Kinetics in interactions between antibodies and haptens.

Association and dissociation kinetics of antibody-hapten interactions of high affinity and specificity have been determined by newly developed techniques using dextran-coated charcoal for rapid separation of free and antibody-bound hapten. Interactions of 12 combinations of four antibody populations (rabbit digoxin-specific antibody, sheep digoxin-specific antibody, rabbit ouabain-specific antibody, and rabbit digitoxin-specific antibody) with three haptens ([3-H]digoxin, [3-H]ouabain, and [3-H]digitoxin) have been studied in terms of both association and dissociation kinetics, and compared in selected instances with association constants determined under equilibrium conditions. Association rate constants determined under both second-order and pseudo-first-order conditions were found to be similar for all antibody-hapten pairs studied (range 0.87-1.7 times 10-7 M-minus 1 sec- minus 1), and were comparable to values previously estimated for antibodies to dye haptens of markedly lower affinity. In contrast, dissociation rate constants varied markedly from 1.9 times 10- minus 4 to 1.7 times 10- minus 2 sec- minus 1. Ratios of association to dissociation rate constants measured by these methods were in satisfactory agreement with average intrinsic association constants measured under equilibrium conditions. These studies support the concept that the major kinetic variable governing antibody-hapten interactions is the rate of dissociation of the complex, and that the strength of antibody-hapten association is determined principally by the activation energy for dissociation.     

The equilibrium unfolding of Azotobacter vinelandii apoflavodoxin II occurs via a relatively stable folding intermediate.

A flavodoxin from Azotobacter vinelandii is chosen as a model system to study the folding of alpha/beta doubly wound proteins. The guanidinium hydrochloride induced unfolding of apoflavodoxin is demonstrated to be reversible. Apoflavodoxin thus can fold in the absence of the FMN cofactor. The unfolding curves obtained for wild-type, C69A and C69S apoflavodoxin as monitored by circular dichroism and fluorescence spectroscopy do not coincide. Apoflavodoxin unfolding occurs therefore not via a simple two-state mechanism. The experimental data can be described by a three-state mechanism of apoflavodoxin equilibrium unfolding in which a relatively stable intermediate is involved. The intermediate species lacks the characteristic tertiary structure of native apoflavodoxin as deduced from fluorescence spectroscopy, but has significant secondary structure as inferred from circular dichroism spectroscopy. Both spectroscopic techniques show that thermally-induced unfolding of apoflavodoxin also proceeds through formation of a similar molten globule-like species. Thermal unfolding of apoflavodoxin is accompanied by anomalous circular dichroism characteristics: the negative ellipticity at 222 nM increases in the transition zone of unfolding. This effect is most likely attributable to changes in tertiary interactions of aromatic side chains upon protein unfolding. From the presented results and hydrogen/deuterium exchange data, a model for the equilibrium unfolding of apoflavodoxin is presented.     

Measuring surface dynamics of biomolecules by total internal reflection fluorescence with photobleaching recovery or correlation spectroscopy.

The theoretical basis of a new technique for measuring equilibrium adsorption/desorption kinetics and surface diffusion of fluorescent-labeled solute molecules at solid surfaces has been developed. The technique combines total internal reflection fluorescence (TIR) with either fluorescence photobleaching recovery (FPR) or fluorescence correlation spectroscopy (FCS). A laser beam totally internally reflects at a solid/liquid interface; the shallow evanescent field in the liquid excites the fluorescence of surface adsorbed molecules. In TIR/FPR, adsorbed molecules are bleaching by a flash of the focused laser beam; subsequent fluorescence recovery is monitored as bleached molecules exchange with unbleached ones from the solution or surrounding nonilluminated regions of the surface. In TIR/FCS, spontaneous fluorescence fluctuations due to individual molecules entering and leaving a well-defined portion of the evanescent field are autocorrelated. Under appropriate experimental conditions, the rate constants and surface diffusion coefficient can be readily obtained from the TIR/FPR and TIR/FCS curves. In general, the shape of the theoretical TIR/FPR and TIR/FCS curves depends in a complex manner upon the bulk and surface diffusion coefficients, the size of the iluminated or observed region, and the adsorption/desorption/kinetic rate constants. The theory can be applied both to specific binding between immobilized receptors and soluble ligands, and to nonspecific adsorption processes. A discussion of experimental considerations and the application of this technique to the adsorption of serum proteins on quartz may be found in the accompanying paper (Burghardt and Axelrod. 1981. Biophys. J. 33:455).     

Equilibrium of conformers in solution: spin-labelled angiotensin

The number of structural parameters were determined for spin-labelled angiotensin in aqueous solution with the use of fluorescence spectroscopy and 1H NMR relaxation induced by the spin label. At the same time all measured parameters were estimated theoretically by means of energy calculations and Monte-Carlo techniques. The matching procedure for experimental and computational data allows one to suggest a dynamic equilibrium between conformers of the molecule in aqueous solution and to estimate the values of their weights.     

Fluorescence polarization study of DNA--proflavine complexes

The binding of proflavine to DNA has been studied by measuring the polarization and intensity of emission of DNA–dye complexes. Such measurements also permit the determination of the fluorescence of the bound dye as a function of the degree of binding. Techniques of emission spectroscopy permit the study of complexing at high phosphate to dye ratios, and we have examined complexes formed at up to 12,300:1 phosphates to dye. At high phosphate to dye ratios, we find that equilibrium plots of the binding data show only one type of binding. Reports in the literature of multiple binding constants are shown to be due to the incorrect assumption that the fluorescence of the bound dye is independent of the amount bound. The emission properties can be qualitatively accounted for by assuming that nearest-neighbor interaction between bound dyes quenches the fluorescence. We report that, within experimental error, the binding constant is insensitive to the base content of the DNA. The DNA-dye complexes show a temperature dependent depolarization, the cause of which is, as yet, unknown. Heat denaturation of the DNA–dye complex may be followed on a Perrin plot.     

Structural predictions of the binding site architecture for monoclonal antibody NC6.8 using computer-aided molecular modeling, ligand binding, and spectroscopy.

Monoclonal antibody NC6.8 binds the superpotent sweetener ligand N-(p-cyanophenyl)-N'-(diphenylmethyl) guanidineacetic acid with high affinity (Kd = 53 nM). Using computer-aided molecular modeling and several experimental techniques, such as competitive ligand binding, absorbance spectroscopy, and fluorescence spectroscopy, we have predicted the structure of the variable domain fragment (Fv) and identified the key residues in the combining site of the antibody. We have identified nine specific amino acids as being involved in ligand recognition and complexation. Most notable are H:33W, which is responsible for ligand-induced tryptophan fluorescence quenching, H:56R, which forms a salt bridge with the carboxylate moiety of the ligand, and L:34H, which, deep in the binding site, interacts with the cyanophenyl portion of the ligand. Two residues located deep in the putative binding pocket, H:35E and H:50E, provide the negatively charged potential for interaction with the protonated aryl nitrogen and the positive guanidinium group. These modeling predictions were made before the solution of high-resolution structures of the native Fab (2.6 A) and the Fab-ligand complex (2.2 A). Comparisons between the theoretical model and experimental native and liganded Fab structures are made.     

A study of GDP binding to purified thermogenin protein from brown adipose tissue.

1. The binding of GDP to purified thermogenin protein was studied by using fluorescence spectroscopy and equilibrium dialysis. 2. GDP binding to thermogenin diminished fluorescence emission in a concentration-dependent manner that exhibited saturation. 3. Kd values for binding of nucleoside di- and tri-phosphates were lower than those for nucleoside monophosphates. 4. The GDP-induced fluorescence quenching was decreased by increasing pH, but the apparent Kd was unaltered by pH changes. 5. Equilibrium dialysis showed a Kd change from 3 to 6 microM when the pH was increased from 6.6 to 8.5. 6. The apparent pK of the fluorescence changes induced by pH (8.3) was identical with the apparent pK of the GDP-binding response. 7. The data are consistent with the existence of protonated and non-protonated forms of thermogenin protein that both bind GDP.     

Combining EPR with Fluorescence Spectroscopy to Monitor Conformational Changes at the Myosin Nucleotide Pocket

We used spin-labeled nucleotide analogs and fluorescence spectroscopy to monitor conformational changes at the nucleotide-binding site of wild-type Dictyostelium discoideum (WT) myosin and a construct containing a single tryptophan at position F239 near the switch 1 loop. Electron paramagnetic resonance (EPR) spectroscopy and tryptophan fluorescence have been used previously to investigate changes at the myosin nucleotide site. A limitation of fluorescence spectroscopy is that it must be done on mutated myosins containing only a single tryptophan. A limitation of EPR spectroscopy is that one infers protein conformational changes from alterations in the mobility of an attached probe. These limitations have led to controversies regarding conclusions reached by the two approaches. For the first time, the data presented here allow direct correlations to be made between the results from the two spectroscopic approaches on the same proteins and extend our previous EPR studies to a nonmuscle myosin. EPR probe mobility indicates that the conformation of the nucleotide pocket of the WT⋅SLADP (spin-labeled ADP) complex is similar to that of skeletal myosin. The pocket is closed in the absence of actin for both diphosphate and triphosphate nucleotide states. In the actin⋅myosin⋅diphosphate state, the pocket is in equilibrium between closed and open conformations, with the open conformation slightly more favorable than that seen for fast skeletal actomyosin. The EPR spectra for the mutant show similar conformations to skeletal myosin, with one exception: in the absence of actin, the nucleotide pocket of the mutant displays an open component that was approximately 4-5 kJ/mol more favorable than in skeletal or WT myosin. These observations resolve the controversies between the two techniques. The data from both techniques confirm that binding of myosin to actin alters the conformation of the myosin nucleotide pocket with similar but not identical energetics in both muscle and nonmuscle myosins.     

Folding of dihydrofolate reductase from Escherichia coli

The urea-induced equilibrium unfolding transition of dihydrofolate reductase from Escherichia coli was monitored by UV difference, circular dichroism (CD), and fluorescence spectroscopy. Each of these data sets were well described by a two-state unfolding model involving only native and unfolded forms. The free energy of folding in the absence of urea at pH 7.8, 15 degrees C is 6.13 +/- 0.36 kcal mol-1 by difference UV, 5.32 +/- 0.67 kcal mol-1 by CD, and 5.42 +/- 1.04 kcal mol-1 by fluorescence spectroscopy. The midpoints for the difference UV, CD, and fluorescence transitions are 3.12, 3.08, and 3.18 M urea, respectively. The near-coincidence of the unfolding transitions monitored by these three techniques also supports the assignment of a two-state model for the equilibrium results. Kinetic studies of the unfolding and refolding reactions show that the process is complex and therefore that additional species must be present. Unfolding jumps in the absence of potassium chloride revealed two slow phases which account for all of the amplitude predicted by equilibrium experiments. Unfolding in the presence of 400 mM KCl results in the selective loss of the slower phase, implying that there are two native forms present in equilibrium prior to unfolding. Five reactions were observed in refolding: two slow phases designated tau 1 and tau 2 that correspond to the slow phases in unfolding and three faster reactions designated tau 3, tau 4, and tau 5 that were followed by stopped-flow techniques. The kinetics of the recovery of the native form was monitored by following the binding of methotrexate, a tight-binding inhibitor of dihydrofolate reductase, at 380 nm.(ABSTRACT TRUNCATED AT 250 WORDS)     

Contributions by ionic and steric features of ligands to their binding with phosphorylcholine-specific immunoglobulin IgA H-8 as determined by fluorescence spectroscopy.

The murine myeloma IgA H-8 Fab' fragment which exhibits a binding specificity for phosphorylcholine was assayed for its ability to bind with a number of charged ligands. Monitoring of the ligand-induced changes of protein fluorescence provided a fast and accurate method of determining the equilibrium binding constants. The binding data along with fluorescence spectral properties of the protein permitted an assessment of the relative importance of some binding parameters as well as an evaluation of certain ionic and steric contributions made by ligands exhibiting significant binding affinity for the antibody fragment. Among the conclusions reached is that the dielectric of the binding site microenvironment is important in determining the strength of binding and that hydrophobic groups surrounding a quaternary cationic ligand are important in creating an appropriate binding site of low dielectric value.