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G Raghunathan

Publications and source records attributed to G Raghunathan.

At least 19 recordsLinked to original sources
PubMed2000

Sequencing and model structure of a Naja naja atra protein fragment.

We report the amino acid sequence of a basic protein isolated from the snake venom of Naja naja atra. An automated Edman sequencer was used to determine the 65-residue sequence, aided by electrospray ionization/mass spectrometry. Online reduction and pyridylethylation of the peptide was performed to identify the cysteine residues. Trypsin, chymotrypsin and aspartic digestions were carried out to derive peptide fragments for further sequencing. Fragmented peptides were overlapped to obtain the complete sequence. Molecular mass measurements of the whole protein and its fragments were used as a countercheck for sequence assignment. Further confirmation of the sequence was indicated by sequence homology to other snake venom neurotoxins. A molecular model of the tertiary structure was constructed based on sequence homology, and was refined by global minimization and extensive quality control algorithms. Electrostatic and hydrophobic surface calculations and molecular dynamics simulations were carried out to determine the functional properties of the molecule.

Amino Acid Sequence↗
PubMed1997

Ideal architecture of residue packing and its observation in protein structures.

A simple model of sphere packing has been investigated as an ideal model for long-range interactions for the packing of non-bonded residues in protein structures. By superposing all residues, the geometry of packing around a central residue is investigated. It is found that all residues conform almost perfectly to this lattice model for sphere packing when a radius of 6.5 A is used to define non-bonded (virtual) interacting residues. Side-chain positions with respect to sequential backbone segments are relatively regular as well. This lattice can readily be used in conformation simulations to reduce the conformational space.

Amino Acids↗
PubMed1996

Structure of Py.Pu.Py DNA triple helices. Fourier transforms of fiber-type x-ray diffraction of single crystals.

Well-formed hexagonal crystals of oligomeric DNA triple helices exhibit fiber-type x-ray diffraction patterns [cf., Liu et al. (1994) Nature Struct. Biol. 1, 11], which can be interpreted in terms of Fourier transforms of these helices. Precession photographs of a triplex formed of dA and dT chains show that it has 13 residues per turn. In contrast, a sequence containing the four natural bases A, G, C, and T has 12 residues per turn. In this sense the triple helices exhibit a sequence-dependent polymorphism, though both have C2'-endo sugar pucker and B rather than A conformation. New models are constructed, using constraints from x-ray diffraction, and Fourier transforms of the models are calculated. Good agreement in the amplitudes and positions of the calculated and observed diffraction intensities confirms the structures for both triple helices. These are the first stereochemically satisfactory DNA triple helices for which coordinates based on adequate experimental data were provided. Sequences for crystallization are designed to achieve unique base alignments and are screened for the presence of sharp bands on gel electrophoresis to assure the absence of multiple species caused by strand slippage. Despite intensive efforts to observe normal crystal diffraction by varying sequences and conditions, all crystals exhibited only fiber-type diffraction. We suggest that this behavior may be an intrinsic property of triple helices and discuss possible reasons for the results. Spectroscopic and chemical experiments establish that the oligonucleotides exist in solution as triple helices under the conditions of crystallization.

Computer Simulation↗
PubMed1995

Symmetry and structure of RNA and DNA triple helices.

Despite wide interest in nucleic acid triple helices, there has been no stereochemically satisfactory structure of an RNA triple helix in atomic detail. AN RNA triplex structure has previously been proposed based on fiber diffraction and molecular modeling [S. Arnott and P. J. Bond (1973) Nature New Biology, Vol. 244, pp. 99-101; S. Arnott, P. J. Bond, E. Selsing, and P. J. C. Smith (1976) Nucleic Acids Research, Vol. 3, pp. 2459-2470], but it has nonallowed close contacts at every triplet and is therefore not stereochemically acceptable. We propose here a new model for an RNA triple helix in which the three chains have identical backbone conformations and are symmetry related. There are no short contacts. The modeling employs a novel geometrical approach using the linked atom least squares [P. J. C. Smith and S. Arnott (1978) Acta Crystallographica, Vol. A34, pp. 3-11] program and is not based on energy minimization. In general, the method leads to a range of possible structures rather than a unique structure. In the present case, however, the constraints resulting from the introduction of a third strand limit the possible structures to a very small range of conformation space. This method was used previously to obtain a model for DNA triple helices [G. Raghunathan, H. T. Miles, and V. Sasisekharan (1993) Biochemistry, Vol. 32, pp. 455-462], subsequently confirmed by fiber-type x-ray diffraction of oligomeric crystals [K. Liu, H. T. Miles, K. D. Parris, and V. Sasisekharan (1994) Nature Structural Biology, Vol. 1, pp. 11-12]. The above triple helices have Watson-Crick-Hoogsteen [K. Hoogsteen (1963) Acta Crystallographica, Vol. 16, pp. 907-916] pairing of the three bases. The same modeling method was used to investigate the feasibility of three-dimensional structures based on the three possible alternative hydrogen-bonding schemes: Watson-Crick-reverse Hoogsteen, Donohue [J. Donohue (1953) Proceedings of the National Academy of Science USA, Vol. 39, pp. 470-475] (reverse Watson-Crick)-Hoogsteen, and Donohue-reverse Hoogsteen. We found that none of these can occur in either RNA or DNA helices because they give rise only to structures with prohibitively short contacts between backbone and base atoms in the same chain.

DNA↗
PubMed1994

A parallel DNA triplex as a model for the intermediate in homologous recombination.

Parallel DNA triplexes considered to be putative intermediates in homologous recombination, are studied by means of theoretical conformational analysis. These triplexes are denoted as the R-form DNA. Two types of triplexes are analyzed: extended R-form DNA, modeling the triple standard structure, created transiently in the presence of recombination proteins (e.g. RecA); and collapsed R-form, obtained after deproteinization. These structures are stereochemically possible for any arbitrary sequence and have the following properties: (1) the third, R-strand, is parallel to the identical duplex strand and is located in the major groove of the duplex; (2) positions of all four bases in the R-strand are nearly isomorphic; (3) the proposed triplets are consistent with the chemical modification data for deproteinized DNA; we suggest, however, that they are the same in the RecA-DNA complex as well. Since the patterns of charges on each base of the R-strand are strictly complementary to the charges of the homologous Watson-Crick (WC) pair in the major groove, we propose that the selection of the homologous sequence may occur through these complementary electrostatic interactions (electrostatic recognition code). We demonstrate that in the collapsed triplex with a rise of about 3.4 A, the bases from the third R-strand can be inclined and interact with two WC base-pairs simultaneously, which could lead to recognition errors. These mispairings are unlikely in the extended triplex. Therefore, we speculate that a functional role of the extended and underwound DNA structure, transiently formed in the complex with RecA protein, is to obviate such errors and increase the stringency of recognition. In other words, RecA plays the role of a DNA chaperone facilitating the recognition of the single stranded DNA and the duplex. Finally, we show that the proposed isomorphic triplets are conformationally advantageous for strand exchange.

Base Composition↗
PubMed1994

Parallel nucleic acid helices with Hoogsteen base pairing: symmetry and structure.

Molecular structures for parallel DNA and RNA double helices with Hoogsteen pairing are proposed for the first time. The DNA helices have sugars in the C2'-endo region and the phosphodiester conformations are (trans, gauche-), and the RNA helices have sugars in the C3'-endo region and the phosphodiester conformations are (gauche-, gauche-). A pseudorotational symmetry relates the two parallel strands of DNA helices and a screw symmetry relates the two strands of RNA helices, which have an associated tilt of the bases. The conformational space of parallel helices with Hoogsteen base pairing, unlike the Watson-Crick duplex, is highly restricted due to the unique positioning of the symmetry axis in the former case. The features of the parallel double helix with Hoogsteen pairing are compared with the Watson-Crick duplex and the corresponding triple helix.

Base Composition↗
PubMed1994

Geometries, charges, dipole moments and interaction energies of normal, tautomeric and novel bases.

Ab initio molecular orbital calculations with the STO-3G and 4-31G basis sets are performed to study the geometries and interactions of natural and "novel" Watson-Crick base pairs, as well as some non-Watson-Crick base pairs. First the optimized geometries of bases are determined using the STO-3G basis set, and then for the base pairs with the STO-3G and 4-31G basis sets. Interaction energies of these base pairs are evaluated, and their relative stabilities are discussed. Hydrogen bond features, partial charges and dipole moments of the base pairs are described. The calculated stabilities are in reasonable agreement with the limited available experimental data from thermal melting studies. Hydrogen bond geometries at the 4-31G level are in good agreement with the crystal structure data. The order of relative stabilities is found to be: iG:iC > G:C > G:T* > rG:rC > A*:C > Am:U > tau:kappa > chi:kappa > G*:T > A:C* > A:U = A:T where, A*, T*, G* and C* are tautomers, iG and iC are iso-G and iso-C, Am is 2-amino adenine, chi is xanthosine, kappa is 2,4-diaminopyrimidine, tau is 7-methyl oxoformycin B, rG is modified guanine with substitutions at positions 5 and 7, and rC is modified cytosine with a substitution at position 6. Pairing strengths with modified bases may affect the efficiency of protein production.

Adenine↗
PubMed1994

Stability and cooperativity of nucleic acid base triplets.

Geometries and stabilities of various base triplets have been studied using ab initio quantum chemical methods. Their optimized geometries are determined using the STO-3G basis set, and those of Hoogsteen and reverse Hoogsteen base pairs are evaluated with the 4-31G basis set. Moreover, the preferred hydrogen bond patterns of the bases in triple helices are discussed. A cooperative effect for base pairing in triplets is presented, and it can be either positive or negative. Almost all base triplets that contain Watson-Crick G:C base pairs show a positive cooperativity. Conversely, the base triplets with Watson-Crick A:T base pairs mostly display a negative cooperativity. The interaction energies of base triplets are reported and the relative stabilities of base triplets are found as follows: A+.GC > C+.GC(H) > C+.GC(rH) > G.GC(H) > G.GC(rH) > A.GC > T.AT(rH) > U.AU(H) > U.AT(H) > A.AT > G.AT > T.AT(m) > G.TA(2) > G.TA(1) H and rH denote the Hoogsteen and reverse Hoogsteen positions of the third base that would lead to parallel and antiparallel orientations respectively of the third chain with respect to the Watson-Crick paired purine chain. 'm' denotes the middle pairing scheme, in which the third base hydrogen bonds to both bases of Watson-Crick pair.

Base Composition↗
PubMed1993

Symmetry and molecular structure of a DNA triple helix: d(T)n.d(A)n.d(T)n.

A structure for the triple helix d(T)n.d(A)n.d(T)n consistent with recent infrared spectral data is proposed, and its salient features are discussed. The present structure preserves the pseudodyad between the Watson-Crick base-paired adenine and thymine strands and in addition has a pseudorotational symmetry relating the Hoogsteen-paired adenine and thymine strands. The simultaneous presence of these two symmetries gives rise to a dyad between the two thymine polynucleotides. These symmetries result in identical backbone conformations for all three strands, unlike any previously proposed model for a triple helix. The proposed structure has an axial rise per residue of 3.26 A and 12 residues per turn obtained from X-ray fiber diffraction [Arnott S., & Selsing, E. (1974) J. Mol. Biol. 88, 509-521]. The present structure is structurally and conformationally similar to double helical B-form DNA and has sugar pucker in the C2'-endo region. This structure is fundamentally different from the one proposed by Arnott and co-workers, which was based on structural and conformational features similar to double helical A-form DNA with C3'-endo sugar pucker. It is stereochemically satisfactory, and it does not have the disallowed nonbonded distances present in the earlier model of Arnott and co-workers. It is energetically much more favorable than their structure. Coordinates of the present structure are given.

DNA↗
PubMed1992

Structure of d(T)n.d(A)n.d(T)n: the DNA triple helix has B-form geometry with C2'-endo sugar pucker.

The polynucleotide helix d(T)n.d(A)n.d(T)n is the only deoxypolynucleotide triple helix for which a structure has been published, and it is generally assumed as the structural basis for studies of DNA triplexes. The helix has been assigned to an A-form conformation with C3'-endo sugar pucker by Arnott and Selsing [1974; cf. Arnott et al. (1976)]. We show here by infrared spectroscopy in D2O solution that the helix is instead B-form and that the sugar pucker is in the C2'-endo region. Distamycin A, which binds only to B-form and not to A-form helices, binds to the triple helix without displacement of the third strand, as demonstrated by CD spectroscopy and gel electrophoresis. Molecular modeling shows that a stereochemically satisfactory structure can be build using C2'-endo sugars and a displacement of the Watson-Crick base-pair center from the helix axis of 2.5 A. Helical constraints of rise per residue (h = 3.26 A) and residues per turn (n = 12) were taken from fiber diffraction experiments of Arnott and Selsing (1974). The conformational torsion angles are in the standard B-form range, and there are no short contacts. In contrast, we were unable to construct a stereochemically allowed model with A-form geometry and C3'-endo sugars. Arnott et al. (1976) observed that their model had short contacts (e.g., 2.3 A between the phosphate-dependent oxygen on the A strand and O2 in the Hoogsteen-paired thymine strand) which are generally known to be outside the allowed range.(ABSTRACT TRUNCATED AT 250 WORDS)

Chemical Phenomena↗
PubMed1992

Magainin 2, a natural antibiotic from frog skin, forms ion channels in lipid bilayer membranes.

We have examined the ion channel forming properties of magainin 2 by incorporating the peptide into artificial lipid bilayers held under voltage clamp. Magainin 2 increased lipid bilayer conductance in a concentration dependent manner with a Hill coefficient of 1.7. The magainin 2 conductance was selective for monovalent cations over anions with a ratio of 5:1 and had both voltage-sensitive and -insensitive components. Two structurally related but antibiotically less potent analogues, magainin 1 and Z-12, also increased lipid bilayer conductance with a similar ion selectivity but these peptides were less potent than magainin 2. We propose that the weak cation selectivity of the magainin channels can be accounted for by the inclusion of negatively charged lipids in the channel complex and suggest two possible structures for such a channel. The ionophoric properties of these peptides are likely to be proximal to their antibiotic activities.

Animals↗
PubMed1992

Modeling the ion channel structure of cecropin.

Atomic-scale computer models were developed for how cecropin peptides may assemble in membranes to form two types of ion channels. The models are based on experimental data and physiochemical principles. Initially, cecropin peptides, in a helix-bend-helix motif, were arranged as antiparallel dimers to position conserved residues of adjacent monomers in contact. The dimers were postulated to bind to the membrane with the NH2-terminal helices sunken into the head-group layer and the COOH-terminal helices spanning the hydrophobic core. This causes a thinning of the top lipid layer of the membrane. A collection of the membrane bound dimers were then used to form the type I channel structure, with the pore formed by the transmembrane COOH-terminal helices. Type I channels were then assembled into a hexagonal lattice to explain the large number of peptides that bind to the bacterium. A concerted conformational change of a type I channel leads to the larger type II channel, in which the pore is formed by the NH2-terminal helices. By having the dimers move together, the NH2-terminal helices are inserted into the hydrophobic core without having to desolvate the charged residues. It is also shown how this could bring lipid head-groups into the pore lining.

Amino Acid Sequence↗
PubMed1991

Conformational feasibility of a hairpin with two purines in the loop. 5'-d-GGTACIAGTACC-3'.

Structural feasibility and conformational requirements for the sequence 5'-d-GGTACIAGTACC-3' to adopt a hairpin loop with I6 and A7 in the loop are studied. It is shown that a hairpin loop containing only two nucleotides can readily be formed without any unusual torsional angles. Stacking is continued on the 5'-side of the loop, with the I6 stacked upon C5. The base A7, on the 3'-side of the loop, can either be partially stacked with I6 or stick outside without stacking. Loop closure can be achieved for both syn and anti conformations of the glycosidic torsions for G8 while maintaining the normal Watson-Crick base pairing with the opposite C5. All torsional angles in the stem fall within the standard B-family of DNA helical structures. The phosphodiesters of the loop have trans,trans conformations. Loop formation might require the torsion about the C4'-C5' bond of G8 to be trans as opposed to the gauche+ observed in B-DNA. These results are discussed in relation to melting temperature studies [Howard et al. (1991) Biochemistry (preceding paper in this issue)] that suggest the formation of very stable hairpin structures for this sequence.

Base Sequence↗
PubMed1991

Structural and functional studies of full-length vascular cell adhesion molecule-1: internal duplication and homology to several adhesion proteins.

Full-length vascular cell adhesion molecule-1 (VCAM-1) cDNA cloned by polymerase chain reaction (PCR) of poly(A)+RNA from interleukin-1 (IL-1)-activated human umbilical vein endothelial cells (HUVEC) contained an insert of 276 nucleotides after position 1,034 of the previously published sequence. Synthetic oligomer probes, specific for each of the two possible species of VCAM-1 mRNA, detected only the longer form of VCAM-1 by Northern analysis of activated endothelial cell mRNA. This full-length VCAM-1 contains two internally repeated domains of approximately 273 amino acids with a high degree of homology. This new sequence information reveals homologies with additional members of the immunoglobulin superfamily and improves ALIGN scores for previously cited adhesion proteins. Removal of the transmembrane domain and the carboxy-terminal end of the full-length VCAM-1 molecule allows the molecule to be secreted into the culture medium from cells transfected with an expression vector containing the corresponding VCAM-1 cDNA.

Amino Acid Sequence↗
PubMed1990

Models of delta-hemolysin membrane channels and crystal structures.

Molecular modeling and energy calculations have been used to study how delta-hemolysin and melittin helices may aggregate on membrane surfaces and insert through membranes to form channels. In these models adjacent antiparallel amphipathic helices form planar "raft" structures, in which one surface is hydrophobic and the other hydrophilic. Models of delta-hemolysin crystal structure were developed using these "rafts." These models are based on the unit cell constants and the crystal symmetry obtained from the preliminary crystal data. Energy calculations favor channel models of delta-hemolysin with six or eight monomers per channel.

Amino Acids↗
PubMed1990

Solvation effects on the sequence variability of DNA double helical conformations.

The role of solvation on the sequence dependent conformational variabilities in DNA has been studied by calculating hydration free energies from solvent accessible surface areas for several base steps, as a function of various helical parameters, roll, twist and propeller twist. The results of roll calculations suggest opposite trends for AA and GG steps, with the former tending to have a compressed minor groove and the latter a compressed major groove. These trends are consistent with the experimental findings on sequence preferences and the nature of anisotropic bending of DNA observed in nucleosomes (Drew, H.R. and Travers, A.A., J. Mol. Biol. 186, 773-790 (1985); Satchwell, S.C., Drew, H.R. and Travers, A.A., J. Mol. Biol. 191, 659-675 (1986)) and CAP-DNA interactions (Gartenberg, M.R. and Crothers, D.M., Nature 333, 824-829, (1988)). Solvation energy profiles also indicate preferences for the base pairs in GG and AA steps to adopt low and high propeller twists, respectively. Such agreements may either reflect a coincidence of solvation effects with other energy terms or a dominance of solvent effects. The results are discussed in the context of the crystallographic observations of structural tendencies.

DNA, Superhelical↗
PubMed1990

Conformational features of DNA containing a cis-syn photodimer.

In an effort to understand the conformational and structural changes in DNA brought about by thymine photodimer, computer modeling and molecular mechanics energy calculations were performed on DNA hexamer and dodecamer duplexes containing a cis-syn photodimer. The conformation of the crystal structure of the cyanoethyl phosphate ester of the thymine dimer (Hruska et al., Biopolymers 25, 1399-1417 (1986)) was used in modeling the photodimer portion. Various starting conformations were used in the modeling procedure and the structures were minimized both retaining and later relaxing the crystallographic geometry of the cyclobutane ring. The results indicate that most of the deformation is restricted to the thymine dimer region, and that the conformational changes decrease rapidly on either side of the region containing the photodimer. The structural changes brought about by the introduction of the photodimer can be accommodated within six base paired duplex without significant bend in the DNA. More conformational changes are observed on the 5'-side of the photodimer than on the 3'-side. The conformational features, such as backbone torsion angles and sugar puckers, of the energy minimized structures are discussed in the context of the solution structures determined by NMR on a series of oligomers containing photodimers (Rycyna et al., Biochemistry 27, 3152-3163 (1988)).

Base Sequence↗