47 research outputs found

    Preferential binding and structural distortion by Fe2+ at RGGG-containing DNA sequences correlates with enhanced oxidative cleavage at such sequences.

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    Certain DNA sequences are known to be unusually sensitive to nicking via the Fe2+-mediated Fenton reaction. Most notable are a purine nucleotide followed by three or more G residues, RGGG, and purine nucleotides flanking a TG combination, RTGR. Our laboratory previously demonstrated that nicking in the RGGG sequences occurs preferentially 5' to a G residue with the nicking probability decreasing from the 5' to 3'end of these sequences. Using 1H NMR to characterize Fe2+ binding within the duplex CGAGTTAGGGTAGC/GCTACCCTAACTCG and 7-deazaguanine-containing (Z) variants of it, we show that Fe2+ binds preferentially at the GGG sequence, most strongly towards its 5' end. Substitutions of individual guanines with Z indicate that the high affinity Fe2+ binding at AGGG involves two adjacent guanine N7 moieties. Binding is accompanied by large changes in specific imino, aromatic and methyl proton chemical shifts, indicating that a locally distorted structure forms at the binding site that affects the conformation of the two base pairs 3' to the GGG sequence. The binding of Fe2+ to RGGG contrasts with that previously observed for the RTGR sequence, which binds Fe2+ with negligible structural rearrangements

    Self-assembly of short DNA duplexes: from a coarse-grained model to experiments through a theoretical link

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    Short blunt-ended DNA duplexes comprising 6 to 20 base pairs self-assemble into polydisperse semi-flexible chains due to hydrophobic stacking interactions between terminal base pairs. Above a critical concentration, which depends on temperature and duplex length, such chains order into liquid crystal phases. Here, we investigate the self-assembly of such double-helical duplexes with a combined numerical and theoretical approach. We simulate the bulk system employing the coarse-grained DNA model recently proposed by Ouldridge et al. [ J. Chem. Phys. 134, 08501 (2011) ]. Then we evaluate the input quantities for the theoretical framework directly from the DNA model. The resulting parameter-free theoretical predictions provide an accurate description of the simulation results in the isotropic phase. In addition, the theoretical isotropic-nematic phase boundaries are in line with experimental findings, providing a route to estimate the stacking free energy.Comment: 13 pages, 10 figure

    Low-Cost Methods for DNA Extraction and Quantification

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    DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด์˜ ์—ผ๊ธฐ์„œ์—ด์— ๋”ฐ๋ฅธ ํ˜•์ƒ ๋ฐ ์—ญํ•™์  ํŠน์„ฑ์„ ์˜ˆ์ธกํ•˜๋Š” ๋ฉ€ํ‹ฐ์Šค์ผ€์ผ ๋ชจ๋ธ๋ง ๋ฐฉ๋ฒ•

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€, 2020. 8. ๊น€๋„๋…„.DNA nanotechnology is a rising field that designs, manufactures, and analyzes DNA nanostructures using the self-assembly principle, creating various related applications. DNA nanostructures are based on the connection between sequences (A, T, G, and C), and its mechanical properties are derived from interactions between atoms. Therefore, to completely understand the mechanical characteristics of DNA nanostructures, all-atomic simulation is required. However, in general, a DNA nanostructure is composed of connections between thousands of sequences in a salt solution, and in order to simulate it on an atomic scale, the atomic system containing billions of degrees of freedom should be solved numerically, which is almost impossible. Accordingly, coarse-grained models have been developed to analyze DNA nanostructures by reducing the degree of freedom, but there are still difficulties to achieve both high efficiency and accuracy of the analysis. Here, this study presents a method to rapidly predict DNA nanostructures at the nanoscale accuracy through multiscale modeling. First, the connections between sequences were classified, and molecular dynamics simulations of a reduced system including them were performed to quantify the sequence-dependent mechanical properties. Next, a finite element model was developed to embody the unique properties, and electrostatic repulsion inside the structure due to the negative charge of DNA in the solution. The assembled finite elements incorporate all the mechanical properties at the sequence-level. Through numerical procedure and normal mode analysis, the equilibrium shape and dynamic properties are rapidly and accurately predicted. The proposed approach can be applied to the analysis of nucleic-acid-based structures and extended to multiscale modeling methods of biomaterials.DNA ๋‚˜๋…ธ๊ธฐ์ˆ ์€ DNA์˜ ์ž๊ฐ€์กฐ๋ฆฝ์›๋ฆฌ๋ฅผ ์ด์šฉํ•ด ๋‚˜๋…ธ ํ•ด์ƒ๋„์˜ ์ •๋ฐ€ํ•œ ๊ตฌ์กฐ์ฒด๋ฅผ ์„ค๊ณ„ ๋ฐ ์ œ์ž‘, ํ•ด์„ํ•˜๋Š” ๋ถ„์•ผ๋กœ, DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด๋ฅผ ์ด์šฉํ•œ ์ˆ˜๋งŽ์€ ์‘์šฉ ์—ฐ๊ตฌ๊ฐ€ ์ง€์†์ ์œผ๋กœ ์ œ์‹œ๋˜๊ณ  ์žˆ๋‹ค. DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด๋Š” ๊ธฐ๋ณธ ์—ผ๊ธฐ(A, T, G, C) ๊ฐ„์˜ ์—ฐ๊ฒฐ์ฒด๋กœ์„œ, ์ด์— ๋”ฐ๋ฅธ ๊ตญ์†Œ์ ์ธ ์—ญํ•™์  ๋ฌผ์„ฑ์€ ์—ผ๊ธฐ๋ฅผ ๊ตฌ์„ฑํ•˜๋Š” ์›์ž ๊ฐ„์˜ ์ƒํ˜ธ์ž‘์šฉ์— ์˜ํ•ด ๋ฐœํ˜„๋œ๋‹ค. ๋”ฐ๋ผ์„œ DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด์˜ ์—ญํ•™์  ๊ฑฐ๋™์„ ์˜จ์ „ํžˆ ์ดํ•ดํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ๋‚˜๋…ธ ์Šค์ผ€์ผ์˜ ์ „์›์ž ์‹œ๋ฎฌ๋ ˆ์ด์…˜์ด ํ•„์š”ํ•˜๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์ผ๋ฐ˜์ ์œผ๋กœ DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด๋Š” ์—ผ์ด ํฌํ•จ๋œ ์ˆ˜์šฉ์•ก ํ™˜๊ฒฝ์—์„œ ์ˆ˜์ฒœ ๊ฐœ์˜ ์—ผ๊ธฐ๊ฐ€ ์—ฐ๊ฒฐ๋˜์–ด ๊ตฌ์„ฑ๋˜๋ฏ€๋กœ, ์ด๋ฅผ ์›์ž ์Šค์ผ€์ผ์—์„œ ํ•ด์„ํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ์–ต ๋‹จ์œ„์˜ ์›์ž ์ž์œ ๋„ ๋ฌธ์ œ๋ฅผ ์ˆ˜์น˜์ ์œผ๋กœ ํ•ด๊ฒฐํ•ด์•ผ ํ•˜์—ฌ, ์‹œ์Šคํ…œ ์ „์ฒด์˜ ์ „์›์ž ์‹œ๋ฎฌ๋ ˆ์ด์…˜์€ ๊ฑฐ์˜ ๋ถˆ๊ฐ€๋Šฅํ•˜๋‹ค. ์ด์— ์ž์œ ๋„๋ฅผ ์ค„์—ฌ DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด๋ฅผ ํ•ด์„ํ•˜๊ธฐ ์œ„ํ•œ ์—ฌ๋Ÿฌ ์ถ•์†Œ๋ชจ๋ธ์ด ๊ฐœ๋ฐœ๋˜๊ณ  ์žˆ์œผ๋‚˜, ํ•ด์„์˜ ๋†’์€ ํšจ์œจ์„ฑ๊ณผ ์ •ํ™•์„ฑ์„ ๋ชจ๋‘ ๋‹ฌ์„ฑํ•˜๋ ค๋ฉด ์—ฌ์ „ํžˆ ๋‚œ์ œ๊ฐ€ ๋งŽ๋‹ค. ์ด์— ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๋ฉ€ํ‹ฐ์Šค์ผ€์ผ ๋ชจ๋ธ๋ง์„ ํ†ตํ•ด ์—ผ๊ธฐ ์Šค์ผ€์ผ์˜ ์ •ํ™•๋„๋กœ DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด๋ฅผ ํšจ์œจ์ ์œผ๋กœ ํ•ด์„ํ•˜๋Š” ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•œ๋‹ค. ๋จผ์ € ์—ผ๊ธฐ ๊ฐ„์˜ ๋‹ค์–‘ํ•œ ์—ฐ๊ฒฐ ๋ฐฉ์‹์„ ๋ถ„๋ฅ˜ํ•˜๊ณ , ์ด๋ฅผ ํฌํ•จํ•œ ์ž‘์€ ์‹œ์Šคํ…œ์˜ ๋ถ„์ž๋™์—ญํ•™ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ํ†ตํ•ด, ์—ผ๊ธฐ์— ๋”ฐ๋ฅธ ์—ญํ•™์  ํŠน์„ฑ์„ ์ •๋Ÿ‰ํ™”ํ•˜๊ณ  ๋ฌผ์„ฑ ๋ผ์ด๋ธŒ๋Ÿฌ๋ฆฌ๋ฅผ ๊ตฌ์ถ•ํ•˜์˜€๋‹ค. ๋‹ค์Œ์œผ๋กœ ์—ผ๊ธฐ ๊ฐ„์˜ ์—ฐ๊ฒฐ์— ๋”ฐ๋ฅธ ๊ณ ์œ ํ•œ ์—ญํ•™์  ๋ฌผ์„ฑ๊ณผ ์ˆ˜์šฉ์•ก ํ™˜๊ฒฝ์—์„œ DNA์˜ ์Œ์ „ํ•˜๋กœ ์ธํ•ด ๋ฐœ์ƒํ•˜๋Š” ๊ตฌ์กฐ์ฒด ๋‚ด๋ถ€์˜ ์ •์ „๊ธฐ์  ๋ฐ˜๋ฐœ๋ ฅ์„ ์™„์ „ํžˆ ๋ฐ˜์˜ํ•˜๋Š” ์œ ํ•œ์š”์†Œ ๋ชจ๋ธ์„ ๊ฐœ๋ฐœํ•˜์—ฌ, DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด๋ฅผ ๊ตฌ์„ฑํ•˜๋Š” ๋ชจ๋“  ์—ผ๊ธฐ ๊ฐ„์˜ ์—ฐ๊ฒฐ๊ณผ ๊ตฌ์กฐ์ฒด ๋‚ด๋ถ€์˜ ์ƒํ˜ธ์ž‘์šฉ์„ ์œ ํ•œ์š”์†Œ ์—ฐ๊ฒฐ์ฒด๋กœ ๋ณ€ํ™˜ํ•˜์˜€๋‹ค. ๊ตฌ์„ฑ๋œ ์œ ํ•œ์š”์†Œ ์—ฐ๊ฒฐ์ฒด๋Š” ์—ผ๊ธฐ ์Šค์ผ€์ผ์˜ ํ•ด์ƒ๋„๋กœ DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด์˜ ์—ญํ•™์  ํŠน์„ฑ์„ ๋ชจ๋‘ ๋‚ดํฌํ•˜๊ณ  ์žˆ์–ด, ๋น„์„ ํ˜• ์ˆ˜์น˜ํ•ด์„๊ณผ ๊ณ ์œ ๋ชจ๋“œ ๋ถ„์„์„ ํ†ตํ•ด DNA ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด์˜ ์—ผ๊ธฐ์„œ์—ด์— ๋”ฐ๋ฅธ ํ‰ํ˜• ํ˜•์ƒ๊ณผ ๋™์  ํŠน์„ฑ์„ ์ •ํ™•ํ•˜๊ณ  ๋น ๋ฅด๊ฒŒ ์˜ˆ์ธกํ•  ์ˆ˜ ์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ ์ œ์‹œํ•˜๋Š” ๊ธฐ๋ฒ•์€ ํ•ต์‚ฐ ๊ธฐ๋ฐ˜์˜ ๊ตฌ์กฐ์ฒด ํ•ด์„์— ์‰ฝ๊ฒŒ ์ ์šฉํ•  ์ˆ˜ ์žˆ์œผ๋ฉฐ, ๋‹ค์–‘ํ•œ ๋ฐ”์ด์˜ค ์žฌ๋ฃŒ์˜ ๋ฉ€ํ‹ฐ์Šค์ผ€์ผ ๋ชจ๋ธ๋ง ๊ธฐ์ˆ ๋กœ ํ™•์žฅ๋  ์ˆ˜ ์žˆ๋‹ค.1. Introduction 28 1.1. Background and objectives 28 1.2. Research outline 30 1.3. Overview of the multiscale modeling approach 32 2. Investigation of the mechanical properties of DNA 37 2.1. Abstract 37 2.2. Methods 38 2.2.1. Generation of DNA oligomers 38 2.2.2. Molecular dynamics simulations of DNA oligomers 41 2.2.3. Overview of characterizing mechanical properties 43 2.2.4. Mechanical properties of a base-pair step 57 2.2.5. Elastic theory for the base-pair step 60 2.2.6. Equivalent isotropic rigidities in bending and shearing 64 2.3. Mechanical rigidities of base-pair steps 66 2.4. Mechanical coupling coefficients of base-pair steps 72 2.5. Effects of simulation parameters and neighboring sequence 75 3. Multiscale modeling of DNA nanostructures 90 3.1. Abstract 90 3.2. Finite element framework for structural motifs 91 3.2.1. Operators 92 3.2.2. The co-rotational formulation of the two-node beam element 93 3.2.3. Internal force vector in the global coordinate 96 3.2.4. Stiffness matrix in the global coordinate 99 3.3. Local stiffness matrix and internal force vector 101 3.3.1. Net displacement in the local coordinate 102 3.3.2. Displacement field 103 3.3.3. Strain field 104 3.3.4. Strain energy 107 3.3.5. Stiffness matrix in the local coordinate 109 3.3.6. Internal force vector in the local coordinate 110 3.4. Intrinsic properties of the base-pair step 111 3.4.1. Relative geometric parameters in the 3DNA definition 111 3.4.2. Relative geometry and mechanical properties 115 3.4.3. Modification of triad axes for beam element 117 3.4.4. Intrinsic properties of the BP step 118 3.5. Intrinsic properties of the crossover step 130 3.5.1. Modification of triad axes in the crossover step 130 3.5.2. Triad angle correction 131 3.5.3. Intrinsic properties of the crossover step 132 3.6. Characterization and modeling of single-stranded DNA 142 3.6.1. Intrinsic end-to-end length 142 3.6.2. Single-stranded DNA properties 145 3.7. Finite element framework for electrostatic interaction 147 3.7.1. Electrostatic interaction model 147 3.7.2. Finite element model of electrostatic interaction 148 3.8. Estimation of characteristic values on the electrostatic interaction 152 3.9. Construction of initial configuration 154 3.9.1. General description 154 3.9.2. Initial BP triads for the 2-helix-bundle structure 155 3.9.3. Initial configuration of structural elements for base-pair steps 158 3.9.4. Initial configuration of structural elements for crossover steps 160 3.9.5. Generation of electrostatic elements 161 3.10. Nonlinear solution procedure 162 3.10.1. Overview of the solution procedure 162 3.10.2. Element properties in the initial and final configuration 164 3.10.3. Boundary condition 165 3.10.4. Control of properties in structural elements 166 3.10.5. Control of the number of electrostatic elements 167 3.10.6. Iterative solution methods 168 3.10.7. Subdivision of time interval 170 3.10.8. Condition number of stiffness matrix 172 3.11. Molecular dynamics simulation of DNA nanostructures 173 4. Structural analysis of DNA nanostructures 183 4.1. Abstract 183 4.2. Shape prediction of monomeric structures 184 4.2.1. Electrostatic effects on the structural shape 184 4.2.2. Control of included angle in hinge structures 187 4.2.3. Structural distortion by the mean helicity 189 4.2.4. Bending and twist control by inserting or deleting base-pairs 193 4.3. Shape prediction of hierarchical assemblies 200 4.3.1. Control of opening angle in geometrically-constrained V brick 200 4.3.2. Assessment of the twist-correction effect in the tube structure 204 4.3.3. Prediction of hierarchically assembled polyhedral structures 206 4.4. Structural details at the base-pair level 212 4.4.1. The dimension of the pointer structure 212 4.4.2. Prediction of the base-pair and crossover configuration 216 5. Twist control of DNA nanostructures through sequence design 218 5.1. Abstract 218 5.2. Methods 219 5.2.1. Mechanical analysis of DNA structures with base-pair insertion 219 5.2.2. Design and simulation of twisted DNA origami structures 223 5.2.3. Molecular dynamics simulation of 6-helix-bundle blocks 228 5.2.4. Measurement of the twist angle of 6-helix-bundle structures 229 5.2.5. CanDo simulation based on finite element method 231 5.2.6. Relation of the trans ratio with the global twist angle 233 5.2.7. Preparation of DNA origami structures 239 5.2.8. Image analysis using atomic force microscopy 240 5.2.9. Agarose gel electrophoresis 249 5.2.10. Comparison of Bio-RP and PAGE in the purification of staples 250 5.3. Twist control of DNA nanostructures by programming nick sequences 253 5.3.1. Sequences design to control the twist of DNA nanostructure 254 5.3.2. Prediction and experimental validation of the global twist angle 257 6. Dynamic characteristics of DNA nanostructures 260 6.1. Abstract 260 6.2. Methods 261 6.2.1. Normal mode analysis 261 6.2.2. Root-mean-square fluctuation and correlation coefficients 263 6.3. Prediction of structural fluctuation 267 6.4. Prediction of correlation coefficients 270 7. Global mechanical rigidities of DNA nanostructures 272 7.1. Abstract 272 7.2. Methods 273 7.2.1. Estimation of persistence length from normal mode analysis 273 7.2.2. Theoretical estimation of persistence lengths 278 7.3. Prediction of bending and torsional persistence length 281 8. Conclusion 291 A. SNUPI (Structured NUcleic acids Programming Interface) 292 A.1. System requirement 292 A.2. Preparation for the analysis 293 A.3. General procedure 294 A.4. Examples 295 A.4.1. Example 1: Simple structural analysis using the default option 295 A.4.2. Example 2: Prediction of structural and dynamic properties 299 A.5. Analysis options 304 A.5.1. Finite element analysis option 304 A.5.2. Base-pair and crossover steps options 305 A.5.3. Single-stranded DNA options 306 A.5.4. Electrostatic interaction options 308 A.5.5. Normal mode analysis options 311 A.5.6. RMSF and correlation options 312 A.5.7. Configuration plot options 314 A.5.8. Output file options 315 Bibliography 317 Abstract in Korean 325Docto

    DNA-Topology Simplification by Topoisomerases

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    The topological properties of DNA molecules, supercoiling, knotting, and catenation, are intimately connected with essential biological processes, such as gene expression, replication, recombination, and chromosome segregation. Non-trivial DNA topologies present challenges to the molecular machines that process and maintain genomic information, for example, by creating unwanted DNA entanglements. At the same time, topological distortion can facilitate DNA-sequence recognition through localized duplex unwinding and longer-range loop-mediated interactions between the DNA sequences. Topoisomerases are a special class of essential enzymes that homeostatically manage DNA topology through the passage of DNA strands. The activities of these enzymes are generally investigated using circular DNA as a model system, in which case it is possible to directly assay the formation and relaxation of DNA supercoils and the formation/resolution of knots and catenanes. Some topoisomerases use ATP as an energy cofactor, whereas others act in an ATP-independent manner. The free energy of ATP hydrolysis can be used to drive negative and positive supercoiling or to specifically relax DNA topologies to levels below those that are expected at thermodynamic equilibrium. The latter activity, which is known as topology simplification, is thus far exclusively associated with type-II topoisomerases and it can be understood through insight into the detailed non-equilibrium behavior of type-II enzymes. We use a non-equilibrium topologicalnetwork approach, which stands in contrast to the equilibrium models that are conventionally used in the DNA-topology field, to gain insights into the rates that govern individual transitions between topological states. We anticipate that our quantitative approach will stimulate experimental work and the theoretical/computational modeling of topoisomerases and similar enzyme systems

    Lesion-induced DNA weak structural changes detected by pulsed EPR spectroscopy combined with site-directed spin labelling

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    Double electron-electron resonance (DEER) was applied to determine nanometre spinโ€“spin distances on DNA duplexes that contain selected structural alterations. The present approach to evaluate the structural features of DNA damages is thus related to the interspin distance changes, as well as to the flexibility of the overall structure deduced from the distance distribution. A set of site-directed nitroxide-labelled double-stranded DNA fragments containing defined lesions, namely an 8-oxoguanine, an abasic site or abasic site analogues, a nick, a gap and a bulge structure were prepared and then analysed by the DEER spectroscopic technique. New insights into the application of 4-pulse DEER sequence are also provided, in particular with respect to the spin probesโ€™ positions and the rigidity of selected systems. The lesion-induced conformational changes observed, which were supported by molecular dynamics studies, confirm the results obtained by other, more conventional, spectroscopic techniques. Thus, the experimental approaches described herein provide an efficient method for probing lesion-induced structural changes of nucleic acids

    DNA Conformational Changes and Phase Transitions Induced by Tension and Twist

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    DNA is a double stranded helical molecule with an intrinsic right handed twist. Its structure can be changed by applying forces and torques in single molecule experiments. In these experiments DNA has been seen to form super-helical structures (supercoils), collapse into tightly condensed states (toroids) and undergo structural changes (phase transitions). Our work focuses on studying all these phenomena by accounting for DNA elasticity, entropic effects due to thermal fluctuations and electrostatics. First, we study the DNA compaction problem in super-helices and toroidal structures. To do so we combine a fluctuating elastic rod model of DNA with electrostatic models for DNA-DNA interactions. Our models are able to predict the onset of the transition to supercoils and toroids under a wide range of experimental conditions. Next, we address DNA phase changes in the presence of mechanical loads.A phenomenon well known from experiments is the overstretching transition associated with the sudden change of DNA extension at high tensions. Depending on the ionic concentration, temperature and pulling rate, DNA can either transform into a melted state (inner strand separation) or S-DNA. Motivated by this, we study the equilibrium and kinetics of the DNA overstretching transitions making use of a quartic potential and non-gaussian integrals to evaluate the free energy of the system. We find that the cooperativity of the transition is a key variable that characterizes the overstretched state. In a separate study we make use of a heterogeneous fluctuating rod model to examine the hypothesis that a newly discovered left-handed form called L-DNA is a mixture of two relatively well-characterized DNA phases - S-DNA and Z-DNA. L-DNA is stable at high tensions and negative twist. We show that if the idea of a mixed state is correct, then the content of S-DNA and Z-DNA varies as a function of the ionic concentration. Finally, we also use our fluctuating rod model to study the mechanical properties of drug-DNA complexes. We show that our methods can predict the results of experiments from various labs if we use only one set of experiments to fit the data to our model

    The Effect of Active Site Mutations on the Homodimeric Behavior of the PvuII Restriction Endonuclease

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    The PvuII restriction endonuclease, a homodimer of two 18 kDa subunits, belongs to the type II family of restriction enzymes. Located in the active site of PvuII, Tyrosine 94 has previously been shown to be involved in the metal ion binding by the enzyme. The profile of the Ca2+ dependence of the DNA binding to the Y94F variant is shown to be clearly biphasic. The application of a sequential binding model yielded a coupling energy (ฮ”Gcoop) at -0.54 for the upper phase and -1.15 kcal/mole for the lower phase. The similar metal binding pattern between the Y94F and the WT PvuII for Mg2+, Ca2+, Tb3+ and Eu3+ in the absence of DNA is also shown. Through 1H-15N HSQC spectroscopy and chemical denaturation of the Y94F variant the conformational impact of Tyr94 is confirmed. The Y94F slightly repositions the metal ions in the active site of PvuII affecting the intra and/or inter-subunit interactions among the metal binding sites. The Single chain (SC) PvuII bearing a covalent linker between the two subunits is utilized in the exploration of the modes of cooperativity among the metal binding sites. The heterodimeric WT|E68A-SC PvuII was prepared and studied in parallel to the WT-SC homodimer. Global analysis of DNA binding isotherms at different Ca2+ concentrations for the WT|E68A-SC variant returned an intra-subunit ฮ”Gcoop at ?1.7 and -2.3 kcal/mole in the absence and presence of DNA, respectively. Combined with similar analysis for the WT-SC variant, the inter-subunit ฮ”Gcoop values are shown at -1.1 and -3.1 kcal/mole. It is shown that the effect of Ca2+ ions on DNA binding is greater than the effect of the DNA on the affinity for Ca2+ ions. The cleavage of plasmid DNA under single turnover conditions reveals a similar dependence of the nicking and linearization rates on the concentration of Mg2+ ions for the WT-SC and the WT|E68A-SC PvuII. The series of events leading to the linear product (DNA association, nicking, release of the intermediate, re-association and linearization) with Mg2+ ions in one PvuII subunit is not slower than the synchronized double strand cleavage with both PvuII subunits bearing Mg2+ ions
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