehydration (10). Even though all exposing the sample to a high power 1H these studies reveal important structural decoupling (ν(1H) = 60 kHz) for 16 hours. characteristics of collagen, many 13C chemical shifts were “hidden” due to a poor spectral NMR parameters resolution. Solid-state NMR analyses were performed on a In the present work, we have investigated, using Bruker Avance III 500 spectrometer at 11.7 T solid-state NMR, structural changes in collagen operating at 500.21 MHz for 1H and 125.79 at high concentrations in four different regimes: MHz for 13C. A Bruker Magic Angle Spinning three native conditions defined as (i) soluble at (MAS) double resonance probe was used with 7 acidic pH (pH 2.5; T = 20°C), (ii) and (iii) mm rotors spun at a frequency νMAS = 2.5 kHz fibrillar at basic pH (pH 8.5; T = 20°C and T = A BCU-X unit was used to regulate the 30°C), and a denatured condition (iv) (pH 8.5; T temperature between 20°C and 35°C. For all 1 13 = 35°C). This last sample was used as a experiments, t90( H) and t90( C) were 11 and 7 reference. We have observed spectrally resolved µs respectively. Relaxation delays of 1 and 3 s 1 13 13 1D and 2D { H}- C MAS spectra ( C typical for 1H and 13C respectively were sufficiently line width from 20 to 40 Hz). We have identified long to record quantitative spectra. 512 scans 13 side chains and backbone C chemical shifts were acquired for 13C single pulse-experiment, modifications upon fribillogenesis passing from 48 scans for the 2D {1H}-13C INEPT MAS acidic to basic pH. We have shown that one experiment. For all 13C spectra a low power given residue can adopt different conformations proton decoupling (4.5 kHz) was applied during along the molecule. We have interpreted our acquisition. The INEPT evolution delay (1.7 ms) 1 data in terms of side chain conformational was matched to an averaged JCH value of 145 modifications using statistical data from ref (15). Hz and the refocusing delay (1.1ms) was We have also quantified those structural matched in order to get the CH, CH2 and CH3 13 modifications by comparing the C chemical resonances similarly phased. 256 t1 transients shifts of denatured collagen to side chain were collected for 2D {1H}-13C INEPT spectra. structural library data. 1H and 13C chemical shifts were referenced (δ = 0 ppm) to TMS. No 13C signal was detected through a cross polarization (CP) MAS 2 experiment (contact time of 10ms, 440 scans and have been fitted (SD always inferior to 6% at pH a 1H decoupling of 40kHz). See SI section figure 8.5). 2. Assignment and fit RESULTS 1H and 13C chemical shifts assignments were Dense collagen I matrices were synthesized based on 2D {1H}-13C INEPT MAS spectra (Fig. through a two-step procedure making use of the 1, Fig. SI-1), and on previous works on a lyotropic properties of collagen molecules at collagen-like peptide (8) and native collagen I acidic pH and self-assembling properties at (9, 10, 17).
Recommended publications
  • POLYMER STRUCTURE and CHARACTERIZATION Professor
    POLYMER STRUCTURE AND CHARACTERIZATION Professor John A. Nairn Fall 2007 TABLE OF CONTENTS 1 INTRODUCTION 1 1.1 Definitions of Terms . 2 1.2 Course Goals . 5 2 POLYMER MOLECULAR WEIGHT 7 2.1 Introduction . 7 2.2 Number Average Molecular Weight . 9 2.3 Weight Average Molecular Weight . 10 2.4 Other Average Molecular Weights . 10 2.5 A Distribution of Molecular Weights . 11 2.6 Most Probable Molecular Weight Distribution . 12 3 MOLECULAR CONFORMATIONS 21 3.1 Introduction . 21 3.2 Nomenclature . 23 3.3 Property Calculation . 25 3.4 Freely-Jointed Chain . 27 3.4.1 Freely-Jointed Chain Analysis . 28 3.4.2 Comment on Freely-Jointed Chain . 34 3.5 Equivalent Freely Jointed Chain . 37 3.6 Vector Analysis of Polymer Conformations . 38 3.7 Freely-Rotating Chain . 41 3.8 Hindered Rotating Chain . 43 3.9 More Realistic Analysis . 45 3.10 Theta (Θ) Temperature . 47 3.11 Rotational Isomeric State Model . 48 4 RUBBER ELASTICITY 57 4.1 Introduction . 57 4.2 Historical Observations . 57 4.3 Thermodynamics . 60 4.4 Mechanical Properties . 62 4.5 Making Elastomers . 68 4.5.1 Diene Elastomers . 68 0 4.5.2 Nondiene Elastomers . 69 4.5.3 Thermoplastic Elastomers . 70 5 AMORPHOUS POLYMERS 73 5.1 Introduction . 73 5.2 The Glass Transition . 73 5.3 Free Volume Theory . 73 5.4 Physical Aging . 73 6 SEMICRYSTALLINE POLYMERS 75 6.1 Introduction . 75 6.2 Degree of Crystallization . 75 6.3 Structures . 75 Chapter 1 INTRODUCTION The topic of polymer structure and characterization covers molecular structure of polymer molecules, the arrangement of polymer molecules within a bulk polymer material, and techniques used to give information about structure or properties of polymers.
    [Show full text]
  • Ideal Chain Conformations and Statistics
    ENAS 606 : Polymer Physics Chinedum Osuji 01.24.2013:HO2 Ideal Chain Conformations and Statistics 1 Overview Consideration of the structure of macromolecules starts with a look at the details of chain level chemical details which can impact the conformations adopted by the polymer. In the case of saturated carbon ◦ backbones, while maintaining the desired Ci−1 − Ci − Ci+1 bond angle of 112 , the placement of the final carbon in the triad above can occur at any point along the circumference of a circle, defining a torsion angle '. We can readily recognize the energetic differences as a function this angle, U(') such that there are 3 minima - a deep minimum corresponding the the trans state, for which ' = 0 and energetically equivalent gauche− and gauche+ states at ' = ±120 degrees, as shown in Fig 1. Figure 1: Trans, gauche- and gauche+ configurations, and their energetic sates 1.1 Static Flexibility The static flexibility of the chain in equilibrium is determined by the difference between the levels of the energy minima corresponding the gauche and trans states, ∆. If ∆ < kT , the g+, g− and t states occur with similar probability, and so the chain can change direction and appears as a random coil. If ∆ takes on a larger value, then the t conformations will be enriched, so the chain will be rigid locally, but on larger length scales, the eventual occurrence of g+ and g− conformations imparts a random conformation. Overall, if we ignore details on some length scale smaller than lp, the persistence length, the polymer appears as a continuous flexible chain where 1 lp = l0 exp(∆/kT ) (1) where l0 is something like a monomer length.
    [Show full text]
  • Native-Like Mean Structure in the Unfolded Ensemble of Small Proteins
    B doi:10.1016/S0022-2836(02)00888-4 available online at http://www.idealibrary.com on w J. Mol. Biol. (2002) 323, 153–164 Native-like Mean Structure in the Unfolded Ensemble of Small Proteins Bojan Zagrovic1, Christopher D. Snow1, Siraj Khaliq2 Michael R. Shirts2 and Vijay S. Pande1,2* 1Biophysics Program The nature of the unfolded state plays a great role in our understanding of Stanford University, Stanford proteins. However, accurately studying the unfolded state with computer CA 94305-5080, USA simulation is difficult, due to its complexity and the great deal of sampling required. Using a supercluster of over 10,000 processors we 2Department of Chemistry have performed close to 800 ms of molecular dynamics simulation in Stanford University, Stanford atomistic detail of the folded and unfolded states of three polypeptides CA 94305-5080, USA from a range of structural classes: the all-alpha villin headpiece molecule, the beta hairpin tryptophan zipper, and a designed alpha-beta zinc finger mimic. A comparison between the folded and the unfolded ensembles reveals that, even though virtually none of the individual members of the unfolded ensemble exhibits native-like features, the mean unfolded structure (averaged over the entire unfolded ensemble) has a native-like geometry. This suggests several novel implications for protein folding and structure prediction as well as new interpretations for experiments which find structure in ensemble-averaged measurements. q 2002 Elsevier Science Ltd. All rights reserved Keywords: mean-structure hypothesis; unfolded state of proteins; *Corresponding author distributed computing; conformational averaging Introduction under folding conditions, with some notable exceptions.14 – 16 This is understandable since under Historically, the unfolded state of proteins has such conditions the unfolded state is an unstable, received significantly less attention than the folded fleeting species making any kind of quantitative state.1 The reasons for this are primarily its struc- experimental measurement very difficult.
    [Show full text]
  • CD of Proteins Sources Include
    LSM, updated 3/26/12 Some General Information on CD of Proteins Sources include: http://www.ap-lab.com/circular_dichroism.htm Far-UV range (190-250nm) Secondary structure can be determined by CD spectroscopy in the far-UV region. At these wavelengths the chromophore is the peptide bond, and the signal arises when it is located in a regular, folded environment. Alpha-helix, beta-sheet, and random coil structures each give rise to a characteristic shape and magnitude of CD spectrum. This is illustrated by the graph below, which shows spectra for poly-lysine in these three different conformations. • Alpha helix has negative bands at 222nm and 208nm and a positive one at 190nm. • Beta sheet shows a negative band at 218 nm and a positive one at 196 nm. • Random coil has a positive band at 212 nm and a negative one around 195 nm. The approximate fraction of each secondary structure type that is present in any protein can thus be determined by analyzing its far-UV CD spectrum as a sum of fractional multiples of such reference spectra for each structural type. (e.g. For an alpha helical protein with increasing amounts of random coil present, the 222 nm minimum becomes shallower and the 208 nm minimum moves to lower wavelengths ⇒ black spectrum + increasing contributions from green spectrum.) Like all spectroscopic techniques, the CD signal reflects an average of the entire molecular population. Thus, while CD can determine that a protein contains about 50% alpha-helix, it cannot determine which specific residues are involved in the helical portion.
    [Show full text]
  • Large-Scale Analyses of Site-Specific Evolutionary Rates Across
    G C A T T A C G G C A T genes Article Large-Scale Analyses of Site-Specific Evolutionary Rates across Eukaryote Proteomes Reveal Confounding Interactions between Intrinsic Disorder, Secondary Structure, and Functional Domains Joseph B. Ahrens, Jordon Rahaman and Jessica Siltberg-Liberles * Department of Biological Sciences, Florida International University, Miami, FL 33199, USA; [email protected] (J.B.A.); jraha001@fiu.edu (J.R.) * Correspondence: jliberle@fiu.edu; Tel.: +1-305-348-7508 Received: 1 October 2018; Accepted: 9 November 2018; Published: 14 November 2018 Abstract: Various structural and functional constraints govern the evolution of protein sequences. As a result, the relative rates of amino acid replacement among sites within a protein can vary significantly. Previous large-scale work on Metazoan (Animal) protein sequence alignments indicated that amino acid replacement rates are partially driven by a complex interaction among three factors: intrinsic disorder propensity; secondary structure; and functional domain involvement. Here, we use sequence-based predictors to evaluate the effects of these factors on site-specific sequence evolutionary rates within four eukaryotic lineages: Metazoans; Plants; Saccharomycete Fungi; and Alveolate Protists. Our results show broad, consistent trends across all four Eukaryote groups. In all four lineages, there is a significant increase in amino acid replacement rates when comparing: (i) disordered vs. ordered sites; (ii) random coil sites vs. sites in secondary structures; and (iii) inter-domain linker sites vs. sites in functional domains. Additionally, within Metazoans, Plants, and Saccharomycetes, there is a strong confounding interaction between intrinsic disorder and secondary structure—alignment sites exhibiting both high disorder propensity and involvement in secondary structures have very low average rates of sequence evolution.
    [Show full text]
  • Protein Folding and Structure Prediction
    Protein Folding and Structure Prediction A Statistician's View Ingo Ruczinski Department of Biostatistics, Johns Hopkins University Proteins Amino acids without peptide bonds. Amino acids with peptide bonds. ¡ Amino acids are the building blocks of proteins. Proteins Both figures show the same protein (the bacterial protein L). The right figure also highlights the secondary structure elements. Space Resolution limit of a light microscope Glucose Ribosome Red blood cell C−C bond Hemoglobin Bacterium 1 10 100 1000 10000 100000 1nm 1µm Distance [ A° ] Energy C−C bond Green Noncovalent bond light Glucose Thermal ATP 0.1 1 10 100 1000 Energy [ kcal/mol ] Non-Bonding Interactions Amino acids of a protein are joined by covalent bonding interactions. The polypep- tide is folded in three dimension by non-bonding interactions. These interactions, which can easily be disrupted by extreme pH, temperature, pressure, and denatu- rants, are: Electrostatic Interactions (5 kcal/mol) Hydrogen-bond Interactions (3-7 kcal/mol) Van Der Waals Interactions (1 kcal/mol) ¡ Hydrophobic Interactions ( 10 kcal/mol) The total inter-atomic force acting between two atoms is the sum of all the forces they exert on each other. Energy Profile Transition State Denatured State Native State Radius of Gyration of Denatured Proteins Do chemically denatured proteins behave as random coils? The radius of gyration Rg of a protein is defined as the root mean square dis- tance from each atom of the protein to their centroid. For an ideal (infinitely thin) random-coil chain in a solvent, the average radius 0.5 ¡ of gyration of a random coil is a simple function of its length n: Rg n For an excluded volume polymer (a polymer with non-zero thickness and non- trivial interactions between monomers) in a solvent, the average radius of gyra- 0.588 tion, we have Rg n (Flory 1953).
    [Show full text]
  • Helix-Coil Conformational Change Accompanied by Anisotropic–Isotropic Transition
    Polymer Journal, Vol.33, No. 11, pp 898—901 (2001) NOTES Helix-Coil Conformational Change Accompanied by Anisotropic–Isotropic Transition † Ning LIU, Jiaping LIN, Tao C HEN, Jianding CHEN, Dafei ZHOU, and Le LI Department of Polymer Science and Engineering, East China University of Science and Technology, Shanghai 200237, P. R. China (Received November 22, 2000; Accepted July 1, 2001) KEY WORDS Helix-Coil Transition / Liquid Crystal Polymer / Polypeptide / Anisotropic– Isotropic Transition / Polypeptides, particularly poly(γ-benzyl-L- limited study of this acid induced anisotropic–isotropic glutamate) (PBLG) and other glutamic acid ester transition has been reported.13, 14 The precise molecular polymers, have the ability to exist in α-helix, a well de- mechanism of the transition remains to be determined. fined chain conformation of long chain order and retain In the present work, the texture changes in the acid- such a structure in numerous organic solvents that sup- induced anisotropic–isotropic transition were studied port intramolecular hydrogen bonding.1, 2 If PBLG and by microscope observations and the corresponding related polypeptides are dissolved in a binary solvent molecular conformational changes were followed by IR mixture containing a non-helicogenic component such measurements. The effect of the polymer concentra- as dichloroacetic acid (DCA) or trifluoroacetic acid tion was studied. According to the information gained (TFA), they can undergo a conformational change from through the experiment, the molecular mechanism with the α-helix to random coil form due to the changes respect to the acid-induced helix-coil conformational in solvent composition, temperature or both.3, 4 The change was suggested.
    [Show full text]
  • Native-Like Secondary Structure in a Peptide From
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Research Paper 473 Native-like secondary structure in a peptide from the ␣-domain of hen lysozyme Jenny J Yang1*, Bert van den Berg*, Maureen Pitkeathly, Lorna J Smith, Kimberly A Bolin2, Timothy A Keiderling3, Christina Redfield, Christopher M Dobson and Sheena E Radford4 Background: To gain insight into the local and nonlocal interactions that Addresses: Oxford Centre for Molecular Sciences contribute to the stability of hen lysozyme, we have synthesized two peptides and New Chemistry Laboratory, University of Oxford, South Parks Road, Oxford OX1 3QT, UK. that together comprise the entire ␣-domain of the protein. One peptide (peptide Present addresses: 1Department of Molecular 1–40) corresponds to the sequence that forms two ␣-helices, a loop region, and Physics and Biochemistry, Yale University, 266 a small ␤-sheet in the N-terminal region of the native protein. The other (peptide Whitney Avenue, PO Box 208114, New Haven, 84–129) makes up the C-terminal part of the ␣-domain and encompasses two CT 06520-8114, USA. 2Department of Chemistry ␣-helices and a 310 helix in the native protein. and Biochemistry, University of California, Santa Cruz, CA 96064, USA. 3Department of Chemistry, University of Illinois, 845 West Taylor Street, Results: As judged by CD and a range of NMR parameters, peptide 1–40 has Chicago, IL 60607-7061, USA. 4Department of little secondary structure in aqueous solution and only a small number of local Biochemistry and Molecular Biology, University of hydrophobic interactions, largely in the loop region.
    [Show full text]
  • Non-Covalent Interactions and How Macromolecules Fold
    Non-covalent interactions and how macromolecules fold Lecture 6: Protein folding and misfolding Dr Philip Fowler Objective: Restate how proteins fold First-year Biophysics course Examine the thermodynamics of how a protein folds. Determine what factors affect the stability of the folded, native structure. Resolve the Levinthal Paradox Investigate the role misfolded proteins play in disease Summary: Proteins are marginally stable We can study the folding of proteins using e.g. denaturants Proteins can be unfolded by changing pH and temperature or by adding denaturants The concept of the protein folding funnel dispenses with the Levinthal Paradox Misfolded proteins can form aggregates known as fibrils; prions are infectious proteins Protein folding unfolded, extended state compact molten globule folded, compact native state (random coil) more water—water clusters of non-covalent interactions fewer protein—water hydrogen bonds hydrogen bonds (can form form cooperatively complete network) ∆H > 0 ☹ ∆H < 0 ☺ ☺ native fold is less flexible protein than molten globule protein can adopt fewer ∆S < 0 ☹ ∆S < 0 ☹ conformations when a molten globule much less local ordering of the water from the perspective of the ∆H < 0 ☺ ∆H ≈ 0 solvent, there is little difference water between the molten globule and ∆S > 0 ☺ ☺ ∆S ≈ 0 the folded, native state The hydrophobic effect causes the extended polypeptide chain to collapse and form a compact but dynamic molten globule. Clusters of non-covalent interactions within the protein then form cooperatively. Thermodynamics of folding lysozyme at 25 °C DG = DH TDS unfolded, extended state − folded, compact native state ΔG = -60.9 kJ mol-1 TΔS = -175 kJ mol-1 ΔH = -236 kJ mol-1 How much lysozyme is unfolded? includes " includes " (a) protein—protein"☺ (a) increase in entropy of the water "☺ DG = RT lnK (b) protein—water " ☹ (b) decrease in the entropy of the protein ☹ − (c) water—water interactions ☺ K ~ 4.7 x 1010 i.e.
    [Show full text]
  • Molecular Dynamics of Folded and Disordered Polypeptides in Comparison with Nuclear
    Molecular Dynamics of Folded and Disordered Polypeptides in Comparison with Nuclear Magnetic Resonance Measurement Thesis Presented in Partial Fulfillment of the Requirements for the Degree Master of Science in the Graduate School of The Ohio State University By Lei Yu Graduate Program in Chemistry The Ohio State University 2018 Thesis Committee Rafael Brüschweiler, Advisor Sherwin Singer Copyrighted by Lei Yu 2018 2 Abstract With continuous increase in computer speed, molecular dynamics (MD) simulations have become a crucial biophysical method for the understanding of biochemical processes at atomic detail. However, current molecular mechanics force fields optimized for globular proteins often result in overly collapsed structures for intrinsically disordered proteins (IDPs). In order to study the relevant biological functions of IDPs, it is of great importance to utilize the appropriate force fields. Chemical shifts and J-coupling measurements from solution nuclear magnetic resonance (NMR) experiments serve as a common ground for force field assessment. Various combinations of protein force fields and water models were assessed by the direct comparison between back-calculated NMR parameters and experimental data. TIP4P-D water model was proven to improve the accuracy of back- calculation by producing more realistic dihedral angle ψ distributions. Amber99SBnmr1- ILDN and RSFF2+ force fields were shown to be optimal choices for tripeptide and IDP fragment simulations. The stability of the simulated two-helix bundle (THB) domain in the eukaryotic Na+/Ca2+ exchanger (NCX) suggested the transferable performance of Amber99SBnmr1-ILDN force field in company with TIP4P-D water model in folded proteins. Based on the assessment results, a research plan for future improvement of force fields by rebalancing dihedral angle distributions was proposed.
    [Show full text]
  • Spring 2012 Lecture 10-12
    CHM333 LECTURE 10 – 12: 2/4 – 2/11/13 SPRING 2013 Professor Christine Hrycyna Levels of Protein Structure: PRIMARY STRUCTURE (1°) - Defined, non-random sequence of amino acids along the peptide backbone o Described in two ways: § Amino acid composition § Amino acid sequence § M-L-D-G-C-G Peptide A § M-L-C-D-G-G Peptide B § Composition is IDENTICAL; Sequence is DIFFERENT - How to determine the COMPOSITION o Purify the protein of interest – separate away from all other types of proteins and biomolecules o Estimate the molecular weight of the protein o Establish the composition by complete hydrolysis of the protein under acidic conditions § Treat with 6M HCl at 110°C; 12-36 hours § Each peptide bond is broken and products are all of the free amino acids § Each amino acid is separated, identified and quantified § Final result: Know HOW MANY of each amino acid present in the original 66 CHM333 LECTURE 10 – 12: 2/4 – 2/11/13 SPRING 2013 Professor Christine Hrycyna - How to determine the ORDER o Determine the C-terminal amino acid § Use carboxypeptidase – enzyme that removes the last (C-terminal) amino acid in a free form by breaking the peptide bond • Hydrolyzes the peptide bond nearest the C-terminus o Identify the N-terminal amino acids in order § Process called SEQUENCING § Often difficult to characterize an intact protein § Instead, employ a “divide and conquer” approach to analyze peptide fragments of the intact protein § Cut large proteins into smaller parts § Use enzymes called PROTEASES • Cleave peptide bond in a specific way • TWO Examples:
    [Show full text]
  • Hydrolyzed Collagen—Sources and Applications
    molecules Review Hydrolyzed Collagen—Sources and Applications Arely León-López 1, Alejandro Morales-Peñaloza 2,Víctor Manuel Martínez-Juárez 1, Apolonio Vargas-Torres 1, Dimitrios I. Zeugolis 3,4 and Gabriel Aguirre-Álvarez 1,* 1 Instituto de Ciencias Agropecuarias, Universidad Autónoma del Estado de Hidalgo, Av. Universidad km 1. Ex Hacienda de Aquetzalpa. Tulancingo, Hidalgo 43600, Mexico; [email protected] (A.L.-L.); [email protected] (V.M.M.-J.); [email protected] (A.V.-T.) 2 Universidad Autónoma del Estado de Hidalgo, Escuela Superior de Apan, Carretera Apan-Calpulalpan s/n, Colonia, Chimalpa Tlalayote, Apan, Hidalgo 43920 Mexico; [email protected] 3 Regenerative, Modular & Developmental Engineering Laboratory (REMODEL), National University of Ireland Galway (NUI Galway), H91 TK33 Galway, Ireland; [email protected] 4 Science Foundation Ireland (SFI) Centre for Research in Medical Devices (CÚRAM) National University of Ireland Galway (NUI Galway), H91 TK33 Galway, Ireland * Correspondence: [email protected]; Tel.: +52-775-145-9265 Academic Editors: Manuela Pintado, Ezequiel Coscueta and María Emilia Brassesco Received: 7 October 2019; Accepted: 5 November 2019; Published: 7 November 2019 Abstract: Hydrolyzed collagen (HC) is a group of peptides with low molecular weight (3–6 KDa) that can be obtained by enzymatic action in acid or alkaline media at a specific incubation temperature. HC can be extracted from different sources such as bovine or porcine. These sources have presented health limitations in the last years. Recently research has shown good properties of the HC found in skin, scale, and bones from marine sources. Type and source of extraction are the main factors that affect HC properties, such as molecular weight of the peptide chain, solubility, and functional activity.
    [Show full text]