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Introduction of magnetisable solid phase extraction procedures have provided various advantages over spin-column based extraction techniques. Although certain methods for magnetic bead based extraction of DNA from human saliva already exist, there is still a need to address the inadequate purity profile and low yield which occur due to the inefficiency of extraction methods. Hence, an improved method for DNA extraction from human saliva using uncoated magnetic nanoparticles (MNPs) intended to resolve the issues mentioned above is described here. The uncoated magnetic nanoparticles used in this study facilitate reversible binding of DNA and due to the absence of surface coating the particle size remains small thereby providing higher surface area to volume ratio for binding DNA. Another objective of this study was to develop a saliva preservation buffer (SPB) to solve the major challenges associated with storage and easy transportation of saliva sample at room temperature. Human saliva samples stored in the saliva preservation buffer were stable up to 160 days at room temperature without any bacterial or fungal growth and the quality of genomic DNA was intact., (Copyright © 2021 Elsevier Inc. All rights reserved.)

We modeled the low-energy electron attachment to the sugar-phosphate-sugar (SPS) molecule for investigating the single-strand break (3' C-O and 5' C-O) at the DNA backbone. In particular, we predicted the electron capture at the phosphate center. We found that 0.6 eV electron can attach to the phosphate group, and the lifetime (∼40-55 fs) of the resulting temporary negative ion state is more than what we found for the lifetime of the metastable species (∼18-20 fs) formed at the cytosine base center. We treated the two competing dissociation channels in SPS molecule, that is, both the 3' C-O and 5' C-O lesions, separately. The activation energy barrier calculated for 5' C-O bond rupture is found to be less than that for 3' C-O bond dissociation. The overall low-energy electron transfer process is found to be mediated through a "shape resonance state" formed at the phosphate center.

Effect of electron correlation on single strand breaks (SSBs) induced by low energy electron (LEE) has been investigated in a fragment excised from a DNA, viz., 2'-deoxycytidine-3'-monophosphate [3'-dCMPH] molecule in gas phase at DFT-B3LYP/6-31+G(d) accuracy level and using local complex potential based time dependent wave packet (LCP-TDWP) approach. The results obtained, in conjunction with our earlier investigation, show the possibility of SSB at very low energy (0.15 eV) where the LEE transfers from π∗ to σ∗ resonance state which resembles a S(N)2 type mechanism. In addition, for the first time, an indication of quantum mechanical tunneling in strand breaking is seen from the highest anionic bound vibrational state (χ(5)), which may have a substantial role during DNA damage.

Although DNA bending plays a crucial role in several biological processes, very little is known experimentally about the relationship between sugar phosphate conformation and sequence directed bending. In this paper, we determine the coupling constants for a nonself-complementary 11-mer A-tract DNA duplex from 2D NMR experiments and along each chain of the duplex, we report the sugar pucker, torsional preferences and conformational averaging about the C3'-O3', C4'-C5' and C5'-O5' bonds for each nucleotide. The A-tract exists as an equilibrium blend of canonical B-form and noncanonical B-form in which the exocyclic C4'-C5' bond is in trans conformation as in the original Watson-Crick model [Crick, F.H.C. & Watson, J.D. (1954) Proc. Roy. Soc. (London), A223, 80-96]. The trans conformation at the C4'-C5' can increase the interphosphate distance and lead to local unwinding of the duplex and rolling of the base pair into the major groove. This will create a kink or hinge. At the 3'-end of the A-tract in the purine-thymine step, the duplex is compressed by the presence of a junction between A and B forms of DNA exclusively in one strand, with consequent reduction of the phosphate-phosphate distance. The coupling constant data seriously disagree with the A-tract DNA bending model of Crothers [Koo, H.-S., Wu, H.-M. & Crothers, D.M. (1986) Nature 320, 501-506], but is in agreement with the finding of Leroy et al. [Leroy, J.-L., Charretier, E., Kochoyan, M. & Gueron, M. (1988) Biochemistry 27, 8894-8898] that the structure that drives bending in the A-tract is locally different from B-DNA. Structural distortions are extremely localized with little or no propagation. It is likely that transcription factor proteins recognize these preexisting deformations in the free DNA itself and mold it into the matrix of the protein.

Investigation of the width of the minor groove using 500 MHz NMR spectroscopy in three closely related 11-mer B-DNA duplexes shows that the minor groove is narrow in a GC rich oligonucleotide, and that a narrow minor groove is not something endemic to DNAs with persistent repetitions of adenine nucleotides (A-tract DNA). The width of the groove is dictated by local sequence contexts and independent of neighboring A-tract DNA.

The oligonucleotide d(G5T5) can in principle form a fully matched duplex with G.T pairing and/or a tetraplex. Non-denaturing gel electrophoresis, circular dichroism and NMR experiments show that the tetraplex is exclusively formed by this oligomer in solution. In the presence of its complementary strand d(A5C5) at low temperature, d(G5T5) forms the tetraplex over the normally expected Watson-Crick duplex. However, when d(G5T5) and d(A5C5) are mixed together in equimolar amounts and heated for several minutes at 85 degrees C, and then allowed to cool, the product was essentially the Watson-Crick duplex. The lack of resolution in the 500 MHz 1H NMR spectra and the presence of extensive spin diffusion do not allow us to derive a quantitative structure for the tetraplex from the NMR data. However, we find good qualitative agreement between the NOESY and MINSY data and a theoretically derived stereochemically sound structure in which the G's and T's are part of a parallel tetraplex.

When the oligodeoxynucleotides d(A)6 and d(T)6 are mixed together in a 1:1 ratio (in 100 mM NaCl), the NH signals in the NMR spectrum gave a typical signature of Watson-Crick paired (WC) and Hoogsteen paired (H) AT base pairs. The observation indicates two schemes: Scheme I, WC and H duplexes in slow equilibrium, i.e., WC in equilibrium with H, Scheme II, the WC helix formed is unstable and that it disproportionates into a triple helix (TR) and free d(A)6. We show that (i) addition of extra d(A)6 does not change the helix composition, (ii) addition of a minor-groove specific drug Dst2 (a distamycin analogue) results in an exclusive WC helix-drug duplex, while it does not destabilize triple helix in a 1:2 mixture. In addition we have compared the melting profile, 31P NMR spectra, 1H NMR spectra and the salt dependence of the 1:1 mixture and that of a pure triple helix. All the data from the above experiments overwhelmingly favor Scheme I. However Scheme II cannot be categorically excluded. Based on 1D/2D NMR studies, we have characterized the structural properties of the Hoogsteen double helix in terms of nucleotide conformations. In addition, we computationally demonstrate that the relative stability of the WC over the H duplexes increases with increasing chain length.

Two-dimensional nuclear magnetic resonance (2D NMR) studies on d(GA4T4C)2 and d(GT4A4C)2 [Sarma, M.H., et al. (1988) Biochemistry 27, 3423-3432; Gupta G., et al. (1988) Biochemistry 27, 7909-7919] showed that A.T pairs are propeller twisted. As a result, A/T tracts form a straight rigid structural block with an array of bifurcated inter base pair H bonds in the major groove. It was demonstrated (previous paper) that replacement of methyl group by hydrogen (changing from T to U) in the major groove does not disrupt the array of bifurcated H bonds in the major groove. In this article, we summarize results of 2D NMR and molecular mechanic studies on the effect of a minor-groove-binding A.T-specific drug on the structure d(GA4T4C)2. A distamycin analogue (Dst2) was used for this study. It is shown that Dst2 binds to the minor groove of d(GA4T4C)2 mainly driven by van der Waals interaction between A.T pairs and the drug; as a consequence, an array of bifurcated H bonds can be formed in the minor groove between amide/amino protons of Dst2 and A.T pairs of DNA. NOESY data suggest that Dst2 predominantly binds at the central 5 A.T pairs. NOESY data also reveal that, upon drug binding, d(GA4T4C)2 does not undergo any significant change in conformation from the free state; i.e., propeller-twisted A.T pairs are still present in DNA and hence the array of bifurcated H bonds must be preserved in the major groove. NOESY data for the A5-T6 sequence also indicate that there is little change in junction stereochemistry upon drug binding.

NMR studies on d(GA4T4C)2 and d(GT4A4C)2 indicated two important factors that contribute to intrinsic DNA bending in polymers containing A/T tracts [Sarma, M.H., et al. (1988) Biochemistry 27, 3423; Gupta, G., et al. (1988) Biochemistry 27, 7909]. They are (i) propeller-twisted A.T pairs with associated bifurcated H bonds inside the A/T tract and (ii) the base sequence that joins the two neighboring A/T tracts. As an extension of our bending project, we carried out quantitative NMR studies on the decamer d(GA4U4C)2, a structural analogue of d(GA4T4C)2, to examine the effect of the methyl group on DNA bending. On the basis of quantitative NMR analysis, we arrive at the following results. (i) The decamer d(GA4U4C)2 adopts the gross morphology of a right-handed B-DNA duplex with A and U nucleotides belonging to C2'-endo,anti domain. (ii) A.U pairs are propeller twisted and hence can result in an array of interstrand bifurcated H bonds involving N6 of A and O4 of U (one base pair apart) inside the A/U tract. (iii) The orientations of A and U with respect to the long axis of the molecule are different; as a result, at the A5-U6 sequence that joins the two A/U tracts, two neighboring frames of reference do not exactly coincide in space and a junction is created at A5-U6. (iv) Inside the A/U tract, intrastrand stacking is more compact (average separation between secessive base planes being 3.2 A) than at the A5-U6 junction, where average separation between the base planes of A5 and U6 is 3.6 A.(ABSTRACT TRUNCATED AT 250 WORDS)

Magnetic shielding constants were calculated for the synthetic deoxyribonucleic acid (DNA) double helix poly(dG-dC).poly(dG-dC) from the x, y, and z coordinates of Z-DNA of Rich and co-workers [Wang, A. H-J., Quigley, G. J., Kolpak, F. J., Crawford, J. L., van Boom, J. H., van der Marel, G., & Rich, A. (1979) Nature (London) 282, 680-686)] and B-DNA of Arnott & Hukins [Arnott, S., & Hukins, D. W. L. (1972) Biochem. Biophys. Res. Commun. 47, 1504-1509], taking into account the contribution to shielding from ring current effects and effects from the diamagnetic and paramagnetic components of the atomic magnetic anisotropy. Comparison of the calculated shielding values with the experimentally observed nuclear magnetic resonance shift data for poly(dG-dC).poly(dG-dC) in high salt solution shows striking agreement for Z-DNA and considerable deviation for B-DNA, indicating that this synthetic DNA double helix is high salt solution can assume the spatial configuration of the left-handed Z-DNA double helix known to occur in crystals.

Intrinsic DNA bending is caused by specific DNA sequences. The decamer d(GA4T4C)2, when it repeats in a synthetic polymer or in kinetoplast DNA, results in a macroscopic bending of the molecule as a whole. We employed high-resolution two-dimensional NMR methods to examine the intrinsic structural properties of the d(GA4T4C)2 duplex in solution. Examination of the NOESY data at 50- and 100-ms mixing times indicated that the kinds of observed NOEs can originate if each of the ten nucleotidyl residues belongs to the B-DNA family, i.e., C2'-endo,anti. However, the degree of observed NOE intensities from the A-T junction as well as the observed AH2-AH2 cross-peaks from adjacent AT pairs could not be rationalized on the basis of a straight B-DNA model but could be explained by only a B-DNA model with some structural discontinuity at the A-T junction--the site of 2-fold symmetry in the molecule. In view of the fact that the degree of observed NOE intensities can be complicated by spin diffusion and by fine structural distortion, we have resorted to the use of quantitative theoretical NOESY simulation (which takes into account primary, secondary, and higher orders of NOE) to delineate the structural discontinuity at the A-T junction and to arrive at a structure for the duplex d(GA4T4C)2. We propose a "junction B-DNA model" which can quantitatively explain the 2D NOESY data at 100- and 50-ms mixing times. In this model the two structural blocks in the molecule, i.e., d(GA4).d(T4C) and d(T4C).d(GA4), are conformationally equivalent and are connected at the A-T junction where the base pairs are stably stacked, but the two local structural frames do not coincide in space. This model can create an overall bending of 10 degrees with a center of curvature 50 A away from the center of the duplex. It is the thesis of this paper that the observed bending in polymers with a repeat of d(GA4T4C)2 and the bending in natural DNAs where AnTn.AnTn repeats are present originate at the oligonucleotide repeat level.

1D NOE 1H NMR spectroscopy at 500 MHz was employed to examine the structure of poly(dA).poly(dT) in solution. NOE experiments were conducted as a function of presaturation pulse length (50, 30, 20 and 10 msec) and power (19 and 20 db) to distinguish the primary NOEs from spin diffusion. The 10 msec NOE experiments took 49 hrs and over 55,000 scans for each case and the difference spectra were almost free from diffusion. The spin diffused NOE difference spectra as well as difference NOE spectra in 90% H2O + 10% D2O in which TNH3 was presaturated enabled to make a complete assignment of the base and sugar protons. It is shown that poly(dA).poly(dT) melts in a fashion in which single stranded bubbles are formed with increasing temperature.

Combined use of shielding constant computations, measurements of chemical shifts and NOE studies reveal that poly(dG-dC).(poly)dG-dC) in low salt solutions exist as a right-handed B-DNA double helix described by Gupta, Dhingra, Sarma, Sarma, Rajagopalan and Sasisekharan, J. Biomole. Str. Dyn. 1. 395, 1983. We present a simple and direct method to determine the handedness of DNA double helices from NOE difference spectra. This method takes advantage of the NOE between base protons and the H2'H2" sugar protons; and in the difference NOE spectra in the H2'H2" region the signatures of the right and left-handed helices become imprinted.

Monitoring of the Watson-Crick GNH1 proton in poly(dG-dC).poly(dG-dC) at 500 MHz in 90% H2O:10% D2O at 30 degrees C as a function of NaCl concentration (1.5 to 3.6 M), demonstrates that the bases retain Watson-Crick pairing throughout the transition. This observation unequivocally demonstrates that during the B-Z transition there is no large scale and detectable base pair opening and that macroscopically the phenomenon can be described as a direct helix to helix transition. We present frame by frame, an energetically sound stereodynamical trajectory for this transfiguration from right-handed B-DNA to left-handed Z-DNA.

It is very well documented that the presence of an An.Tn tract causes intrinsic DNA bending. Hagerman demonstrated that the sequence in which the An.Tn tracts are joined plays a very crucial role in determining DNA bending. For example, Hagerman showed that the polymer with a repeat of d(GA4T4C)n greater than or equal to 10 is bent but the polymer with a repeat of d(GT4A4C)n greater than or equal to 10 is not bent [Hagerman, P. J. (1986) Nature (London) 326, 720-722]. Earlier we have shown that the decamer repeat d(GA4T4C)2 is itself bent with a finite structural discontinuity at the A----T sequence [Sarma, M. H., Gupta, G., & Sarma, R. H. (1988) Biochemistry 27, 3423-3432]. In the present article, we summarize our studies on the decamer repeat d(GT4A4C)2 structure in solution. By employment of 1D and 2D 1H NMR studies at 500 MHz a complete sequential assignment has been made for the exchangeable and nonexchangeable protons belonging to the ten nucleotides. NOESY data were collected for d(GT4A4C)2 at 17 degrees C in D2O for three mixing times, 150, 100, and 50 ms. A quantitative NOESY simulation technique was employed to arrive at a structural model of d(GT4A4C)2 in solution. Our detailed analyses revealed the following structural features: (i) The duplex adopts the gross morphology of a B-DNA. (ii) All the A.T pairs are propeller twisted (less than or equal to -15 degrees). (iii) Although both A and T nucleotides belong to the C2'-endo,anticonformational domain, there is a mild variation in the actual conformation of the A and T residues. (iv) Even though there is a subtle conformational difference in the A and T nucleotides, two structural frames of T4.A4 segments are joined at the T----A sequence in such a way that there is no finite discontinuity at the junction; i.e., two neighboring frames exactly coincide at the T----A junction. Thus, our studies on d(GA4T4C)2 (Sarma et al., 1988) and on d(GT4A4C)2 (this article) reveal the structural peculiarity of the An.Tn tract and the effect of A----T/T----A sequence in causing DNA bending.

The oligomer d(GCCGCAGC) can adopt two different conformations: i) a duplex with two mismatched A.C base pairs and ii) a hairpin with two C.G base pairs and a single stranded loop. We report molecular mechanics, normal mode analysis, and thermodynamic stability calculations for both structures. We show that the energy-minimized structure and harmonic-dynamics results are in complete agreement with the observed NOE spectrum and imino proton exchange data. We conclude that the high stability of the hairpin structure over the duplex at low salt concentration is due to the higher vibrational entropy contribution to the system free energy by the single stranded loop and to the lack of minor groove phosphate/phosphate electrostatic repulsions that tend to destabilize the duplex.

A hairpin structure contains two conformationally distinct domains: a double-helical stem with Watson-Crick base pairs and a single-stranded loop that connects the two arms of the stem. By extensive 1D and 2D 500-MHz 1H NMR studies in H2O and D2O, it has been demonstrated that the DNA oligomers d(CGCCGCAGC) and d(CGCCGTAGC) form hairpin structures under conditions of low concentration, 0.5 mM in DNA strand, and low salt (20 mM NaCl, pH 7). From examination of the nuclear Overhauser effect (NOE) between base protons H8/H6 and sugar protons H1' and H2'/H2", it was concluded that in d(CGCCGCAGC) and d(CGCCGTAGC) all the nine nucleotides display average (C2'-endo,anti) geometry. The NMR data in conjunction with molecular model building and solvent accessibility studies were used to derive a working model for the hairpins.

Extensive studies using one- and two-dimensional 1H NMR at 500 MHz revealed that the oligonucleotide d(CGCCGCAGC) in solution at 5 degrees C forms a double helix under conditions of high salt (500 mM in NaCl, 1 mM sodium phosphate), low pH (pH 4.5), and high DNA concentration (4 mM in duplex). The presence of very strong nuclear Overhauser effects (NOEs) from base H8/H6 to sugar H2',H2" and the absence of NOE from base H8/H6 to sugar H3' suggested that the oligomer under these solution conditions forms a right-handed B-DNA double helix. The following lines of experimental evidence were used to conclude that C4 and A7 form an integral part of the duplex: (i) the presence of a NOESY cross-peak involving H8 of A7 and H8 of G8, (ii) the presence of a two-dimensional NOE (NOESY) cross-peak between H6 of C3 and H6 of C4, (iii) base protons belonging to C4 and A7 forming a part of the H8/H6---H1' cross-connectivity route, and (iv) the pattern of H8/H6---H2',H2" NOESY cross-connectivity based upon a B-DNA model requiring that both C4 and A7 form an integral part of the duplex. The possibility of an A-C pair involving H bonds was also examined. Two possible structural models of the duplex at pH 4.5 are proposed: in one model A-C pairing involves two H bonds, and in the other A-C pairing involves a single H bond.