Magnesium-DNA interactions from interpretation of 25Mg-nmr relaxation rates: Field and coion dependence

We have used ²⁵Mg-nmr to investigate the binding of magnesium ions to double-stranded DNA. We have measured line shapes for ²⁵Mg in the presence of monodisperse calf thymus DNA (160 base pairs; b.p.) (magnesium : phosphate = 2.0) at two different field strengths, 11.75 T and 7.05 T, and used the isotropic model of two-site exchange developed by Westlund and Wennerstrom to simultaneously fit the line shapes at both field strengths. This model does not reproduce the observed field dependence. This is in contrast to a previous study [E. Berggren, L. Nordenskiold, and W. H. Braunlin (1992), Biopolymers, Vol. 32, pp. 1339–1350] in which a similar model of isotropic two-site exchange qualitatively reproduced the temperature dependence of the line widths. Relaxation rates were also measured as a function of magnesium : phosphate ratio and colon type. These measurements were used to assess the sensitivity of magnesium relaxation measurements to small changes in DNA structure induced by changes in the solvent environment. The temperature dependence of the line shape varies with the type of coion (chloride or sulfate) present. This coion dependence of the line shape is consistent with the coion dependence of the aggregation midpoint temperature reported by Bloomfield and co-workers [O. A. Knoll, M. G. Fried, and V. A. Bloomfield (1988) in Structure and Expres-sion, Vol. 2, R. H. Sarma and M. H. Sarma, Eds., Adenine Press, New York] and attributed to a lyotropic effect. These results suggest that even at low magnesium : phosphate ratios, relaxation parameters are specific to each magnesium–coion–DNA system. © 1994 John Wiley & Sons, Inc.     

Interpretation of 25Mg spin relaxation in Mg-DNA solutions: temperature variation and chemical exchange effects.

The temperature dependencies of line shapes and spin-lattice relaxation times T1 have been measured for 25Mg in dilute solutions of Na-DNA/NaCl containing varying amounts of added magnesium(II) ions. The 25Mg spectrum is clearly non-Lorentzian, due to the presence of motions modulating the quadrupolar interaction that are slow compared to the inverse of the Larmor frequency. The weakly temperature-dependent line shapes and relaxation rates appear to be influenced by the relatively slow exchange of the Mg2+ ions between the DNA surface and the aqueous bulk phase. The observed temperature dependencies depend on the ratio of total magnesium to DNA phosphate, Mg/P. The line shape as well as the temperature dependence of the line width at half height can be qualitatively reproduced with a two-site discrete exchange model for the quadrupolar relaxation of a spin 5/2 nucleus in isotropic solution. The calculations give a value of the lifetime for magnesium bound to DNA of 4 ms at room temperature. Previously reported temperature-dependent 43Ca relaxation measurements in DNA solution can be reproduced under the assumption of a mean lifetime of bound calcium that is not larger than 2 ms but not smaller than 50 microseconds at room temperature. The temperature variation of T1 for 25Mg has been calculated, giving some qualitative agreement with the data. The correlation time for bound 25Mg has been found to be about 40 ns at room temperature.     

Voltage-dependent processes in the electroneutral amino acid exchanger ASCT2

Neutral amino acid exchange by the alanine serine cysteine transporter (ASCT)2 was reported to be electroneutral and coupled to the cotransport of one Na⁺ ion. The cotransported sodium ion carries positive charge. Therefore, it is possible that amino acid exchange is voltage dependent. However, little information is available on the electrical properties of the ASCT2 amino acid transport process. Here, we have used a combination of experimental and computational approaches to determine the details of the amino acid exchange mechanism of ASCT2. The [Na⁺] dependence of ASCT2-associated currents indicates that the Na⁺/amino acid stoichiometry is at least 2:1, with at least one sodium ion binding to the amino acid–free apo form of the transporter. When the substrate and two Na⁺ ions are bound, the valence of the transport domain is +0.81. Consistently, voltage steps applied to ASCT2 in the fully loaded configuration elicit transient currents that decay on a millisecond time scale. Alanine concentration jumps at the extracellular side of the membrane are followed by inwardly directed transient currents, indicative of translocation of net positive charge during exchange. Molecular dynamics simulations are consistent with these results and point to a sequential binding process in which one or two modulatory Na⁺ ions bind with high affinity to the empty transporter, followed by binding of the amino acid substrate and the subsequent binding of a final Na⁺ ion. Overall, our results are consistent with voltage-dependent amino acid exchange occurring on a millisecond time scale, the kinetics of which we predict with simulations. Despite some differences, transport mechanism and interaction with Na⁺ appear to be highly conserved between ASCT2 and the other members of the solute carrier 1 family, which transport acidic amino acids.     

Influence of divalent magnesium ion on DNA: molecular dynamics simulation studies

A large amount of experimental evidence is available on the effect of magnesium ions on the structure and stability of DNA double helix. Less is known, however, on how these ions affect the stability and dynamics of the molecule. The static time average pictures from X-ray structures or the quantum chemical energy minimized structures lack understanding of the dynamic DNA–ion interaction. The present work addresses these questions by molecular dynamics simulation studies on two DNA duplexes and their interaction with magnesium ions. Results show typical B-DNA character with occasional excursions to deviated states. We detected expected stability of the duplexes in terms of backbone conformations and base pair parameter by the CHARMM-27 force field. Ion environment analysis shows that Mg²⁺ retains the coordination sphere throughout the simulation with a preference for major groove over minor. An extensive analysis of the influence of the Mg²⁺ ion shows no evidence of the popular predictions of groove width narrowing by dipositive metal ion. The major groove atoms show higher occupancy and residence time compared to minor groove for magnesium, where no such distinction is found for the charge neutralizing Na⁺ ions. The determining factor of Mg²⁺ ion’s choice in DNA binding site evolves as the steric hindrance faced by the bulky hexahydrated cation where wider major groove gets the preference. We have shown that in case of binding of Mg²⁺ to DNA non electrostatic contributions play a major role.

An animated Interactive 3D Complement (I3DC) is available in Proteopedia at http://proteopedia.org/w/Journal:JBSD:5     

A 43Ca-NMR study of Ca(II)-DNA interactions

High-field ⁴³Ca-nmr is applied to characterize the interactions of calcium ions with double-helical DNA. Under the conditions examined, ⁴³Ca lineshapes are always Lorentzian and single spin-lattice relaxation rates are obtained. The measured transverse and longitudinal relaxation rates are, however, not equal, which implies that the relaxation is in the near-extreme narrowing regime. Relative to the transverse relaxation rate, calcium ions near the DNA exchange rapidly with the bulk solution. The ⁴³Ca linewidths, spin-lattice relaxation rates, and chemical shifts observed over the course of a titration of DNA with calcium salt are not well described by simple electrostatic models. Deviations are most pronounced at low ratios of calcium to DNA phosphate. In contrast, at higher Ca/P ratios, the changes observed are well described by an electrostatic model based on the Poisson–Boltzmann equation. These results suggest that there is a small class of site-bound calcium as well as a large background of delocalized calcium electrostatically associated with the DNA. In contrast to previous studies of ²⁵Mg²⁺–DNA interactions, for which significant site-binding effects were also indicated, it appears rather easy to displace bound ⁴³Ca²⁺ by competition with sodium or magnesium cations. Unfortunately, neither these earlier results nor the present work allows a precise quantitation of the extent of site-bound divalent cation.     

Interactions of DNA with divalent metal ions. I. 31P-nmr studies

³¹P-nmr has been used to investigate the specific interaction of three divalent metal ions, Mg²⁺, Mn²⁺, and Co⁺², with the phosphate groups of DNA. Mg²⁺ is found to have no significant effect on any of the ³¹P-nmr parameters (chemical shift, line-width, T₁, T₂, and NOE) over a concentration range extending from 20 to 160 mM. The two paramagnetic ions, Mn²⁺ and Co²⁺, on the other hand, significantly change the ³¹P relaxation rates even at very low levels. From an analysis of the paramagnetic contributions to the spin–lattice and spin–spin relaxation rates, the effective internuclear metal–phosphorus distances are found to be 4.5 ± 0.5 and 4.1 ± 0.5 Å for Mn²⁺ and Co²⁺, respectively, corresponding to only 15 ± 5% of the total bound Mn²⁺ and Co²⁺ being directly coordinated to the phosphate groups (inner-sphere complexes). This result is independent of any assumptions regarding the location of the remaining metal ions which may be bound either as outer-sphere complexes relative to the phosphate groups or elsewhere on the DNA, possibly to the bases. Studies of the temperature effects on the ³¹P relaxation rates of DNA in the absence and presence of Mn²⁺ and Co²⁺ yielded kinetic and thermodynamic parameters which characterize the association and dissociation of the metal ions from the phosphate groups. A two-step model was used in the analysis of the kinetic data. The lifetimes of the inner-sphere complexes are 3 × 10^?7 and 1.4 × 10^?5 s for Mn²⁺ and Co²⁺, respectively. The rates of formation of the inner-sphere complexes with the phosphate are found to be about two orders of magnitude slower than the rate of the exchange of the water of hydration of the metal ions, suggesting that expulsion of water is not the rate-determining step in the formation of the inner-sphere complexes. Competition experiments demonstrate that the binding of Mg²⁺ ions is 3–4 times weaker than the binding of either Mn²⁺ or Co²⁺. Since the contribution from direct phosphate coordination to the total binding strength of these metal ion complexes is small (～15%), the higher binding strength of Mn²⁺ and Co²⁺ may be attributed either to base binding or to formation of stronger outer-sphere metal–phosphate complexes. At high levels of divalent metal ions, and when the metal ion concentration exceeds the DNA–phosphate concentration, the fraction of inner-sphere phosphate binding increases. In the presence of very high levels of Mg²⁺ (e.g., 3.1M), the inner-sphere ? outer-sphere equilibrium is shifted toward ～100% inner-sphere binding. A comparison of our DNA results and previous results obtained with tRNA indicates that tRNA and DNA have very similar divalent metal ion binding properties. A comparison of the present results with the predictions of polyelectrolyte theories is presented.     

Phase transition kinetics of phosphatidic acid bilayers A stopped-flow study of the electrostatically induced transition

The kinetics of the electrostatically induced phase transition of dimyristoyl phosphatidic acid bilayers was followed using the stopped-flow technique. The phase transition was triggered by a fast change in the pH or the magnesium ion concentration and followed by recording the time dependence of the absorbance. When the phase transition was induced by a pH jump the time course of the absorbance could be described by two exponentials, their time constants displaying the for cooperative processes characteristic maximum at the transition midpoint. The time constants are in the 10 and 100 ms range for the H⁺ triggered transition from the fluid to the ordered state. A third slower process shows no appreciable temperature dependence and is probably caused by vesicle aggregation. For the OH^--induced transition fron the ordered to the fluid state the time constants are in the 100 and 1000 ms range. The fluid-ordered transition could also be triggered by addition of magnesium ions. Of the several observed processes only the fastest in the 10–100 ms time range could definitely be assigned to the fluid-ordered transition while the others are due to aggregation phenomena. The experimental data were compared with results obtained from pressure jump experiments and could be interpreted on the basis of theories for non-equilibrium relaxation.     

Coordinate repression of cholesterol biosynthesis and cytoplasmic 3-hydroxy-3-methylglutaryl coenzyme A synthase by glucocorticoids in HeLa cells.

The stability constants for the calcium and magnesium complexes of rhodanese are >10⁵m^?1 at both high and low substrate concentrations. The stoichiometry of alkaline earth metal ion binding totals close to 1 per 18,500 molecular weight. The usual assay reagents contain sufficient amounts of these metal ions to maintain added enzyme in its metal-complexed form. When reaction mixtures are treated with oxalate to remove calcium ions, inhibition of rhodanese activity is virtually complete under circumstances such that the contribution of magnesium ion is low.Zinc and a number of transition metal ions are inhibitors of rhodanese activity. Studies of the concentration dependence of these effects with zinc, copper, and nickel showed that: 1) Some cyanide complexes of these metals are competitive with the donor substrate, thiosulfate ion. The binding of the copper and zinc complexes is mutually competitive. 2) Another cyanide species of copper appears to combine with the free enzyme to form a functionally active complex. 3) The zinc cyanide species with a net positive charge is an inhibitor competitive with the acceptor substrate, cyanide ion.All of these observations are consistent with a model in which metal ions serve as the electrophilic site of rhodanese.     

Effects of calcium and manganese ions on the helix–coil transition of DNA

The thermal denaturation method was employed to study the effect of Ca²⁺ and Mn²⁺ ions on the DNA helix–coil transition parameters at Na⁺ concentrations of 10^?3–10^?1M. At low ion concentrations, thermal stability increases, the melting range passes through a maximum, and the denaturation curves become asymmetric. These changes are quantitatively similar for Mn²⁺ and Ca²⁺ ions. With a further increase in the concentration of bivalent ions, the conformational transition temperatures pass through a maximum, and the melting range first tends to saturation and then rapidly decreases to 1–2°C. The Mn²⁺ concentrations, at which the above effects occur, are an order of magnitude lower than the Ca²⁺ concentrations. Comparison of experimental results and calculation in terms of the ligand theory permitted estimation of binding constants characterizing association between Mn²⁺ and Ca²⁺ ions and bases of native and denatured DNA. We show that, unlike the interaction with phosphates, bivalent ion–DNA base binding is weakly dependent on monovalent ion concentration in the solution.     

Influence of magnesium ions on helix-coil transition of DNA determined by modified differential scanning calorimeter

The thermal effect of magnesium ions on the helix–coil transition of DNA was studied calorimetrically by a modified differential scanning calorimeter (DSC). It was found that the transition temperature of DNA depends on both the DNA and magnesium ion concentrations. The dependence of the helix–coil transition of DNA on the mole ratio of magnesium ions to DNA(P) can be classified into two groups. When this mole ratio is less than 1, magnesium ions tend to stabilize the double-helix DNA, so that the transition temperature increases linearly and the heat of transition increases significantly with increasing mole ratio. When the mole ratio is more than 1, magnesium ions tend to destabilize the double-helix DNA, so that DNA precipitates when the temperature is raised above the transition temperature. In this case, both the transition temperature and the heat of transition decrease with increasing mole ratio.     

Coordination of iron ions in the form of histidinyl dinitrosyl complexes does not prevent their genotoxicity

Formation of dinitrosyl iron complexes (DNICs) was observed in a wide spectrum of pathophysiological conditions associated with overproduction of NO. To gain insight into the possible genotoxic effects of DNIC, we examined the interaction of histidinyl dinitrosyl iron complexes (HIS-DNIC) with DNA by means of circular dichroism. Formation of DNIC was monitored by EPR and FT/IR spectroscopy. Vibrational bands for aquated HIS-DNIC are reported. Dichroism results indicate that HIS-DNIC changes the conformation of the DNA in a dose-dependent manner in 10 mM phosphate buffer (pH 6). Increase of the buffer pH or ionic strength decreased the effect. Comparison of HIS-DNIC DNA interaction with the effect of hydrated Fe²⁺ ion revealed many similarities. The importance of iron ions in HIS-DNIC induced genotoxicity is confirmed by plasmid nicking assay. Treatment of pUC19 plasmid with 1 μM HIS-DNIC did not affect the plasmid supercoiling. Higher concentrations of HIS-DNIC induced single strand breaks. The effect was completely abrogated by addition of deferoxamine, a specific strong iron chelator. Our data reveal that formation of HIS-DNIC does not prevent DNA from iron-induced damage and imply that there is no direct interrelationship between iron–NO coordination and their mutual toxicity modulation.     

Interaction of deoxyribonucleic acid with anthracenedione derivatives

Spectrophotometric, calorimetric and chrioptical techniques have been used to investigate the interaction of two new anthracenedione derivatives, 1-(ω-diethylaminopropylamido)-4-hydroxy-9,10-anthracenedione hydrochloride (I) and 1-(ω)-diethylaminopropylamido)-2-methoxy-4-hydroxy-9,10-anthracenedione hydrochloride (II) to DNA. Measurements were carried out at four different Na⁺ concenetrations. From the dependence of the binding constant on ionic strength the number of ion pairs formed between the ligand and DNA, along with the binding free energy were estimated. Calorimetric measurements show that the binding process is exothermic for both ligands. Experiments carried out with DNA from various sources indicate no marked preference for G-C or A-T binding sites. Compounds I and II increase the T_m for DNA melting by more than 25°C at high drug/base pair ratios. Circular dichroism studies indicate that the structural properties of DNA are substantially affected by the interaction with the above mentioned compounds. All data from these studies are consistent with an intercalative mechanism of binding for the anthracendione derivatives to DNA.     

Additive Modulation of DNA-DNA Interactions by Interstitial Ions

Quantitative understanding of biomolecular electrostatics, particularly involving multivalent ions and highly charged surfaces, remains lacking. Ion-modulated interactions between nucleic acids provide a model system in which electrostatics plays a dominant role. Using ordered DNA arrays neutralized by spherical cobalt³⁺ hexammine and Mg²⁺ ions, we investigate how the interstitial ions modulate DNA-DNA interactions. Using methods of ion counting, osmotic stress, and x-ray diffraction, we systematically determine thermodynamic quantities, including ion chemical potentials, ion partition, DNA osmotic pressure and force, and DNA-DNA spacing. Analyses of the multidimensional data provide quantitative insights into their interdependencies. The key finding of this study is that DNA-DNA forces are observed to linearly depend on the partition of interstitial ions, suggesting the dominant role of ion-DNA coupling. Further implications are discussed in light of physical theories of electrostatic interactions and like-charge attraction.     

Characterization of micellar-packaged gramicidin A channels.

The effects of heating, on an aqueous gramicidin A lysolecithin system, were examined by carbon-13 nuclear magnetic resonance (¹³C-NMR), circular dichroism (CD), and sodium-23 nuclear magnetic resonance (²³Na-NMR), and the results are collectively interpreted to indicate micellar-packaging of gramicidin channels and cation occupancy in the channel. ¹³C-NMR of the gramicidin-lysolecithin system demonstrates a decrease in mobility of the micellar lipid on heating which is indicative of incorporation of gramicidin into the hydrophobic core of the micelle. A unique and reproducible CD spectrum is obtained for the heat incorporated state. Sodium-23 spin-lattice relaxation times (T₁) demonstrated sodium interaction to be dependent on heat incorporation. The T₁ identified interaction is blocked by silver ion which is known to block sodium transport through the channel in lipid bilayer studies. The temperature dependence of the sodium-23 line width defines an exchange process with an activation energy of 6.8 kcal/mole which is essentially the same as the activation energy reported for transport through the channel in lecithin bilayer studies, and the sodium exchange process is blocked by thallium ion which is also known to block sodium transport through the channel.     

Buoyant density and solvation of magnesium DNA

The buoyant density of T-4 DNA was determined by equilibrium sedimentation in a density gradient, of mixed solutions of cesium and magnesium chlorides and bromides. The preferential hydration was calculated from these data, allowing appropriately for the exchange equilibrium of DNA with Cs⁺ and Mg⁺⁺ ions. The charge and intrinsic solvation of the counterions were found to have no appreciable effect on the hydration of the DNA, the extent of solvation depending only on the thermodynamic, activity of the water. Various reasonable hypotheses are discussed to account for these results.     

Interaction of metal ions with gastrointestinal hormones: Binding studies of Mg++ to biologically active analogs of little gastrin and minigastrin

The interaction of magnesium ions with Des-Trp¹-Nle¹²-minigastrin I (Nle¹¹-HG-13) and Nle¹¹⁵-little gastrin I (Nle¹⁵-HG-17) has been studied by CD and spectrophotometric techniques in trifluoroethanol. Spectrophotometric titrations using murexide as a metallochromic indicator showed that there are three binding sites for magnesium ions in Nle¹¹-HG-13, with binding constants of the order of (6 ± 2) × 10⁶, (1.7 ± 0.5) × 10⁶, and (5.0 ± 0.5) × 10⁵M^?1. These figures have been independently confirmed by CD measurements in the far-uv in the presence of increasing amounts of magnesium ions. Elongation of the peptide chain from Nle¹¹-HG-13 to Nle¹⁵-HG-17 does not provide any additional binding site for the metal ions. In both hormones, we have observed different responses in the near- and fur-uv CD properties with regard to added magnesium. The intensity of the CD bands in the aromatic region changes cooperatively with the ion/hormone molar ratio. These findings lead us to conclude that at the C-terminal, the biologically important sequence, -Trp-Nle-Asp-Phe-Nh₂, is directly involved in the interaction with magnesium.     

High affinity DNA-microtubule associated protein interaction

We have isolated the MAP/tau proteins from twice-cycled chick brain microtubule preparations and demonstrated that they are responsible for the nitrocellulose DNA binding activity we and others have measured. Using the isolated MAP/tau proteins we then measured the apparent affinity constant K_app for the homologous chick DNA interaction and found evidence for two equilibrium affinity classes-a K_app = 6 × 10⁷ M^–1, responsible for the bulk of the DNA binding activity and a small (< 10%) higher affinity K_app = 10⁸ – 10⁹ M^–1, likely due to sequence specific binding protein species. Using the same chick brain MAP-tau protein, a heterologous interaction with D. melanogaster DNA, was found to possess just the lower affinity class-K_app = 2 × 10⁷ M^–1. Under stringent binding conditions we carried out equilibrium nitrocellulose filter binding experiments in a ternary reaction mixture at constant MAP/tau protein and ³⁵S radiolabelled chick DNA concentration using increasing and excess concentrations of competitor DNAs of different sources. The order of competitor strengths found was-chick DNA > mouse DNA > D. melanogaster = E. coli. DNA. These data and specifically the homologous DNA: protein case being the strongest competitor corroborate our previous studies using total microtubule protein and provide new evidence for a conserved interaction of a small DNA sequence class with MAP/tau protein species. Moreover, these data allow us to conclude that the conserved DNA sequence: MAP/tau protein interactions do not critically depend upon any energetic feature co-involving tubulin for their properties since tubulin is absent from these preparations.     

Interaction between proteins and salt solutions. IV. Enrichment of salts in collagen during denaturation

Using ¹⁴C-labeled KSCN and ³⁶Cl-labeled KC1, we have determined the selective removal of ions and water by fibrous, crosslinked collagen both below and above the denaturation temperatures at several molarities under or near isoelectric conditions. The results for KSCN show there is an increase in ion binding at the denaturation temperature. These data, in conjunction with date from the literature, have been used to evaluate binding constants and mole fractions of available binding sites, as well as the free energy of binding various salts to collagen and gelatin. The values so obtained correlate satisfactorily with similar quantities obtained from the experimental dependence of the shrinkage temperature of collagen on salt concentration using a simple theory for the melting point depression which includes the effect of binding in the denatured state. Salting-out agents show negligible binding to the protein, and this confirms the earlier finding that the interaction between these agents and the protein can be approximately described by conventional polymer–diluent theories which do not consider ion binding. Also, an analysis of the role of unequal anion and cation binding is presented.     

Light-scattering study of DNA condensation: Competition between collapse and aggregation

Light-scattering studies were done to investigate the DNA collapse transition, a large and discontinuous reduction in the radius of gyration. Of particular concern was differentiating the compaction of a single DNA molecule from aggregation. Solutions of RK2 plasmid DNA (M_r = 37 × 10⁶) or bacteriophage T7 DNA (M_r = 25 × 10⁶) were titrated with the condensing reagents spermidine in aqueous solvent or magnesium ion in ethanol–water solvent. The transition was followed by the change in scattering at a single angle or by the change in the angular dependence of scattering. At concentrations below 1 μg/mL, only aggregation could be detected by observation at a single angle; therefore, to study the collapse transition, it was necessary to measure the angular dependence of scattering. The intensities measured between the angles 30° and 60° were fit to known scattering functions. At low concentrations of the condensing reagent, the data were consistent with the scattering function of a random coil. On the other hand, during the transition at higher reagent concentrations, the curve that fit the data required two components—the scattering function for a random coil with a large radius of gyration, plus that for a sphere with a radius about one-fifth of that of the coil. The fractional concentration of the sphere increased with increasing condensing-reagent concentration. This two-component behavior is in apparent contrast to the situation with a more flexible polymer such as polystyrene, in accord with theoretical predictions. At still higher reagent concentrations, aggregation was apparent. Condensation to a collapsed state was reversible without hysteresis, while dissolution of the aggregated state nearly always occurred with hysteresis. Qualitative agreement between the observed DNA collapse transition and the theoretical phase diagram presented in the preceding paper was found, although the light-scattering results did not show quantitative agreement with the simple theoretical model.     

Determining the Locations of Ions and Water around DNA from X-Ray Scattering Measurements

Nucleic acids carry a negative charge, attracting salt ions and water. Interactions with these components of the solvent drive DNA to condense, RNA to fold, and proteins to bind. To understand these biological processes, knowledge of solvent structure around the nucleic acids is critical. Yet, because they are often disordered, ions and water evade detection by x-ray crystallography and other high-resolution methods. Small-angle x-ray scattering (SAXS) is uniquely sensitive to the spatial correlations between solutes and the surrounding solvent. Thus, SAXS provides an experimental constraint to guide or test emerging solvation theories. However, the interpretation of SAXS profiles is nontrivial because of the difficulty in separating the scattering signals of each component: the macromolecule, ions, and hydration water. Here, we demonstrate methods for robustly deconvoluting these signals, facilitating a more straightforward comparison with theory. Using SAXS data collected on an absolute intensity scale for short DNA duplexes in solution with Na⁺, K⁺, Rb⁺, or Cs⁺ counterions, we mathematically decompose the scattering profiles into components (DNA, water, and ions) and validate the decomposition using anomalous scattering measurements. In addition, we generate a library of physically motivated ion atmosphere models and rank them by agreement with the scattering data. The best-fit models have relatively compact ion atmospheres when compared to predictions from the mean-field Poisson-Boltzmann theory of electrostatics. Thus, the x-ray scattering methods presented here provide a valuable measurement of the global structure of the ion atmosphere that can be used to test electrostatics theories that go beyond the mean-field approximation.