Hyperconjugation Versus Intramolecular Hydrogen Bond: Origin of the Conformational Preference of Gaseous Glycine

Total Page:16

File Type:pdf, Size:1020Kb

Hyperconjugation Versus Intramolecular Hydrogen Bond: Origin of the Conformational Preference of Gaseous Glycine http://www.paper.edu.cn Chemical Physics Letters 370 (2003) 147–153 Hyperconjugation versus intramolecular hydrogen bond: origin of the conformational preference of gaseous glycine Weizhou Wang a, Xuemei Pu a, Wenxu Zheng a, Ning-Bew Wong b, Anmin Tian a,* a Faculty of Chemistry, Sichuan University, Chengdu, Sichuan 610064, PR China b Department of Biology and Chemistry, City University of Hong Kong, Kowloon, Hong Kong, PR China Received 11 November 2002; in final form 16 December 2002 Abstract Three experimentally detected low-energy conformers of gaseous glycine are selected as models to investigate the origin of the conformational preference of nonionized glycine, employing the atoms in molecules (AIM) and natural bond orbital (NBO) analysis methods. At the B3LYP/6-311++G(3d,3p) theory level, it is found that the importance of intramolecular hydrogen bond was overemphasized in the previous studies and it is hyperconjugation not intramo- lecular hydrogen bond that determines the order and relative energy of the conformers considered in this Letter. Ó 2003 Elsevier Science B.V. All rights reserved. 1. Introduction understanding of the ground state potential energy surface of glycine has proven to be a serious The simplest amino acid, glycine, H2NCH2 challenge to both experiment and electronic COOH, has three internal rotational degrees of structure theory [1–15]. Such an understanding is freedom in its nonionized state: the rotation of the very important because glycine can be regarded as hydroxyl group around the CAO bond, the rota- a prototype for other amino acids, peptides and tion around the CAC bond, and the rotation of proteins. the amino group around the CAN bond. This Previous theoretical calculations mainly focused leads to more than a dozen rotational conformers on the geometries and relative stability of all pos- [1–8] (three low-energy structures Ip, IIn and IIIn sible conformers of glycine [1–15]. The following are depicted in Fig. 1, and the nomenclature is intramolecular hydrogen bonds have been con- taken from [4]; p denotes the planar heavy-atom ventionally assumed to explain the relative stabil- arrangement while n stands for nonplanar heavy- ity of glycine conformers: intramolecular hydrogen atom arrangement). A complete and quantitative bond involving the amino hydrogen and the car- bonyl oxygen, intramolecular hydrogen bond in- volving the carboxylic acid hydrogen and the * Corresponding author. Fax: +86-028-85412907. amino nitrogen and intramolecular hydrogen E-mail address: [email protected] (A. Tian). bond that involves the carboxylic acid hydrogen 0009-2614/03/$ - see front matter Ó 2003 Elsevier Science B.V. All rights reserved. doi:10.1016/S0009-2614(03)00072-1 转载 中国科技论文在线 http://www.paper.edu.cn 148 W. Wang et al. / Chemical Physics Letters 370 (2003) 147–153 Fig. 1. Chemical structures and atomic numbering, the corresponding molecular graphs (small dots represent critical points) and some selected molecular orbitals for three glycine conformers Ip, IIn and IIIn, respectively. and the carbonyl group. For instance, the exis- It has been demonstrated recently that hypercon- tence of two equal NAHÁÁÁO H-bonds and one jugation, rather than steric repulsion, is the OAHÁÁÁO bond was suggested in Ip, which was primary cause that determines molecular confor- always regarded as the origin of Ip being the mation in simple organic molecules like ethane lowest-energy form of neutral glycine in the gas [16,17]. Broadly speaking, hydrogen bond belongs [1–15]. It was also stated that IIn has a single hy- to a kind of intermolecular hyperconjugative in- drogen bond between the hydroxyl hydrogen and teraction. In this Letter, we still separate them the amino nitrogen and IIIn has a hydrogen bon- customarily and treat of the subject from the two ded trans-carboxylic acid moiety and a bifurcated aspects, respectively. NAHÁÁÁO bond between the amino hydrogens and The low-energy conformers Ip and IIn of gly- the carbonyl oxygen. These conclusions were em- cine have been identified by microwave spectros- pirically made in terms of interatomic distances. It copy [9–13]. The third conformer (IIIn) has is surprising that almost in all of the studies so far recently been found in the Ar matrix at tempera- published on glycine the information provided by tures below 13 K [8,14]. In this Letter, we selected the electron distribution has been ignored. Elec- the three ÔtrueÕ conformers as models to undertake tron delocalization and its concomitant stabiliza- a detailed investigation on the origin of the con- tion is a natural feature of the molecular orbital formational preference of gaseous glycine. The approach to bonding. A useful chemical concept Ôglycine storyÕ is continued. for electron delocalization is hyperconjugation which is defined as the favourable interaction of a filled or partially filled orbital, typically a r orbi- 2. Computational details tal, with a nearby empty orbital. Hyperconjuga- tion rationalizes certain chemical phenomena in The relative stability and molecular properties terms of filled-orbital–empty-orbital interactions. of the structures under investigation were deter- 中国科技论文在线 http://www.paper.edu.cn W. Wang et al. / Chemical Physics Letters 370 (2003) 147–153 149 mined by the analytic gradient techniques em- However the stability order and the structures of ploying the hybrid density functional method the other glycine conformers depend on the level (DFT) with BeckeÕs three-parameter functional for of theory. For our selected three glycine con- exchange and the Lee, Yang and Parr correlation formers, the optimized structural parameters at the functional (B3LYP) [18,19]. The adequacy of B3LYP(MP2)/aug-cc-pVDZ level of theory have density functional methods for the study of the been reported previously to be in excellent agree- conformational behavior of glycine and other ment with available experimental data [8]. Our amino acids has been the subject of several studies results at the B3LYP/6-311++G(3d,3p) level are [7,8,20,21]. The results obtained have shown that almost the same as those obtained at the the hybrid methods, in particular the B3LYP B3LYP(MP2)/aug-cc-pVDZ level of theory. The method [7,8,20], provide very similar structural energy difference is 0.48 kcal molÀ1 between Ip and parameters and relative stabilities compared IIn and 1.62 kcal molÀ1 between Ip and IIIn. The with MP2 formalism. The standard PopleÕs torsion angle, NCC@O, is )179.35° for IIn and 6-311++G(3d,3p) basis set was used in conjunc- )178.27° for IIIn. It is notable that the deviation tion with the DFT method [22]. The three con- from the planarity of heavy-atom arrangement is formers are all confirmed as true minima on the very small for conformers IIn and IIIn. potential energy surface of gaseous glycine by the presence of only real frequencies after the 3.2. AIM topological analysis of the electronic corresponding vibrational analysis. density The bonding characteristics of the different conformers were analyzed by using the Ôatoms in Recently, the rigorous AIM theory has been moleculesÕ (AIM) theory of Bader [23], which is successfully applied in characterizing hydrogen based on a topological analysis of the electron bonds of different strengths in a wide variety of charge density and its Laplacian. The AIM theory molecular complexes [27,28]. Popelier proposed a has proved itself a valuable tool to conceptually set of criteria for the existence of H-bonding within define what is an atom, and above all what is a the AIM formalism [27,28]. The most prominent bond in a quantum calculation of a molecular evidence of hydrogen bonding is the existence of a structure. The analysis went further with those bond path, containing a bond critical point (BCP) obtained by means of the natural bond obital between the donor hydrogen nucleus and the ac- (NBO) theory of Weihnhold and co-workers [24]. ceptor. The molecular graphs (the ensemble of The NBO analysis will allow us quantitatively bond paths connecting atoms) of the three con- evaluating the above mentioned hyperconjugative formers can be visualized in Fig. 1. Only one reg- interactions and intramolecular hydrogen bonds ular hydrogen bond between N5 and H6AO2 in which would be responsible for the origin of the conformer IIn is found. Table 1 shows the most conformational preference. significant topological local properties at the bond All the calculations were performed using critical points ð3; À1Þ for conformers Ip, IIn and GAUSSIAN 98 program package [25]. The molec- IIIn. The bond lengths are also included. It is ular graphs were generated with the AIM2000 clearly seen from Table 1 that the values of electron (Version 1.0) program [26]. density and Laplacian at N5 ÁÁÁH6 BCP in con- former IIn are also the hydrogen bond type (q 10À2 a.u. and positive r2q). Table 1 also 3. Results and discussion highlights that the OAH bond length in conformer IIn is longer than that in conformer Ip or IIIn, 3.1. Structure and energetics which comes about as a result of the formation of intramolecular hydrogen bond. The formation of All calculations have been consistent in pre- intramolecular hydrogen bond results in the exis- dicting that conformer Ip is the stablest form tence of ring critical point. No other intramolecular among all the conformers of gaseous glycine. hydrogen bond in the three conformers is found. 中国科技论文在线 http://www.paper.edu.cn 150 Table 1 Bond length (in AA)and topological properties (in a.u.) of the electronic charge density at the corresponding bond critical points of glycine conformers Ip, IIn and IIIna Bond Ip IIn IIIn d q r2qe ndq r2qe ndq r2qe n C1AO2 1.203 0.4339 )0.6629 0.1012 1.402 1.338 0.3137 )0.7363 0.0200 0.981 1.354 0.3009 )0.7015 0.0018 0.946 C1AO3 1.354 0.3015 )0.7113 0.0002 0.941 1.201 0.4371 )0.6805 0.1167 1.406 1.204 0.4341 )0.6821 0.1038 1.405 C1AC4 1.523 0.2521 )0.5744 0.1033 0.964 1.536 0.2481 )0.5498 0.1033 0.954 1.526 0.2502 )0.5663 0.1075 0.967 C4AH7 1.092 0.2821 )0.9627 0.0351 0.933 1.090 0.2839 )0.9730 0.0378 0.945 1.091 0.2832 )0.9719 0.0386 0.932 C4AH8 1.092 0.2821 )0.9627 0.0351 0.933 1.090 0.2838 )0.9727 0.0375 0.944 1.092 0.2827 )0.9681 0.0384 0.931 W.
Recommended publications
  • 2.#Water;#Acid.Base#Reac1ons
    8/24/15 BIOCH 755: Biochemistry I Fall 2015 2.#Water;#Acid.base#reac1ons# Jianhan#Chen# Office#Hour:#M#1:30.2:30PM,#Chalmers#034# Email:#[email protected]# Office:#785.2518# 2.1#Physical#Proper1es#of#Water# • Key$Concepts$2.1$ – Water#molecules,#which#are#polar,#can#form#hydrogen#bonds#with# other#molecules.# – In#ice,#water#molecules#are#hydrogen#bonded#in#a#crystalline#array,#but# in#liquid#water,#hydrogen#bonds#rapidly#break#and#re.form#in#irregular# networks.# – The#aTrac1ve#forces#ac1ng#on#biological#molecules#include#ionic# interac1ons,#hydrogen#bonds,#and#van#der#Waals#interac1ons.# – Polar#and#ionic#substances#can#dissolve#in#water.# (c)#Jianhan#Chen# 2# 1 8/24/15 2.1#Physical#Proper1es#of#Water# • Key$Concepts$2.1$ – The#hydrophobic#effect#explains#the#exclusion#of#nonpolar#groups#as#a# way#to#maximize#the#entropy#of#water#molecules.# – Amphiphilic#substances#form#micelles#or#bilayers#that#hide#their# hydrophobic#groups#while#exposing#their#hydrophilic#groups#to#water.# – Molecules#diffuse#across#membranes#which#are#permeable#to#them# from#regions#of#higher#concentra1on#to#regions#of#lower# concentra1on.# – In#dialysis,#solutes#diffuse#across#a#semipermeable#membrane#from# regions#of#higher#concentra1on#to#regions#of#lower#concentra1on.# (c)#Jianhan#Chen# 3# Human#Body#Mass#Composi1on# (c)#Jianhan#Chen# 4 2 8/24/15 Structure#of#Water# (c)#Jianhan#Chen# 5 Water#Hydrogen#Bonding# ~1.8 Å, 180o Acceptor Donor (c)#Jianhan#Chen# 6# 3 8/24/15 Typical#Bond#Energies# (c)#Jianhan#Chen# 7# Hydrogen#bond#networks#of#water/ice# (c)#Jianhan#Chen#
    [Show full text]
  • A New Way for Probing Bond Strength J
    A New Way for Probing Bond Strength J. Klein, H. Khartabil, J.C. Boisson, J. Contreras-Garcia, Jean-Philip Piquemal, E. Henon To cite this version: J. Klein, H. Khartabil, J.C. Boisson, J. Contreras-Garcia, Jean-Philip Piquemal, et al.. A New Way for Probing Bond Strength. Journal of Physical Chemistry A, American Chemical Society, 2020, 124 (9), pp.1850-1860. 10.1021/acs.jpca.9b09845. hal-02377737 HAL Id: hal-02377737 https://hal.archives-ouvertes.fr/hal-02377737 Submitted on 27 Mar 2021 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. A New Way for Probing Bond Strength Johanna Klein,y Hassan Khartabil,y Jean-Charles Boisson,z Julia Contreras-Garc´ıa,{ Jean-Philip Piquemal,{ and Eric H´enon∗,y yInstitut de Chimie Mol´eculaire de Reims UMR CNRS 7312, Universit´ede Reims Champagne-Ardenne, Moulin de la Housse 51687 Reims Cedex 02 BP39 (France) zCReSTIC EA 3804, Universit´ede Reims Champagne-Ardenne, Moulin de la Housse 51687 Reims Cedex 02 BP39 (France) {Sorbonne Universit´es,UPMC, Laboratoire de Chimie Th´eoriqueand UMR CNRS 7616, 4 Pl Jussieu, 75252 Paris Cedex 05(France) E-mail: [email protected] Phone: +33(3)26918497 1 Abstract The covalent chemical bond is intimately linked to electron sharing between atoms.
    [Show full text]
  • Bond Distances and Bond Orders in Binuclear Metal Complexes of the First Row Transition Metals Titanium Through Zinc
    Metal-Metal (MM) Bond Distances and Bond Orders in Binuclear Metal Complexes of the First Row Transition Metals Titanium Through Zinc Richard H. Duncan Lyngdoh*,a, Henry F. Schaefer III*,b and R. Bruce King*,b a Department of Chemistry, North-Eastern Hill University, Shillong 793022, India B Centre for Computational Quantum Chemistry, University of Georgia, Athens GA 30602 ABSTRACT: This survey of metal-metal (MM) bond distances in binuclear complexes of the first row 3d-block elements reviews experimental and computational research on a wide range of such systems. The metals surveyed are titanium, vanadium, chromium, manganese, iron, cobalt, nickel, copper, and zinc, representing the only comprehensive presentation of such results to date. Factors impacting MM bond lengths that are discussed here include (a) n+ the formal MM bond order, (b) size of the metal ion present in the bimetallic core (M2) , (c) the metal oxidation state, (d) effects of ligand basicity, coordination mode and number, and (e) steric effects of bulky ligands. Correlations between experimental and computational findings are examined wherever possible, often yielding good agreement for MM bond lengths. The formal bond order provides a key basis for assessing experimental and computationally derived MM bond lengths. The effects of change in the metal upon MM bond length ranges in binuclear complexes suggest trends for single, double, triple, and quadruple MM bonds which are related to the available information on metal atomic radii. It emerges that while specific factors for a limited range of complexes are found to have their expected impact in many cases, the assessment of the net effect of these factors is challenging.
    [Show full text]
  • Noncovalent Interactions Involving Microsolvated Networks of Trimethylamine N-Oxide
    University of Mississippi eGrove Electronic Theses and Dissertations Graduate School 2014 Noncovalent Interactions Involving Microsolvated Networks Of Trimethylamine N-Oxide Kristina Andrea Cuellar University of Mississippi Follow this and additional works at: https://egrove.olemiss.edu/etd Part of the Physical Chemistry Commons Recommended Citation Cuellar, Kristina Andrea, "Noncovalent Interactions Involving Microsolvated Networks Of Trimethylamine N-Oxide" (2014). Electronic Theses and Dissertations. 407. https://egrove.olemiss.edu/etd/407 This Thesis is brought to you for free and open access by the Graduate School at eGrove. It has been accepted for inclusion in Electronic Theses and Dissertations by an authorized administrator of eGrove. For more information, please contact [email protected]. NONCOVALENT INTERACTIONS INVOLVING MICROSOLVATED NETWORKS OF TRIMETHYLAMINE N-OXIDE Kristina A. Cuellar A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science Physical Chemistry University of Mississippi August 2014 Copyright © 2014 Kristina A. Cuellar All rights reserved. ABSTRACT This thesis research focuses on the effects of the formation of hydrogen-bonded networks with the important osmolyte trimethylamine N-oxide (TMAO). Vibrational spectroscopy, in this case Raman spectroscopy, is used to interpret the effects of noncovalent interactions by solvation with select hydrogen bond donors such as water, methanol, ethanol and ethylene glycol in the form of slight changes in vibrational frequencies. Spectral shifts in the experimental Raman spectra of interacting molecules are compared to the results of electronic structure calculations on explicit hydrogen bonded molecular clusters. The similarities in the Raman spectra of microsolvated TMAO using a variety of hydrogen bond donors suggest a common structural motif in all of the hydrogen bonded complexes.
    [Show full text]
  • Hydrogen Bond
    HYDROGEN BOND Hydrogen bond is not a real bond, actually it is a type of electrostatic attraction. It plays very important role in the case of water. So let’s learn more about it with the example of water molecule. You have studied bonding and hybridization of H2O molecule. H2O is a bent shaped molecule. There is a considerable electronegativity difference between H and O atoms which makes the H-O bond polar. More electronegative O pulls bonding pair of electrons and acquires a partial negative charge while Hydrogen develops a partial positive charge. When two molecules of water come closer, the electrostatic force comes in action. Partially negative charged Oxygen of one molecule attracts partially positive charged Hydrogen of another molecule by electrostatic attraction. Electron rich Oxygen shares its lone pair of electron with electron deficient Hydrogen atom and forms an invisible bond of attraction which is called Hydrogen bond. This electrostatic attraction isn’t sufficiently strong to form an ionic bond and the electrons are not shared enough to make it a coordinate covalent bond, but this attraction is somehow capable of keeping the molecules together. Hydrogen bond is represented by a dotted line. It is weaker than ionic and covalent bond. But it is solely responsible for the amazing nature of water. Let’s see how it makes water so wonderful. Hydrogen bonds make a network of water molecules which is responsible for the liquid state of water. When we try to evaporate water into vapours, we need to break a large number of hydrogen bonds to let water molecule free from the network.
    [Show full text]
  • Non-Covalent Short Range Interactions
    WORKSHOP Nanoscience on the Tip Non-Covalent Short Range Interactions Table of Contents: 1. Motivation ............................................................................................................ 1 2. Short Range Interactions and Surface Forces ...................................................... 1 3. Van der Waals Interactions for Point Interactions ............................................... 3 4. Surface Forces...................................................................................................... 4 5. Hamaker Constant................................................................................................ 5 6. Van der Waals Retardation Effects ...................................................................... 6 7. Adhesion and Surface Energies............................................................................ 6 8. Cutoff Distance for Van der Waals Calculations................................................. 7 9. Capillary Forces due to Vapor Condensation ...................................................... 8 10. Critical Humidity for Capillary Neck Formation................................................. 9 11. Estimation of the Tip Radius Utilizing the Capillary Effects ............................10 12. Modification of Hydrophobicity (Wettability)................................................... 12 13. Force Displacement Curves ............................................................................... 13 References ................................................................................................................
    [Show full text]
  • Interplay of Ring Puckering and Hydrogen Bonding In
    Article Cite This: J. Phys. Chem. A 2019, 123, 7087−7103 pubs.acs.org/JPCA Interplay of Ring Puckering and Hydrogen Bonding in Deoxyribonucleosides Published as part of The Journal of Physical Chemistry virtual special issue “Leo Radom Festschrift”. ‡ ‡ Siying Lyu, Nassim Beiranvand, Marek Freindorf, and Elfi Kraka* Computational and Theoretical Chemistry Group (CATCO), Department of Chemistry, Southern Methodist University, 3215 Daniel Ave, Dallas, Texas 75275-0314, United States *S Supporting Information ABSTRACT: The Cremer−Pople ring puckering analysis and the Konkoli−Cremer local mode analysis supported by the topological analysis of the electron density were applied for the first comprehensive analysis of the interplay between deoxy- ribose ring puckering and intramolecular H-bonding in 2′- deoxycytidine, 2′-deoxyadenosine, 2′-deoxythymidine, and 2′- deoxyguanosine. We mapped for each deoxyribonucleoside the complete conformational energy surface and the corresponding pseudorotation path. We found only incomplete pseudorotation cycles, caused by ring inversion, which we coined as pseudolibration paths. On each pseudolibration path a global and a local minimum separated by a transition state were identified. The investigation of H-bond free deoxyribonucleo- side analogs revealed that removal of the H-bond does not restore the full conformational flexibility of the sugar ring. Our work showed that ring puckering predominantly determines the conformational energy; the larger the puckering amplitude, the lower the conformational energy. In contrast no direct correlation between conformational energy and H-bond strength was found. The longest and weakest H-bonds are located in the local minimum region, whereas the shortest and strongest H-bonds are located outside the global and local minimum regions at the turning points of the pseudolibration paths, i.e., H-bonding determines the shape and length of the pseudolibration paths.
    [Show full text]
  • Transition Metal Activation and Functionalization of Carbon-Hydrogen Bonds
    FINAL REPORT SUBMITTED TO THE DEPARTMENT OF ENERGY BY University of Rochester River Campus Rochester, New York 14627 FOR TRANSITION METAL ACTIVATION AND FUNCTIONALIZATION OF CARBON-HYDROGEN BONDS William D. Jones, Principal Investigator Phone: 716-275-5493 Contract No. DE-FG02-86ER13569 Project Period: December 1, 1998 - November 30, 2001 Total Award Amount (3 years): $ 396,000 Unexpended Balance at End of Grant Period: $0 DOE Report, 1998-2001 2 William D. Jones Overview of Research Accomplishments for the Period Dec. 1, 1998-Nov. 30, 2001: These past 3 years, our research has focussed on the items presented in our proposal where we have had success. These include: (1) carbon-carbon bond cleavage reactions, (2) fundamental studies of C-H bond cleavage reactions of trispyrazolylboraterhodium complexes, (3) catalytic C-H and C-C bond functionalization, and (4) carbon-fluorine bond activation. We have made progress in each of these areas, as described in the following report, and will continue our studies in these areas. Our carbon-carbon bond cleavage study is based upon the notion that metal-phenyl bonds are the strongest metal-carbon bonds. Cleavage of the C-C bonds in biaryl systems will therefore give two very strong metal-aryl bonds, and consequently offers the most thermodynamically preferred situation for observing C-C cleavage. We have had extensive success in C-C cleavage with biphenylene, a molecule with a weaker C-C bond than biphenyl. The success includes not only several new nickel, palladium, and platinum based metal systems of the type [M(chelating phosphine)] but also related rhodium systems for C-C cleavage.
    [Show full text]
  • Electrostatic Potential Topology for Probing Molecular Structure, Bonding and Reactivity
    molecules Review Electrostatic Potential Topology for Probing Molecular Structure, Bonding and Reactivity Shridhar R. Gadre 1,* , Cherumuttathu H. Suresh 2,* and Neetha Mohan 2 1 Department of Chemistry, Interdisciplinary School of Scientific Computing, Savitribai Phule University, Pune 411007, India 2 Chemical Sciences and Technology Division, CSIR-National Institute for Interdisciplinary Science and Technology, Trivandrum 695019, India; [email protected] * Correspondence: [email protected] (S.R.G.); [email protected] (C.H.S.) Abstract: Following the pioneering investigations of Bader on the topology of molecular electron density, the topology analysis of its sister field viz. molecular electrostatic potential (MESP) was taken up by the authors’ groups. Through these studies, MESP topology emerged as a powerful tool for exploring molecular bonding and reactivity patterns. The MESP topology features are mapped in terms of its critical points (CPs), such as bond critical points (BCPs), while the minima identify electron-rich locations, such as lone pairs and π-bonds. The gradient paths of MESP vividly bring out the atoms-in-molecule picture of neutral molecules and anions. The MESP-based characterization of a molecule in terms of electron-rich and -deficient regions provides a robust prediction about its interaction with other molecules. This leads to a clear picture of molecular aggregation, hydrogen bonding, lone pair–π interactions, π-conjugation, aromaticity and reaction mechanisms. This review summarizes the contributions of the authors’ groups over the last three decades and those of the Citation: Gadre, S.R.; Suresh, C.H.; other active groups towards understanding chemical bonding, molecular recognition, and reactivity Mohan, N. Electrostatic Potential through topology analysis of MESP.
    [Show full text]
  • Hydrogen Bonds
    Hydrogen Bonds Hydrogen bonds have played an incredibly important role in the history of structural biology. Both the structure of DNA and of protein a-helices and b-sheets were predicted based largely on the hydrogen bonds these structures form. So understanding hydrogen bonds is clearly important, but much like the hydrophobic effect, hydrogen bonds are surprisingly complex and are not completely understood in every last detail. So take the things I will tell you with a grain of salt. The electrostatic nature of hydrogen bonds Hydrogen bonds are formed when an electronegative atom approaches a hydrogen atom bound to another electro-negative atom. The most common electro negative atoms in biochemical systems are oxygen (3.44) and nitrogen (3.04) while carbon (2.55) and hydrogen (2.22) are relatively electropositive (the electronegativity values are given on the Pauling scale, and don’t have a direct physical meaning). A gradient in electronegativity along a covalent bond results in the more electronegative ions pulling shared electrons towards themselves resulting in an electric dipole along the bond. One obvious result of this is that the two dipoles will attract one another in the type of simple electrostatic dipole-dipole interaction we learned about earlier in class. As you know this interaction falls off with 1/r3 so the interaction will only matter between nearest neighbors. This dipole-dipole interaction provides much of the source for a hydrogen bond’s energy. Lets see how much energy this type of interaction is worth. For example in a helix the dipole along the peptide bond is roughly +0.4 -0.4.
    [Show full text]
  • Fluorine in a C−F Bond As the Key to Cage Formation
    Angewandte Minireviews Chemie International Edition: DOI: 10.1002/anie.201710423 Fluorinated Cage Molecules German Edition: DOI: 10.1002/ange.201710423 Fluorine in a CÀF Bond as the Key to Cage Formation Maxwell Gargiulo Holl, Cody Ross Pitts, and Thomas Lectka* cage molecules · fluorine · hydrogen bonds · neighboring group effects · noncovalent interactions Cage molecules have long been employed to trap reactive or transient species, as their rigid nature allows them to enforce situations that otherwise would not persist. In this Minireview, we discuss our use of rigid cage structures to investigate the close noncovalent interactions of fluorine with other functional groups and determine how mutual proximity affects both physical properties and reactivity. Unusual Weak cages are exemplified by inter- covalent interactions of fluorine are also explored: the cage can close actions of the CÀF bond with C=C and to form the first solution-phase C-F-C fluoronium ion. C=O bonds, stronger cages are re- vealed by hydrogen bonding interac- tions (F···HO, F···HC); and a B···F 1. Introduction interaction is only predicted to form a cage in its transition state. The strongest cage is represented As the most electronegative element, fluorine usually gets by a symmetrical C-F-C fluoronium ion, in which the C-F-C its way with other atoms, much in the manner a wild cat gets interaction is highly covalent. A weak cage arises again in his way with prey. Once part of a CÀF bond, the fluorine atom novel aromatic substitution chemistry in which F interacts is tamed and has a much-diminished desire to interact with an aryl ring.
    [Show full text]
  • Hydrophobicity, Hydrophilicity
    Hydrophobicity, Hydrophilicity and Silanes Water, water everywhere is the refrain from the rhyme of the ancient mariner and a concern of every modern coatings technologist. hether decorative, protective are playing an increasing role in controlling the inter- or functional, coatings must action of water with a surface. contend with water in the Silanes are silicon chemicals that possess a hydrolyti- environment. A problem dis- cally sensitive center that can react with inorganic sub- tinct from the issue of wet strates such as glass to form stable covalent bonds and Wadhesion and hydrolytic stability of coatings is con- organic substitution that alters the physical interac- trolling the interaction of water with a coated surface. tions of treated substrates (Figure 1). Different than Very often the descriptors hydrophobic or hydrophilic most additives, which have a limited performance are applied to coated surfaces. Although the terms range, they can achieve surface properties ranging from hydrophobic and hydrophilic are casually used, they hydrophobic to hydrophilic. They may be a sole active are usually not defined. A growing number of applica- ingredient or a component in a coatings formulation, tions ranging from architectural coatings to aortic controlling the interaction of water over a broad spec- stents require a precise control and, therefore, precise trum of requirements. In order to understand how definition of substrate interaction with water. Silanes silanes can affect hydrophobicity and hydrophilicity, it is important to understand some of the fundamentals of Figure 1 | Silanes and surface modification. the interaction of water with surfaces. OCH 2CH 3 Water, Hydrophobicity CH 3CH 2CH 2CH 2CH 2CH 2CH 2CH 2— Si — OCH 2CH 3 and Hydrophilicity Hydrophobic and hydrophilic are frequently used OCH CH 2 3 descriptors of surfaces.
    [Show full text]