Lessons learned in atomistic simulation of double-stranded DNA: Solvation and salt concerns [Article v1.0]

Coarse-grained modeling of DNA-RNA hybrids

We introduce oxNA, a new model for the simulation of DNA-RNA hybrids that is based on two previously developed coarse-grained models-oxDNA and oxRNA. The model naturally reproduces the physical properties of hybrid duplexes, including their structure, persistence length, and force-extension characteristics. By parameterizing the DNA-RNA hydrogen bonding interaction, we fit the model's thermodynamic properties to experimental data using both average-sequence and sequence-dependent parameters. To demonstrate the model's applicability, we provide three examples of its use-calculating the free energy profiles of hybrid strand displacement reactions, studying the resolution of a short R-loop, and simulating RNA-scaffolded wireframe origami.

Assessment of A- to B- DNA Transitions Utilizing the Drude Polarizable Force Field

In addition to the well-characterized B-form of DNA, duplex DNA can adopt various conformations, such as A or Z-DNA. Though less common, these structures can be induced biologically through protein or ligand interactions or experimentally with niche environmental conditions, such as high salt concentrations or in mixed water-ethanol. Reproducing these alternate structures through molecular dynamics simulations in recent years has been quite challenging with the currently available force fields, simulation techniques, and time scales. In this study, the Drude polarizable force field is tested for its ability to facilitate transitions between A-DNA and B-DNA or maintain A-DNA. Though transitions away from B-DNA were observed in high concentrations of ethanol, the resulting structures had hybrid properties taken from both B-DNA and A-DNA structures. This was also true for A-DNA in ethanol, which lost some of the A-DNA properties that it was expected to maintain. When B-DNA was tested in high salt environments, the resulting B-DNA structures showed no distinguishable differences with the increasing salt concentrations tested. These results with the Drude FF and recent results with additive force fields suggest that at present the current additive and polarizable force fields do not facilitate a complete transition between B- to A-DNA conformations under the conditions simulated. At present, the Drude FF favors A-B DNA hybrid structures when simulated in nonphysiological conditions.

Why Na+ has higher propensity than K+ to condense DNA in a crowded environment

Experimentally, in the presence of the crowding agent polyethylene glycol (PEG), sodium ions compact double-stranded DNA more readily than potassium ions. Here, we have used molecular dynamics simulations and the "ion binding shells model" of DNA condensation to provide an explanation for the observed variations in condensation of short DNA duplexes in solutions containing different monovalent cations and PEG; several predictions are made. According to the model we use, externally bound ions contribute the most to the ion-induced aggregation of DNA duplexes. The simulations reveal that for two adjacent DNA duplexes, the number of externally bound Na+ ions is larger than the number of K+ ions over a wide range of chloride concentrations in the presence of PEG, providing a qualitative explanation for the higher propensity of sodium ions to compact DNA under crowded conditions. The qualitative picture is confirmed by an estimate of the corresponding free energy of DNA aggregation that is at least 0.2kBT per base pair more favorable in solution with NaCl than with KCl at the same ion concentration. The estimated attraction free energy of DNA duplexes in the presence of Na+ depends noticeably on the DNA sequence; we predict that AT-rich DNA duplexes are more readily condensed than GC-rich ones in the presence of Na+. Counter-intuitively, the addition of a small amount of a crowding agent with high affinity for the specific condensing ion may lead to the weakening of the ion-mediated DNA-DNA attraction, shifting the equilibrium away from the DNA condensed phase.

Structure and dynamics of an archetypal DNA nanoarchitecture revealed via cryo-EM and molecular dynamics simulations

DNA can be folded into rationally designed, unique, and functional materials. To fully realise the potential of these DNA materials, a fundamental understanding of their structure and dynamics is necessary, both in simple solvents as well as more complex and diverse anisotropic environments. Here we analyse an archetypal six-duplex DNA nanoarchitecture with single-particle cryo-electron microscopy and molecular dynamics simulations in solvents of tunable ionic strength and within the anisotropic environment of biological membranes. Outside lipid bilayers, the six-duplex bundle lacks the designed symmetrical barrel-type architecture. Rather, duplexes are arranged in non-hexagonal fashion and are disorted to form a wider, less elongated structure. Insertion into lipid membranes, however, restores the anticipated barrel shape due to lateral duplex compression by the bilayer. The salt concentration has a drastic impact on the stability of the inserted barrel-shaped DNA nanopore given the tunable electrostatic repulsion between the negatively charged duplexes. By synergistically combining experiments and simulations, we increase fundamental understanding into the environment-dependent structural dynamics of a widely used nanoarchitecture. This insight will pave the way for future engineering and biosensing applications.

Twisting DNA by salt

The structure and properties of DNA depend on the environment, in particular the ion atmosphere. Here, we investigate how DNA twist -one of the central properties of DNA- changes with concentration and identity of the surrounding ions. To resolve how cations influence the twist, we combine single-molecule magnetic tweezer experiments and extensive all-atom molecular dynamics simulations. Two interconnected trends are observed for monovalent alkali and divalent alkaline earth cations. First, DNA twist increases monotonously with increasing concentration for all ions investigated. Second, for a given salt concentration, DNA twist strongly depends on cation identity. At 100 mM concentration, DNA twist increases as Na+ < K+ < Rb+ < Ba2+ < Li+ ≈ Cs+ < Sr2+ < Mg2+ < Ca2+. Our molecular dynamics simulations reveal that preferential binding of the cations to the DNA backbone or the nucleobases has opposing effects on DNA twist and provides the microscopic explanation of the observed ion specificity. However, the simulations also reveal shortcomings of existing force field parameters for Cs+ and Sr2+. The comprehensive view gained from our combined approach provides a foundation for understanding and predicting cation-induced structural changes both in nature and in DNA nanotechnology.

Multiscale computational investigations of the translesion synthesis bypass of tobacco-derived DNA adducts: critical insights that complement experimental biochemical studies

Among the numerous agents that damage DNA, tobacco products remain one of the most lethal and result in the most diverse set of DNA lesions. This perspective aims to provide an overview of computational work conducted to complement experimental biochemical studies on the mutagenicity of adducts derived from the most potent tobacco carcinogen, namely 4-(methylnitrosamino)-1-(3-pyridyl)-1-butanone (nicotine-derived nitrosaminoketone or NNK). Lesions ranging from the smallest methylated thymine derivatives to the larger, flexible pyridyloxobutyl (POB) guanine adducts are considered. Insights are obtained from density functional theory (DFT) calculations and molecular dynamics (MD) simulations into the damaged nucleobase and nucleoside structures, the accommodation of the lesions in the active site of key human polymerases, the intrinsic base pairing potentials of the adducts, and dNTP incorporation opposite the lesions. Overall, the computational data provide atomic level information that can rationalize the differential mutagenic properties of tobacco-derived lesions and uncover important insights into the impact of adduct size, nucleobase, position, and chemical composition of the bulky moiety.

Searching for Low Probability Opening Events in a DNA Sliding Clamp

The β subunit of E. coli DNA polymererase III is a DNA sliding clamp associated with increasing the processivity of DNA synthesis. In its free form, it is a circular homodimer structure that can accomodate double-stranded DNA in a nonspecific manner. An open state of the clamp must be accessible before loading the DNA. The opening mechanism is still a matter of debate, as is the effect of bound DNA on opening/closing kinetics. We use a combination of atomistic, coarse-grained, and enhanced sampling strategies in both explicit and implicit solvents to identify opening events in the sliding clamp. Such simulations of large nucleic acid and their complexes are becoming available and are being driven by improvements in force fields and the creation of faster computers. Different models support alternative opening mechanisms, either through an in-plane or out-of-plane opening event. We further note some of the current limitations, despite advances, in modeling these highly charged systems with implicit solvent.

Molecular Modeling and Simulations of DNA and RNA: DNAzyme as a Model System

Nowadays, the structural dynamics of DNA and RNA is accessible on an atomistic level on a micro- to millisecond time scale via molecular dynamics simulations. However, as DNA or RNA are highly charged molecules, performing such simulations is challenging as to the representation of intramolecular electrostatic interactions and those to solvent molecules and ions. This is particularly true for DNAzymes, where DNA and RNA backbones can come as close as 2.4 Å with their charged phosphate groups during the catalytic cycle. Here, we present tools to simulate the structural dynamics of a DNAzyme, with a focus on detailed instructions for the Amber suite of programs. Furthermore, we will show how to analyze metal ion binding within the DNAzyme.

Similarities and Differences between Na+ and K+ Distributions around DNA Obtained with Three Popular Water Models

We have compared distributions of sodium and potassium ions around double-stranded DNA, simulated using fixed charge SPC/E, TIP3P, and OPC water models and the Joung/Cheatham (J/C) ion parameter set, as well as the Li/Merz HFE 6-12 (L/M HFE) ion parameters for OPC water. In all the simulations, the ion distributions are in qualitative agreement with Manning's condensation theory and the Debye-Hückel theory, where expected. In agreement with experiment, binding affinity of monovalent ions to DNA does not depend on ion type in every solvent model. However, behavior of deeply bound ions, including ions bound to specific sites, depends strongly on the solvent model. In particular, the number of potassium ions in the minor groove of AT-tracts differs at least 3-fold between the solvent models tested. The number of sodium ions associated with the DNA agrees quantitatively with the experiment for the OPC water model, followed closely by TIP3P+J/C; the largest deviation from the experiment, ∼10%, is seen for SPC/E+J/C. On the other hand, SPC/E+J/C model is most consistent (67%) with the experimental potassium binding sites, followed by OPC+J/C (60%), TIP3P+J/C (53%), and OPC+L/M HFE (27%). The use of NBFIX correction with TIP3P+J/C improves its consistency with the experiment. In summary, the choice of the solvent model matters little for simulating the diffuse atmosphere of sodium and potassium ions around DNA, but ion distributions become increasingly sensitive to the solvent model near the helical axis. We offer an explanation for these trends. There is no single gold standard solvent model, although OPC water with J/C ions or TIP3P with J/C + NBFIX may offer an imperfect compromise for practical simulations of ionic atmospheres around DNA.

Impact of DNA Adduct Size, Number, and Relative Position on the Toxicity of Aromatic Amines: A Molecular Dynamics Case Study of ANdG- and APdG-Containing DNA Duplexes

Human exposure to aromatic amines (AAs) can result in carcinogenic DNA adducts. To complement previous work geared toward understanding the mutagenicity of AA-derived adducts, which has almost exclusively studied (monoadducted) DNA containing a single lesion, the present work provides the first in-depth comparison of the structure of monoadducted and diadducted DNA duplexes. Specifically, molecular dynamics (MD) simulations were initially performed on DNA containing the nonmutagenic single-ringed N-(deoxyguanosin-8-yl)-aniline (^ANdG) or the mutagenic four-ringed N-(deoxyguanosin-8-yl)-1-aminopyrene (^APdG) lesion at G₁, G₂, or G₃ in the AA deletion hotspot (5'-G₁G₂CG₃CC) in the anti or syn glycosidic orientation (B/S duplex conformation). Subsequently, diadducted strands were assessed that span each combination of damaged sites (G₁G₂ (nearest neighbors), G₂G₃ (next-nearest neighbors), and G₁G₃ (two intervening nucleotides)) and anti/syn lesion glycosidic orientations. Despite other N-linked C8-dG adducts exhibiting sequence dependence conformational heterogeneity, a single ^ANdG or ^APdG lesion induces helical conformational homogeneity that is exclusively controlled by aryl moiety size. However, the preferred damaged DNA conformation can change upon the addition of a second adduct depending on lesion separation, with neighboring lesions stabilizing a nonmutagenic conformation and next-nearest damaged sites stabilizing a promutagenic conformation regardless of adduct size. As a result, diadducted DNA is found to adopt conformations that are unfavored for the corresponding monoadducted system, pointing to differential replication and repair outcomes for diadducted DNA compared to those for monoadducted DNA. Thus, although the toxicity of monoadducted DNA is most significantly dictated by lesion size, the toxicity can increase or decrease upon a second damaging event depending on lesion size and relative position. Overall, our work adds the number of lesions and their spatial separation to the growing list of factors that determine the structure and biological outcomes of adducted DNA.