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M T Record

Publications and source records attributed to M T Record.

At least 19 recordsLinked to original sources

Binding of cationic (+4) alanine- and glycine-containing oligopeptides to double-stranded DNA: thermodynamic analysis of effects of coulombic interactions and alpha-helix induction.

Coulombic interactions and coupled conformational changes make important contributions to stability and specificity of many protein-nucleic acid complexes. As models of these phenomena in simpler systems, we have investigated the binding to mononucleosomal (160 base-pair) calf thymus DNA of a high charge density (compact) 5-residue (+4) oligopeptide (with 4 lysines and 1 tryptophan) and of four lower charge density (extended) 17-residue (+4) oligopeptides (each with 4 lysines, 10-12 alanines, 0-2 glycines, and 1 tryptophan). The fractional helicity (f(h)) of each oligopeptide before and after DNA binding was determined using circular dichroism. At low univalent cation concentration ([M+] = 6.4 mM), binding to DNA increases f(h) significantly for all but one of the extended oligopeptides. Oligopeptide-DNA binding constants (K(obs)) and apparent binding site sizes (n) were quantified using the noncooperative McGhee-von Hippel isotherm to fit tryptophan fluorescence quenching data. For each of the oligopeptides studied, n is found to be approximately equal to four, the number of lysine charges. In the range 6.4 mM < or = [M+] < or = 21.5 mM, power dependences of K(obs) on [M+] (SK(obs) = d log K(obs)/d log[M+]) for all 17-residue (+4) oligopeptides are similar with an average value of -3.7 +/- 0.4, which is indistinguishable (outside uncertainty) from the value obtained here for the compact (+4) oligopeptide and from values reported elsewhere for another compact tetralysine and for spermine (+4). Our results are consistent with the conclusion that the nonspecific binding to DNA of all these tetravalent ligands is driven primarily by coulombic interactions. At any [M+] investigated, values of K(obs) for the four extended (+4) oligopeptides differ by less than an order of magnitude, but all are 1-2 orders of magnitude less than values of K(obs) for two compact (+4) oligopeptides and for spermine. The differences in K(obs) for oligopeptide-DNA complexes, which all have similar n and similar SK(obs) indicate that when an extended oligopeptide binds to DNA it becomes more compact as a result of conformational changes, such as the additional alpha-helix formation detected by circular dichroism.

Alanine

Thermodynamics of the interactions of lac repressor with variants of the symmetric lac operator: effects of converting a consensus site to a non-specific site.

What are the thermodynamic consequences of the stepwise conversion of a highly specific (consensus) protein-DNA interface to one that is nonspecific? How do the magnitudes of key favorable contributions to complex stability (burial of hydrophobic surfaces and reduction of DNA phosphate charge density) change as the DNA sequence of the specific site is detuned? To address these questions we investigated the binding of lac repressor (LacI) to a series of 40 bp fragments carrying symmetric (consensus) and variant operator sequences over a range of temperatures and salt concentrations. Variant DNA sites contained symmetrical single and double base-pair substitutions at positions 4 and/or 5 [sequence: see text] in each 10 bp half site of the symmetric lac operator (Osym). Non-specific interactions were examined using a 40 bp non-operator DNA fragment. Disruption of the consensus interface by a single symmetrical substitution reduces the observed equilibrium association constant (K(obs)) for Osym by three to four orders of magnitude; double symmetrical substitutions approach the six orders in magnitude difference between specific and non-specific binding to a 40 bp fragment. At these adjacent positions in the consensus site, the free energy effects of multiple substitutions are non-additive: the first reduces /deltaG(obs)o/ by 3 to 5 kcal mol(-1), approximately halfway to the non-specific level, whereas the second is less deleterious, reducing /deltaG(obs)o/ by less than 3 kcal mol(-1). Variant-specific dependences of K(obs) on temperature and salt concentration characterize these LacI-operator interactions. In general, binding constants and standard free energies of binding both exhibit characteristic extrema near 290 K. As a consequence, both the enthalpic and entropic contributions to stability of Osym and variant complexes change from positive (i.e. entropy driven) at lower temperatures to negative (i.e. enthalpy driven) at higher temperatures, indicating that the heat capacity change upon binding, deltaC(obs)o, is large and negative. In general, /deltaC(obs)o/ decreases as the specificity and stability of the variant complex decreases. Stabilities of complexes of LacI with Osym and all variant operators are strongly [salt]-dependent. Binding constants for the variant complexes exhibit a power-dependence on [salt] that is larger in magnitude (i.e. more negative) than for Osym, but no obvious trend relates changes in contributions from the polyelectrolyte effect and the observed reductions in stability (delta deltaG(obs)o). These variant-specific thermodynamic signatures provide novel insights into the consequences of converting a consensus interface to a less specific one; such insights are not obtained from comparisons at the level of delta deltaG(obs)o. We propose that this variant-specific behavior arises from a strong effect of operator sequence on the extent of induced conformational changes in the protein (and possibly also in the DNA site) which accompany binding.

Bacterial Proteins

Thermodynamic characterization of interactions of native bovine serum albumin with highly excluded (glycine betaine) and moderately accumulated (urea) solutes by a novel application of vapor pressure osmometry.

The thermodynamic consequences of interactions of native bovine serum albumin (BSA) with two smaller solutes (glycine betaine or urea) in aqueous solution are characterized by a novel application of vapor pressure osmometry (VPO), which demonstrates the utility of this method of investigating preferential interactions involving solutes that are either accumulated or excluded near the surface of a protein. From VPO measurements of osmolality (water activity) as a function of the solute concentration in the presence and absence of BSA, we determine the dependence of the solute molarity (C3) on that of BSA (C2) at fixed temperature (37 degrees C), pressure (approximately 1 atm), and osmolality (over the range 0-1.6 molal). After some thermodynamic transformations, these results yield values of [formula: see text] which characterizes the interdependence of solute molalities when temperature, pressure, and the chemical potential of solute 3 are fixed. This form of the preferential interaction coefficient can be interpreted directly in terms of the molecular exclusion or accumulation of the solute (relative to water) near the protein surface. Within experimental uncertainty, [formula: see text] is proportional to m3 both for glycine betaine (0-0.9 m) and for urea (0-1.6 m). For glycine betaine [formula: see text] = -49 +/- 4, a value consistent with the interpretation that this solute is completely excluded from the hydrated surface of BSA, whereas for urea [formula: see text] = 6 +/- 1, which indicates a moderate extent of accumulation at the surface of native BSA. The preferential accumulation of solutes (e.g., urea) that have some binding affinity for a protein can be quantified and interpreted using the two-domain model if the extent of hydration of the protein has been determined using a completely excluded solute (e.g., glycine betaine). Complete exclusion from the local hydration domain surrounding proteins, if general, justifies the use of glycine betaine as a thermodynamic probe of the changes in hydration that accompany protein folding, protein association, and protein-ligand binding interactions.

Betaine

Cooperative and anticooperative effects in binding of the first and second plasmid Osym operators to a LacI tetramer: evidence for contributions of non-operator DNA binding by wrapping and looping.

The interaction of lac operator DNA with lac repressor (LacI) is a classic example of a genetic regulatory switch. To dissect the role of stoichiometry, subunit association, and effects of DNA length in positioning this switch, we have determined binding isotherms for the interaction of LacI with a high affinity (Osym) operator on linearized plasmid (2500 bp) DNA over a wide range of macromolecular concentrations (10(-14) to 10(-8) M). Binding data were analyzed using a thermodynamic model involving four equilibria: dissociation of tetramers (T) into dimers (D), and binding of operator-containing plasmid DNA (O) to dimers and tetramers to form three distinct complexes, DO, TO, and TO2. Over the range of concentrations of repressor, operator, and salt (0.075 M K+ to 0.40 M K+) investigated, we find no evidence for any significant thermodynamic effect of LacI dimers. Instead, all isotherms can be interpreted in terms of just two equilibria, involving only T and the TO and TO2 complexes. As a reference binding equilibrium, which we propose must approximate the DO binding interaction, we compare the plasmid Osym results with our extensive studies of the binding of a 40 bp Osym DNA fragment to LacI. On this basis, we obtain a lower bound on the LacI dimer-tetramer equilibrium constant and values of the equilibrium constants for formation of TO and TO2 complexes. At a salt concentration of 0.40 M, the Osym plasmid binding data are consistent with a model with two independent and identical binding sites for operator per LacI tetramer, in which the binding to a site on the tetramer is only slightly more favorable than the reference binding interaction. Increasingly large deviations from the independent-site model are observed as the salt concentration is reduced; binding of a second operator to from TO2 becomes strongly disfavored relative to formation of TO at low salt concentrations (0.075 to 0.125 M). In addition, binding of both the first and second plasmid operator DNA molecules to the tetramer becomes increasingly more favorable than the reference binding interaction as [K+] is reduced from 0.40 M to 0.125 M. At 0.075 M K+, however, the strength of binding of the second plasmid operator DNA to the LacI tetramer is dramatically reduced; this interaction is much less favorable than binding the first plasmid operator DNA, and becomes much less favorable than the reference binding interaction. We propose that these differences arise from changes in the nature of the TO and TO2 complexes with decreasing salt concentration. At low salt concentration, we suggest the hypothesis that flanking non-operator sequences bind non-specifically (coulombically) by local wrapping, and that distant regions of non-operator DNA occupy the second operator-binding site by looping. We propose that wrapping stabilizes both 1:1 and 2:1 complexes at low salt concentration, and that looping stabilizes the 1:1 complex but competitively destabilizes the 2:1 TO2 complex at low salt concentration. These effects must play a role in adjusting the stability and structure of the LacI-lac operator repression complex as the cytoplasmic [K+] varies in response to changes in extracellular osmolarity.

Bacterial Proteins

Compensating effects of opposing changes in putrescine (2+) and K+ concentrations on lac repressor-lac operator binding: in vitro thermodynamic analysis and in vivo relevance.

Ion concentrations (K+, Glu-) in the cytoplasm of growing Escherichia coli cells increase strongly with increases in the osmolarity of a defined growth medium. While in vitro experiments demonstrate that the extent of protein-nucleic acid interactions (PNAI) depends critically on salt concentration, in vivo measurements indicate that cells maintain a relatively constant extent of PNAI independent of the osmolarity of growth. How do cells buffer PNAI against changes in the cytoplasmic environment? At high osmolarity, the increase in macromolecular crowding which accompanies the reduction in amount of cytoplasmic water in growing cells appears quantitatively sufficient to compensate for the increase in [K+]. At low osmolarity, however, changes in crowding appear to be insufficient to compensate for changes in [K+], and additional mechanisms must be involved. Here we report quantitative determinations of in vivo total concentrations of polyamines (putrescine(2+), spermidine(3+)) as a function of osmolarity (OsM) of growth, and in vitro binding data on the effects of putrescine concentration on a specific PNAI (lac repressor-lac operator) as a function of [K+]. The total concentration of putrescine in cytoplasmic water decreases at least eightfold from low osmolarity (approximately 64 mmol (l H2O)-1 at 0.03 OsM) to high osmolarity (approximately 8 mmol (l H2O)-1 at 1.02 OsM). Over this osmotic range the total [K+] increases from approximately 0.2 mol (l H2O)-1 to approximately 0.8 mol (lH2O)-1. We find that the effect of putrescine concentration on the repressor-operator interaction in vitro is purely competitive and is quantitatively described by a simple competition formalism in which lac repressor behaves a a specific-binding oligocation (ZR = 8+/-3). We demonstrate that this thermodynamic result is consistent with a structural analysis of the number of positively charged side-chains on two DNA binding domains of repressor which interact with the phosphodiester backbone of the operator site. Since this oligocation character of the binding surface of DNA-binding proteins appears to be general, we propose the competitive effects of putrescine and K+ concentrations on the strength of specific binding are general. At low osmolarity, compensating changes in putrescine and K+ concentration in response to changes in external osmolarity provide a general mechanism for E. coli to vary cytoplasmic osmolarity while maintaining a constant extent of PNAI.

Base Sequence

Large electrostatic differences in the binding thermodynamics of a cationic peptide to oligomeric and polymeric DNA.

Results presented here demonstrate that the thermodynamics of oligocation binding to polymeric and oligomeric DNA are not equivalent because of long-range electrostatic effects. At physiological cation concentrations (0.1-0.3 M) the binding of an oligolysine octacation KWK6-NH2 (+8 charge) to single-stranded poly(dT) is much stronger per site and significantly more salt concentration dependent than the binding of the same ligand to an oligonucleotide, dT(pdT)10 (-10 charge). These large differences are consistent with Poisson-Boltzmann calculations for a model that characterizes the charge distributions with key preaveraged structural parameters. Therefore, both the experimental and the theoretical results presented here show that the polyelectrolyte character of a polymeric nucleic acid makes a large contribution to both the magnitude and the salt concentration dependence of its binding interactions with simple oligocationic ligands.

Cations

HO. and DNase I probing of E sigma 70 RNA polymerase--lambda PR promoter open complexes: Mg2+ binding and its structural consequences at the transcription start site.

Chemical and enzymatic probing (footprinting) of the reactivity of the promoter DNA backbone is applied to characterize two binary open complexes RPo1 (-Mg2+) and RPo2 (+Mg2+), formed by Escherichia coli RNA polymerase (E sigma 70) at the lambda PR promoter. We report that HO. detects major differences in backbone reactivity between RPo1 and RPo2 in the open region from -4 to +1 relative to the transcription start site. Deoxyribose sugars at positions -4 to +1 of the t (template) strand react with HO. in RPo2 but are relatively protected in RPo1. Binding of Mg2+ to convert RPo1 to RPo2 therefore increases the reactivity of two negatively charged footprinting agents [MnO4-; Suh, W.-C., Ross, W., & Record, M. T., Jr., (1993) Science 259, 358-361; and Fe(EDTA)2-/HO.] at the start site and is required for binding of the negatively-charged initiating nucleotides to the polymerase and the t strand at the start site. We propose that these effects result from binding of two Mg2+ ions to the catalytic carboxyls in the nucleotide binding sites. Except for the key region on the t strand at the start site, the promoter DNA of both RPo1 and RPo2 is continuously protected from DNase I and hydroxyl radical (HO.) cleavage between the -12 and +25 promoter positions. Protection in the upstream region, extending from -13 to about -70, is periodic, with an 11 base pair periodicity indicative of binding of polymerase to a single face of the DNA helix.(ABSTRACT TRUNCATED AT 250 WORDS)

Bacteriophage lambda

Thermodynamic investigation of hirudin binding to the slow and fast forms of thrombin: evidence for folding transitions in the inhibitor and protease coupled to binding.

Temperature dependent studies of the interaction of the clotting enzyme thrombin with the potent natural inhibitor hirudin reveal a large negative heat capacity change of -1.7(+/- 0.2) kcal/mol per K associated with the formation of the thrombin-hirudin complex, independent of the allosteric state of the enzyme. Binding of N-terminal fragments of hirudin (hir1-49 and hir1-43) is characterized by heat capacity changes of -1.2(+/- 0.1) and -0.9(+/- 0.1) kcal/mol per K, respectively. The magnitude of these heat capacity changes is unprecedented for protease-inhibitor interactions. A thermodynamic analysis based on observed heat capacity and entropy changes predicts that binding is accompanied by substantial coupled folding transitions in both hirudin and thrombin. In the absence of a structure of free thrombin, analysis of differences in the predicted number of residues which fold upon binding hirudin and its fragments leads to the following structural model: three surface loops in thrombin (W60d, W148 and fibrinogen binding loops) are disordered in the free state and fold upon formation of the thrombin-hirudin complex. Molecular dynamics simulations, run over a time scale of 5 ps, are consistent with the hypothesis of large scale coupled folding transitions in both hirudin and thrombin upon formation of the complex. Comparison of the thermodynamics for the interaction of hirudin with the slow and fast forms of thrombin allows dissection of the coupling free energy for allosteric switching. The coupling free energy for the slow-->fast transition increases linearly, in absolute value, with temperature. The coupling enthalpy and entropy terms for hirudin were found to be delta Hoc = 12(+/- 1) kcal/mol and delta Soc = 47(+/- 4) cal/mol per K. Preferential interaction with the fast form is therefore due to the balance of two opposite forces, both quite large in magnitude. The contribution of enthalpic effects opposes the slow-->fast transition and stabilizes binding to the slow form. The contribution of entropic effects favors the slow-->fast transition and stabilizes binding to the fast form. In the physiological temperature range the entropic effects prevail and result in preferential binding of hirudin to the fast form. The region of thrombin recognizing the N-terminal domain of hirudin contains most of the residues that are energetically linked to the slow-->fast transition. This region is part of the "allosteric core" of thrombin and includes the W60d loop, shaping the specificity site S2, and the Na+ binding loop connecting the last two beta-strands of the B chain.

Allosteric Regulation

K(+)-ribosome interactions determine the large enhancements of 39K NMR transverse relaxation rates in the cytoplasm of Escherichia coli K-12.

As a probe of physical chemical properties of the intracellular environment, we measured 39K NMR transverse relaxation rates in concentrated cell slurries of Escherichia coli K-12 grown in minimal medium over a range of osmolarities (from 0.1 to 1.0 OsM) and after plasmolysis. The 39K transverse relaxation at a resonance frequency of approximately 18.67 MHz is biexponential under all conditions, and 100% of the expected signal intensity is detected. Both components of the 39K NMR transverse relaxation are very fast, and the difference between the fast and slow relaxation rates is very large compared to previous measurements on 23Na and 39K in protein and nucleic acid solutions in vitro. The 39K transverse relaxation rates decrease as the osmolarity of the growth media increases but increase dramatically when cells grown in 0.1 OsM media are plasmolyzed at 1.0 OsM. The homogeneous nature and the 100% visibility of the 39K signal indicate the existence of fast exchange among the multiple, magnetically distinguishable populations of 39K which probably exist in the cytoplasm. The absence of static quadrupolar splitting of the cytoplasmic 39K signal (as indicated by a single peak in the spectrum) indicates that the cytoplasm, as probed by 39K NMR, behaves like a concentrated but isotropic nucleic acid solution rather than an anisotropic nucleic acid liquid crystal. To understand the origins of the striking NMR relaxation behavior of 39K in viable cells, we have investigated NMR transverse relaxation rates of 39K (and also 23Na and 35Cl) in E. coli 50S and 70S ribosome solutions in vitro. At concentrations of ions and of ribosomes that to the extent possible mimic those of the cytoplasm of E. coli, we find that 39K, 23Na, and 35Cl transverse relaxation rates all exhibit biexponential behavior, and 39K and 23Na exhibit the large magnitudes and the large difference between the slow and the fast relaxation rates observed in viable cells. These polyanionic ribosome solutions are the only in vitro model system discovered to date that exhibits 39K transverse relaxation rates comparable to those in viable cells. We conclude that K(+)-ribosome interactions are the dominant source of the NMR properties of K+ in E. coli.(ABSTRACT TRUNCATED AT 400 WORDS)

Cytoplasm

Inhibition of transcription initiation by lac repressor.

Initiation of transcription of the lac operon by RNA polymerase (R) is inhibited by binding of lac repressor (L) to an operator site which overlaps the lac promoter (P). We have investigated repression of the lac UV5 promoter in vitro for a choice of the repressor--operator binding constant and ranges of thermodynamic activities of L and R which appear to be relevant in vivo. Effects of [L] on the extent of formation and the kinetics of association and dissociation of abortively-initiating open complexes (RPinit) were examined using fluorescence detected abortive initiation and KMnO4 chemical probing. The nitrocellulose filter assay was used to measure the dissociation rate constant and the equilibrium constant for binding for L to its operator site in the absence of R. For the chosen solution conditions, we find that both the observed velocity of abortive RNA oligomer synthesis and the KMnO4 reactivities of bases in the open region are functions of [L] and [R], demonstrating that formation of both RPinit and the repressor-operator complex (PL) are reversible processes under these conditions, and requiring the use of a relaxation-to-equilibrium analysis to interpret the kinetics. The agreement between dissociation rate constants of RPinit when challenged with either lac repressor or heparin, and the dependences on [L] and [R] of abortive synthesis velocities at binding equilibrium and of relaxation rate constants for reversible formation of RPinit from PL, all provide evidence for a simple competition mechanism. In this mechanism, and in contrast to recent proposals from other laboratories, lac repressor inhibits formation of RPinit and hence the observed rate of abortive product synthesis by reducing the equilibrium extent of formation of the first closed complex (RPc1), without affecting either the nature of RPinit or steps in formation of RPinit from RPc1.

DNA, Superhelical

Grand canonical Monte Carlo molecular and thermodynamic predictions of ion effects on binding of an oligocation (L8+) to the center of DNA oligomers.

Grand canonical Monte Carlo (GCMC) simulations are reported for aqueous solutions containing excess univalent salt (activities a +/- = 1.76-12.3 mM) and one of the following species: an octacationic rod-like ligand, L8+; a B-DNA oligomer with N phosphate charges (8 < or = N < or = 100); or a complex resulting from the binding of L8+ at the center of an N-mer (24 < or = N < or = 250). Simplified models of these multiply charged species are used in the GCMC simulations to predict the fundamental coulombic contributions to the following experimentally relevant properties: 1) the axial distance over which ligand binding affects local counterion concentrations at the surface of the N-mer; 2) the dependence on N of GCMC preferential interaction coefficients, gamma 32MC identical to delta C3/delta C2l a +/-, T, where C3 and C2 are, respectively, the molar concentrations of salt and the multiply charged species (ligand, N-mer or complex); and 3) the dependence on N of SaKobs identical to d in Kobs/d in a +/- = delta (magnitude of ZJ + 2 gamma 32J), where Kobs is the equilibrium concentration quotient for the binding of L8+ to the center of an N-mer and delta denotes the stoichiometric combination of terms, each of which pertains to a reactant or product J having magnitude of ZJ charges. The participation of electrolyte ions in the ligand binding interaction is quantified by the magnitude of SaKobs, which reflects the net (stoichiometrically weighted) difference in the extent of thermodynamic binding of salt ions to the products and reactants. Results obtained here from GCMC simulations yield a picture of the salient molecular consequences of binding a cationic ligand, as well as thermodynamic predictions whose applicability can be tested experimentally. Formation of the central complex is predicted to cause a dramatic reduction in the surface counterion (e.g., Na+) concentration over a region including but extending well beyond the location of the ligand binding site. For binding a cationic ligand, SaKobs is predicted to be negative, indicating net electrolyte ion release in the binding process. At small enough N, -SaKobs is predicted to decrease strongly toward zero with decreasing N. At intermediate N, -SaKobs appears to exceed its limiting value as N-->infinity.

Cations

Interpretation of preferential interaction coefficients of nonelectrolytes and of electrolyte ions in terms of a two-domain model.

For a three-component system consisting of solvent (1), polymer or polyelectrolyte (2J), and a nonelectrolyte or electrolyte solute (3), a two-domain description is developed to describe thermodynamic effects of interactions between solute components (2J) and (3). Equilibrium dialysis, which for an electrolyte solute produces the Donnan distribution of ions across a semipermeable membrane, provides a fundamental basis for this two-domain description whose applicability is not restricted, however, to systems where dialysis equilibrium is established. Explicit expressions are obtained for the solute-polymer preferential interaction coefficient gamma 3,2J (nonelectrolyte case) and for gamma +,2J and gamma -,2J, which are corresponding coefficients defined for single (univalent) cations and anions, respectively: gamma +,2J = magnitude of ZJ + gamma -,2J = 0.5(magnitude of ZJ + B-,2J + B+,2J) - B1,2Jm3/m1 Here B+,2J, B-,2J, and B1,2J are defined per mole of species J, respectively, as the number of moles of cation, anion, and water included within the local domains that surround isolated molecules of J; ZJ is the charge on J; m3 is the molal concentration of uniunivalent electrolyte, and m1 = 55.5 mol/kg for water. Incorporating this result into a general thermodynamic description(derived by us elsewhere) of the effects of the activity a+ of excess uniunivalent salt on an equilibrium involving two or more charged species J (each of which is dilute in comparison with the salt) yields:SaKobs bS/d a+ A(r+2J r 2j) A(B+2J B-2 2B12Jm3/m1)where KObS is an equilibrium quotient defined in terms of the molar concentrations of the participants, J, and A denotes astoichio metrically weighted combination of terms pertaining to the reactant(s) and product(s). The derivation presented here does not depend on any particular molecular model for salt-polyelectrolyte (or solute-polymer) interactions; it therefore generalizes our earlier (1978) derivation.

Biophysical Phenomena

Analyses of thermodynamic data for concentrated hemoglobin solutions using scaled particle theory: implications for a simple two-state model of water in thermodynamic analyses of crowding in vitro and in vivo.

Quantitative description of the thermodynamic consequences of macromolecular crowding (excluded volume nonideality) is an important component of analyses of the thermodynamics and kinetics of noncovalent interactions of biopolymers in vivo and in concentrated polymer solutions in vitro. By analyzing previously published thermodynamic data, we have investigated extensively the comparative applicability of two forms of scaled particle theory (SPT). In both forms, macromolecules are treated as hard spheres, but MSPT, introduced by Ross and Minton, treats the solvent as a structureless continuum, whereas bulk water molecules are included explicitly as hard spheres in BSPT, an approach developed by Berg. Here we use both MSPT and BSPT to calculate the excluded volume component of the macromolecular activity coefficient of hemoglobin (Hb) at concentrations up to 509 mg/ml by fitting osmotic pressure data for Hb and sedimentation equilibrium data for Hb and sickle-cell Hb (HbS). Both forms of SPT also are used here to analyze the effects of other globular proteins (BSA and Hb) on the solubility of HbS. In applying MSPT and BSPT to analyze macromolecular crowding, the extent of hydration delta Hb (in gH2O/gprotein) is introduced as an adjustable parameter to specify the effective (hard sphere) radius of hydrated Hb. In our nonlinear least-squares fittings based on BSPT, the hard sphere radius of bulk water molecules is either fixed at 1.375 A or floated. Although both forms of SPT yield good fittings (with different values of delta Hb) at Hb concentrations up to 350 mg/ml, only BSPT gives good fittings of all available Hb osmotic pressure data as well as of the sedimentation equilibrium and solubility data. Only BSPT predicts values for delta Hb (approximately 0.5-0.6 g/g) in the range obtained for Hb from hydrodynamic measurements (approximately 0.36-0.78 g/g). These findings indicate the applicability, at least in the context of BSPT, of a simple two-state classification of water (bulk water and water of macromolecular hydration) as a basis for interpreting excluded volume nonideality in concentrated solutions of globular proteins.

Biophysical Phenomena

Importance of coulombic end effects on cation accumulation near oligoelectrolyte B-DNA: a demonstration using 23Na NMR.

The local cation concentration at the surface of oligomeric or polymeric B-DNA is expected, on the basis of MC simulations (Olmsted, M. C., C. F. Anderson, and M. T. Record, Jr. 1989. Proc. Natl. Acad. Sci. USA. 86:7766-7770), to decrease sharply as either end of the molecule is approached. In this paper we report 23Na NMR measurements indicating the importance of this "coulombic" end effect on the average extent of association of Na+ with oligomeric duplex DNA. In solutions containing either 20-bp synthetic DNA or 160-bp mononucleosomal calf thymus DNA at phosphate monomer concentrations [P] of 4-10 mM, measurements were made over the range of ratios 1 < or = [Na]/[LP] < or = 20, corresponding to Na+ concentrations of 4-200 nM. The longitudinal 23Na NMR relaxation rates measured in these NaDNA solutions, Robs, are interpreted as population-weighted averages of contributions from "bound" (RB) and "free" (RF) 23Na relaxation rates. The observed enhancements of Robs indicate that RB significantly exceeds RF, which is approximately equal to the 23Na relaxation rate in an aqueous solution containing only NaCl. Under salt-fre-tconditions ([Na]/[P] = 1), where the enhancement in Robs is maximal, we find that Robs--RF in the solution containing 160-bp DNA is approximately 1.8 times that observed for the 20-bp DNA. For the 160-bp oligomer (which theoretical calculations predict to be effectively polyion-like), we find that a plot of Robs v. [P]/[Na] is linear, as observed previously for sonicated (approximately 700 bp) DNA samples. For the 20-bp oligonucleotide this plot exhibits a marked departure from linearity that can be fitted to a quadratic function of [P]/[Na]. Monte Carlo simulations based on a simplified model are capable of reproducing the qualitative trends in the 23Na NMR measurements analyzed here. In particular, the dependences of Robs--RF on DNA charge magnitude of Z(320 vs. 38 phosphates) and (for the 20-bp oligomer) on [Na]/[P] are well correlated with the calculated average surface concentration of Na+. Thus, effects of sodium concentration on RB appear to be of secondary importance. We conclude that 23Na NMR relaxation measurements are a sensitive probe of the effects of oligomer charge on the extent of ion accumulation near B-DNA oligonucleotides, as a function of [Na] and [P].

Animals

Salt-nucleic acid interactions.

Coulombic interactions of salt ions with polymeric and oligomeric nucleic acids in solution have large and distinctive effects on ion distributions, on thermodynamic coefficients, and hence on equilibrium processes involving nucleic acids, such as their conformational transitions and binding interactions. In experimental or theoretical studies where an oligonucleotide is taken to represent the corresponding polynucleotide, the impact of coulombic end effects on molecular and thermodynamic properties must be taken into account. Observable consequences of coulombic interactions in nucleic acid solutions have been calculated by using models with varying degrees of detail and methods formulated at varying levels of rigor. From comparisons of experimental results with predictions of the prevalent theoretical approaches, this review concludes that the more rigorous methods have proved capable of accounting for thermodynamic (and some molecular) consequences of coulombic interactions with a minimal number of preaveraged parameters that represent the most important structural features of the nucleic acid solution.

Electrolytes

Preparative-scale purification of DNA restriction fragments by continuous-flow gel electrophoresis.

A method is described for large-scale (10-100 micrograms) purification of individual DNA fragment lengths from a mixture of fragment lengths using a continuous-flow, toroidal gel electrophoresis system that is commercially available. Preparative-scale separations of fragments up to approximately 1000 bp differing in length by as little as 100 bp are obtained. Typical recoveries of purified DNA fragments range from 25% to 40% of starting material.

DNA

Coupling of local folding to site-specific binding of proteins to DNA.

Thermodynamic studies have demonstrated the central importance of a large negative heat capacity change (delta C degree assoc) in site-specific protein-DNA recognition. Dissection of the large negative delta C degree assoc and the entropy change of protein-ligand and protein-DNA complexation provide a thermodynamic signature identifying processes in which local folding is coupled to binding. Estimates of the number of residues that fold on binding obtained from this analysis agree with structural data. Structural comparisons indicate that these local folding transitions create key parts of the protein-DNA interface. The energetic implications of this "induced fit" model for DNA site recognition are considered.

Base Sequence

Factor independent activation of rrnB P1. An "extended" promoter with an upstream element that dramatically increases promoter strength.

The extraordinary strength of the Escherichia coli rRNA promoter rrnB P1 derives primarily from sequences upstream of the core (-10, -35) region. We find that sequences between -40 and -60 increase the activity of this promoter at least 30-fold in vitro and in vivo. This region, which we refer to as the upstream (UP) element, is located between the -35 consensus hexamer and the previously characterized binding sites for the rRNA transcription factor Fis. The effect of the UP element is independent of Fis in vivo, and independent of any other proteins besides RNA polymerase (RNAP) in vitro. The UP element increases the overall second-order rate constant for association of RNAP with the promoter (ka) and probably the apparent overall first-order isomerization constant (ki). Together with the previously reported protection of the UP element region by RNAP in footprinting experiments, these results indicate that rrnB P1 has an "extended" promoter structure, consisting of the UP element and the core promoter region. We find that the UP element is a separable promoter module that can function to increase the activity of the lac core promoter in an rrnB P1-lac hybrid promoter construct. A functional UP element is not absolutely essential for stimulation of rrnB P1 by the Fis protein.

Base Sequence