NMR relaxation processes of 31P in macromolecules

³¹P-Nmr relaxation parameters (spin-lattice relaxation time, linewidth, and nuclear Overhauser effect) were obtained at three different frequencies for poly(U) and a well-defined (145 ± 3 base-pair) fragment of DNA in solution. Data sets for the two samples were analyzed by theories which included relaxation by the mechanisms of ³¹P chemical shift anisotropy as well as by ¹H-³¹P dipole–dipole interaction. Neither data set could be satisfactorily described by a single correlation time. A model of a rigid rotor most nearly fits the data for the DNA molecule. Parameters obtained from the least-square fit indicate (1) that the DNA undergoes anisotropic reorientation with a correlation time τ₀ = 6.5 × 10^?7 sec for the end-to-end motion, (2) the ratio of diffusion constants D_∥/D_⊥ is 91, and (3) that the linewidth is due to chemical shift dispersion to the extent of 0.5 ppm. Some deviations of the calculated from the observed values suggested that significant torsional and bending motions may also take place for this DNA. Another model which contains isotropic motion but with a broad distribution of correlation times was required to fit the data for poly(U). A log ? χ² distribution function of correlation times [Scheafer, J. (1973) Macromolecules 6 , 881–888] described well the motion of poly(U) with the average correlation time τ = 3.3 × 10^?9 sec and a distribution parameter p = 14.     

Structural investigation of poly d(BrU-A) by ultraviolet resonance raman spectroscopy

The resonance Raman spectra of a DNA containing bromodeoxy-uridine (BrdUrd), the poly d(BrU-A), are reported, using U.V. laser as a source of excitation. The conformational change from the ordered, base paired form of poly d(BrU-A) (at 25°C) to the melted form at high temperature (63°C) is reflected in a pronounced hyperchromism of Raman bands at 1627 cm^?1, 1352 cm^?1 and 1230 cm^?1. Particularly the band at 1627 cm^?1 assigned to the vibrations of C4 carbonyl which is hydrogen bonded to adenine increases strongly its intensity upon melting. This represents a new approach for a detection of base unpairing and of modifications in geometry of selective molecules (BrdUrd) in a DNA chain in dilute solutions (10^?4 M).     

Fluorescence of proflavine--DNA complexes: heterogeneity of binding sites

Measurements of the relative quantum yield of fluorescence of proflavine bound to DNA as a function of the number of bound dyes per nucleotide and the ionic strength allow the determination of the binding constants and respective number of the two types of sites previously postulated. It is demonstrated that 2–3% of the base pairs form sites where the dye is strongly bound and fluoresces normally while in the other set of sites the binding constant is 3–4 times weaker and the fluorescence completely quenched. Comparison with complexes of Pro with double stranded polynucleotides poly (A + U), poly (I + C), poly(G + C), confirm that the strong binding sites correspond to A-T-rich regions of the DNA while the quenched sites seem to require the presence of a neighboring guanine. The role of charge transfer in quenching of fluorescence and mutagnic action is considered. An original method for the determination of free dye and bound dye, based upon the use of an external quencher is described in the Appendix.     

Equilibrium and kinetic studies on the binding of des-N-tetramethyltriostin A to DNA

The interaction between TANDEM (a des-methyl analogue of triostin A) and poly(dA-dT) results in extension of the helix by 6.8 Å for each ligand molecule bound, exactly as predicted for a bis-intercalation reaction. Cooperativity is evident in Scatchard plots for the interaction at ionic strengths of 0.2 and 1.0, where the binding constant is diminished compared to that which pertains at low salt concentration. Binding to a natural DNA (calf thymus), already considerably weaker than binding to poly(dA-dT), is also sensitive to increased ionic strength. With a self-complementary octanucleotide d(G-G-T-A-T-A-C-C) the binding curve indicates the presence of a single des-N-tetramethyltriostin A binding site per helical fragment with a non-cooperative association constant about 6·10⁶ M^?1. Detergent-induced dissociation of des-N-tetramethyltriostin A-poly(dA-dT) complexes results in a simple exponential decay at all levels of binding, but the time constant of decay is dependent upon the initial binding ratio. This behaviour cannot directly explain the cooperativity of equilibrium binding isotherms but suggests the occurrence of relatively long-lived perturbations of the helical structure by binding of the ligand. [Ala³, Ala⁷]des-N-tetramethyltriostin A, which has a more flexible octapeptide ring lacking the disulphide cross-bridge, dissociates from poly(dA-dT) much faster than des-N-tetramethyltriostin A. Dissociation of des-N-tetramethyltriostin A from calf thymus DNA is more rapid than dissociation of triostin A or other quinoxaline antibiotics, which may account for its low antimicrobial activity.     

Influence of poly A-poly U on early events in the immune response in vitro

Adjuvant action of artificial homopolyribonucleotides and nucleic acid digests was studied in mouse spleen-cell cultures, stimulated with sheep red cells by the technique of Mishell and Dutton. Assays of antibody-forming cells were performed according to the Jerne and Nordin technique. Doublestranded poly A-poly U, and RNA digests had adjuvant activity over a wide dose range (0.01–100 μg/ml). DNA digests, single stranded polynucleotides (poly A, poly U, poly C) and mixtures of ribonucleosides and ribonucleotides had little or no enhancing effect at comparable doses. From our study of the kinetics of increase of plaque-forming cells in cultures treated with poly A-poly U, in conjunction with in vivo studies of others, we concluded that adjuvant action, during induction, indirectly increased the number of bone marrow-derived cells that responded to antigenic stimulation by increasing the effectiveness of the thymus-derived cells in the culture.     

Enzyme-Free Detection of Mutations in Cancer DNA Using Synthetic Oligonucleotide Probes and Fluorescence Microscopy

Background

Rapid reliable diagnostics of DNA mutations are highly desirable in research and clinical assays. Current development in this field goes simultaneously in two directions: 1) high-throughput methods, and 2) portable assays. Non-enzymatic approaches are attractive for both types of methods since they would allow rapid and relatively inexpensive detection of nucleic acids. Modern fluorescence microscopy is having a huge impact on detection of biomolecules at previously unachievable resolution. However, no straightforward methods to detect DNA in a non-enzymatic way using fluorescence microscopy and nucleic acid analogues have been proposed so far.

Methods and Results

Here we report a novel enzyme-free approach to efficiently detect cancer mutations. This assay includes gene-specific target enrichment followed by annealing to oligonucleotides containing locked nucleic acids (LNAs) and finally, detection by fluorescence microscopy. The LNA containing probes display high binding affinity and specificity to DNA containing mutations, which allows for the detection of mutation abundance with an intercalating EvaGreen dye. We used a second probe, which increases the overall number of base pairs in order to produce a higher fluorescence signal by incorporating more dye molecules. Indeed we show here that using EvaGreen dye and LNA probes, genomic DNA containing BRAF V600E mutation could be detected by fluorescence microscopy at low femtomolar concentrations. Notably, this was at least 1000-fold above the potential detection limit.

Conclusion

Overall, the novel assay we describe could become a new approach to rapid, reliable and enzyme-free diagnostics of cancer or other associated DNA targets. Importantly, stoichiometry of wild type and mutant targets is conserved in our assay, which allows for an accurate estimation of mutant abundance when the detection limit requirement is met. Using fluorescence microscopy, this approach presents the opportunity to detect DNA at single-molecule resolution and directly in the biological sample of choice.     

Characterization of the binding of YO to [poly(dA-dT)]2 and [poly(dG-dC)]2, and of the fluorescent properties of YO and YOYO complexed with the polynucleotides and double-stranded DNA

The interaction between the fluorescent dye YO (oxazole yellow) and the alternating polynucleotides [poly(dA-dT)]₂[the duplex of alternating poly(dA-dT)]and [poly(dG-dC)]₂[the duplex of alternating poly(dG-dC)] has been studied with optical spectroscopic techniques including absorbance, flow linear dichroism, CD, and fluorescence measurements. The principal features of the spectra are very similar for the two polynucleotide solutions, showing that YO binds quite similarly to AT and GC base pairs. From a strongly negative reduced linear dichroism (LD^r) in the dye absorption band, an induced negative CD, and transfer of energy from the bases to bound YO, we conclude that at low mixing ratios YO is intercalated in both [poly(dA-dT)]₂ and [poly(dG-dC)]₂. At higher mixing ratios an external binding mode starts to contribute, evidenced from the appearance of an exciton CD. The conclusion that YO binds in a similar way to AT and GC base pairs should be valid also for the dimer YOYO since its YO units have been found to bind to double-stranded (dsDNA) in the same way as the YO monomer. The fluorescence properties of YO and YOYO complexed with DNA or the polynucleotides have been characterized by studying the dependence of fluorescence intensity on temperature, mixing ratio, and ionic strength. The fluorescence intensity and fluorescence lifetime of YO-DNA decrease strongly with increasing mixing ratio, whereas the fluorescence intensity of YOYO-DNA shows a weaker dependence, indicating that the quantum yield depends on the distance between the YO chromophores on the DNA chain. Further, the fluorescence intensity of YO depends on the base sequence; the quantum yield and fluorescence lifetime for YO complexed with [poly(dG-dC)]₂ are about twice as large as for YO complexed with [poly(dA-dT)]₂. Measurements of excitation spectra at different mixing ratios and different emission wavelengths indicate that the fluorescence of the externally bound chromophores is negligible compared to the intercalated ones. © 1995 John Wiley & Sons, Inc.     

Fluorescence decay studies of the DNA-3,6-diaminoacridine complexes

The interaction of several 3,6-diaminoacridines with DNAs of various base composition has been studied by steady-state and transient fluorescence measurements. The acridine dyes employed are of the following two classes: class I - proflavine, acriflavine and 10-benzyl proflavine; class II - acridine yellow, 10-methyl acridine yellow and benzoflavine. It is found that the fluorescence decay kinetics follows a single-exponential decay law for free dye and the poly[d(A-T)]-dye complex, while that of the dye bound to DNA obeys a two-exponential decay law. The long lifetime (tau 1) for each complex is almost the same as the lifetime for the poly[d(A-T)]-dye complex, and the amplitude alpha 1 decreases with increasing GC content of DNA. The fluorescence quantum yields (phi F) of dye upon binding to DNA decrease with increasing GC content; the phi F values for class I are nearly zero when bound to poly(dG) X poly(dC), but those for class II are not zero. This is in harmony with the finding that GMP almost completely quenches the fluorescence for class I, whereas a weak fluorescence arises from the GMP-dye complex for class II. The fluorescence spectra of the DNA-dye complexes gradually shift toward longer wavelengths with increasing GC content. In this connection, the fluorescence decay parameters show a dependence on the emission wavelength; alpha 1 decreases with an increase in the emission wavelength. In view of these results, it is proposed that the decay behavior of the DNA-dye complexes has its origin in the heterogeneity of the emitting sites; the long lifetime tau 1 results from the dye bound to AT-AT sites, while the short lifetime tau 2 is attributable to the dye bound in the vicinity of GC pairs. Since GC pairs almost completely quench the fluorescence for class I, partly intercalated or externally bound dye molecules may play an important role in the component tau 2.     

Histone-induced conformational changes in DNA as probed by quasi-elastic light scattering.

Quasi-elastic light scattering as measured by intensity fluctuation (self-beat) spectroscopy in the time domain can be profitably used to follow both the translational diffusion D and the dominant internal flexing mode τ_int of DNA and its complexes with various histones in aqueous salt solutions. Without histones, DNA is found to have D = 1.6 × 10^?8 cm²/sec and τ_int ? 5 × 10^?4 sec in 0.8 M NaCl, 2 M urea at 20°C. Total histone as well as fraction F2A induce supercoiling (D = 2.6 × 10^?8 cm²/sec, τ_int ? 2.8 × 10^?4 sec) whereas fraction F1 induces uncoiling (D = 1.0 × 10^?8 cm²/sec, τ_int ? 9.4 × 10^?4 sec). Upon increasing the salt concentration to 1.5 M the DNA–histone complex dissociates (D = 1.8 × 10^?8 cm²/sec). Upon decreasing the salt concentration to far below 0.8 M, the DNA–histone complex eventually precipitates as a chromatin gel.     

Mechanisms of chromosome banding

A series of biochemical investigations were undertaken to determine the mechanism of Q-banding. The results were as follows: 1. In agreement with previous studies, highly AT-rich DNA, such as poly(dA)-poly(dT), markedly enhanced quinacrine fluorescence while GC containing DNA quenched fluorescence. These effects persisted at DNA concentrations comparable to those in the metaphase chromosome. 2. Studies of quinacrine-DNA complexes in regard to the hypochromism of quinacrine, DNA Tm, DNA viscosity, and equilibrium dialysis, indicated the quinacrine was bound by intercalation with relatively little side binding. 3. Single or double stranded nucleotide polymers, in the form of complete or partial helices, were 1000-fold more effective in quenching than solutions of single nucleotides, suggesting that base stacking is required for quenching. 4. Studies of polymers in the A conformation, such as transfer RNA and DNA-RNA hybrids, indicated that marked base tilting does not affect the ability of nucleic acids to cause quenching or enhancement of quinacrine fluorescence. 5. Salts inhibit the binding of quinacrine to DNA. 6. Spermine, polylysine and polyarginine, which bind in the small groove of DNA, inhibited quinacrine binding and quenching, while histones, which probably bind in the large groove, had little effect. This correlated with the observation that removal of histones with acid has no effect on Q-banding. 7. Mouse liver chromatin was separated into five fractions. At concentrations of quinacrine from 2×10^?6 to 2×10^?5 M all fractions inhibited to varying degrees the ability of the chromatin DNA to bind quinacrine and quench quinacrine fluorescence. At saturating levels of quinacrine two fractions, the 400 g pellet (rich in heterochromatin) and a dispersed euchromatin supernatant fraction, showed a decreased number of binding sites for quinacrine. These two fractions were also the richest in non-histone proteins. 8. DNA isolated from the different fractions all showed identical quenching of quinacrine fluorescence. 9. Mouse GC-rich, mid-band, AT-rich, and satellite DNA, isolated by CsCl and Cs₂SO₄-Ag⁺ centrifugation all showed identical quenching of quinacrine fluorescence, indicating that within a given organism, except for very AT or GC-rich satellites, the variation in base composition is not adequate to explain Q-banding. — We interpret these results to indicate that: (a) quinacrine binds to chromatin by intercalation of the three planar rings with the large group at position 9 lying in the small groove of DNA, (b) most pale staining regions are due to a decrease binding of quinacrine, and (c) this inhibition of binding is predominately due to non-histone proteins.     

Spectroscopic and microcalorimetric studies on the molecular binding of food colorant acid red 27 with deoxyribonucleic acid

Interaction of the food colorant acid red 27 with double stranded DNA was investigated using spectroscopic and calorimetric methods. Absorbance and fluorescence studies suggested an intimate binding interaction between the dye and DNA. The quantum efficiency value testified an effective energy transfer from the DNA base pairs to the dye molecules. Minor groove displacement assay with Hoechst 33258 revealed that the binding occurs in the minor groove of DNA. Circular dichroism studies revealed that acid red 27 induces moderate conformational perturbations in DNA. Results of calorimetric studies suggested that the complexation process was driven largely by positive entropic contribution with a smaller favorable enthalpy contribution. The equilibrium constant of the binding was calculated to be (3.04 ± 0.09) × 10⁴ M^?1 at 298.15 K. Negative heat capacity value along with the enthalpy–entropy compensation phenomenon established the involvement of dominant hydrophobic forces in the binding process. Differential scanning calorimetry studies presented evidence for an increased thermal stability of DNA on binding of acid red 27. Copyright © 2016 John Wiley & Sons, Ltd.     

Study of the hydratation of the double-helical poly A-poly U complex by IR-spectroscopy and piezogravimetry methods

IR-spectra of a double-helical poly A-poly U complex and coiled poly U were studied at various r.h. in a 900-3800 cm-1 region. By the method of piezomicrobalance hydration isotherms for these polynucleotides were obtained. It is concluded that, as in the DNA case, simultaneous hydration of nucleic bases the backbone of polynucleotides occurs at lower r.h., and that the poly A-poly U hydration level is higher than poly A and poly U ones separately. Drastic changes in spectral parameters of poly A poly U uracil and adenine in-ring and out-of-ring absorption bands observed in 44-76% r.h. region were interpreted as a transition to helical conformation of the complex. Calculation of resonance frequencies for these normal vibrations in the dipole-dipole approximation agrees with the experimental data.     

Condensed states of nucleic acids. II. Effects of molecular size, base composition, and presence of intercalating agents on the psi transition of DNA.

Circular dichroism spectroscopy has been used to investigate the influence of DNA molecular size, base composition, and the presence of intercalating agents upon the Ψ transition of DNA brought about by high concentrations of poly(ethylene oxide) and salt (Lerman (1971) Proc. Natl. Acad. Sci. (U.S.) 68 , 1886–1890). A molecular weight of 0.15–3.0 × 10⁶ daltons yields maximum formation of Ψ-DNA. Both the amplitude of the large negative CD band at 265 nm—a chief characteristic of the Ψ state—and the thermal stability of Ψ-DNA increase linearly with increasing mole fraction of guanine plus cytosine in the DNA sample. Either ethidium or proflavine, at concentrations where approximately one dye is bound per 5–10 nucleotide residues, can prevent the transition completely. Striking similarities between the Ψ-DNA produced by poly(ethylene oxide) + salt and the complexes formed between DNA and lysine-rich histone f1 suggest the presence of similar nucleic acid–nucleic acid interactions in both types of condensed phase.     

Cooperative nonenzymic base recognition. Kinetics of the binding of a base monomer to a complementary polynucleotide template

The kinetics of double-helix formation by poly U and the complementary monomer N-6,9-dimethyladenine (m⁶m⁹A) has been measured using a new fast temperature-jump apparatus. The cooperative binding kinetics are complicated by the extensive self-association of the monomers, but a satisfactory analysis using average relaxation times was possible in terms of three different models. Application of a model which considers only monomer binding yields the upper limit for the binding rate constant of an m⁶m⁹A monomer next to an already bound monomer on a poly U strand: (2 ± 0.4) × 10⁸ M^?1sec^?1. A lower limit is found by using a model which allows for binding of all m⁶m⁹A stacks to poly U with equal rate constants: (3 ± 0.3) × 10⁷ M^?1sec^?1. A third model with “weighted” rate constants consistent with the data: (7.5 ± 1.0) × 10⁷ M^?1sec^?1. The rate of cooperative binding of m⁶m⁹A to the trimer UpUpU has also been measured. The rate constants obtained with the trimer agree with those obtained with the polymer for each of the three models within experimental error.     

Conformational dependence of the Raman scattering intensities from polynucleotides. 3. Order-disorder changes in helical structures

Raman spectra are presented on ordered and presumably helical structures of DNA and RNA as well as the poly A·poly U helical complex, polydAT, and the helical aggregates of 5′-GMP and 3′-GMP. The changes in the frequency and the intensity of the Raman bands as these structures undergo order-disorder transitions have been measured. In general the changes we have found can be placed into three categories: (1) A reduction in the intensities of certain ring vibrations of the polynucleotide bases is observed when stacking or ordering occurs (Raman hypochromism). Since the ring vibrational frequencies are different for each type of base, we have been able to obtain some estimate of average amount of order of each type of base in partially ordered helical systems. (2) A very large increase in the intensity of a sharp, strongly polarized band at about 815 cm^?1 is observed when polyriboA and polyriboU are formed into a helical complex. Although this band is not present in the separated chains at high temperature, a broad diffuse band at about 800 cm^?1 is present. The 815 cm^?1 band undoubtedly arises from the vibrations of the phosphate-sugar portions of the molecule and provides a sensitive handle to the back-bone conformation of the polymer. This band also appears upon ordering of RNA, formation of the helical aggregate of 5′-riboGMP, and to some extent in the selfstacking of the polyribonucleotides polyA, polyU in the presence of Mg⁺⁺, PolyC, and polyG. No such intense, polarized band is found, however, in ordered DNA, polydAT, or the 3′-riboGMP aggregate, although there is a conformationally independent band at about 795 cm^?1 in DNA and polydAT. (3) Numerous frequency changes occur during Conformational changes. In particular the 1600–1700 cm^?1 region in D₂O shows significant conformationally dependent changes in the C?O stretching region analogous to the changes in this region which have been observed in these substances in the infrared. Thus, Raman scattering appears to provide a technique for simultaneously observing the effects of base stacking, backbone conformation and carbonyl hydrogen bonding in nucleic acids in moderately dilute (10–25 mg/ml) aqueous solutions.     

The binding of Mg++ ions to polyadenylate, polyuridylate, and their complexes

The binding of Mg ⁺⁺ to polyadenylate (poly A), Polyuridylate(poly U), and their complexes, poly (A + U) and poly (A + 2U), was studied by means of a technique in which the dye eriochrome black T is used to measure the concentration of free Mg^?. The apparent binding constant K_X = [MgN]/[Mg⁺⁺][N], N = site for Mg⁺⁺ binding (the phosphate group of the nucleotide), was found to decrease rapidly as the extent of binding increased and, at low extents of binding, as the concentration of Na^? increased in poly A, poly (A + U), and poly (A + 2U), and somewhat less so in poly U. K_x is generally in the range 10⁴ > K_X > 10². The cause of these dependences is apparently, primarily, the displacement of Na⁺ by Mg⁺⁺ in poly U and poly (A + U) on the basis of the similarity of extents of displacement measured in this work and those measured potentiometrically. was calculated and was found to approach zero as the concentration of Na⁺ increased. In poly U, poly (A + U), and poly (A + 2U) at low ΔH′ v.H. > 0, about + 2 kcal/“mole.” In poly A, also at low salt, ΔH′ v.H. ≈ ?4 kcal/“mol” for the initial binding of Mg⁺⁺, and increases to +2 kcal/“mol” at saturation. This enthalpic variation probably accounts for the anticooperativity in the binding of Mg⁺⁺ not ascribable to the displacement of Na⁺⁺.     

Optical studies of complexes of quinacrine with DNA and chromatin: implications for the fluorescence of cytological chromosome preparations

The fluorescence and circular dichroism of quinacrine complexed with nucleic acids and chromatin were measured to estimate the relative magnitudes of factors influencing the fluorescence banding patterns of chromosomes stained with quinacrine or quinacrine mustard. DNA base composition can influence quinacrine fluorescence in at least two ways. The major effect, evident at low ratios of quinacrine to DNA, is a quenching of dye fluorescence, correlating with G-C composition. This may occur largely prior to relaxation of excited dye molecules. At higher dye/DNA saturations, which might exist in cytological chromosome preparations stained with high concentrations of quinacrine, energy transfer between dye molecules converts dyes bound near G-C base pairs into energy sinks. In contrast to its influence on quinacrine fluorescence, DNA base composition has very little effect on either quinacrine binding affinity or the circular dichroism of bound quinacrine molecules. The synthetic polynucleotides poly(dA-dT) and poly(dA)-poly(dT) have a similar effect on quinacrine fluorescence, but differ markedly in their affinity for quinacrine and in the circular dichroism changes associated with quinacrine binding. Quinacrine fluorescence intensity and lifetime are slightly less when bound to calf thymus chromatin than when bound to calf thymus DNA, and minor differences in circular dichroism between these complexes are observed. Chromosomal proteins probably affect the fluorescence of chromosomes stained with quinacrine, although this effect appears to be much less than that due to variations in DNA base composition. The fluorescence of cytological chromosome preparations may also be influenced by fixation effects and macroscopic variations in chromosome coiling.     

Sensitive determination of enoxacin in pharmaceutical formulations by its quench effect on the fluorescence of glutathione‐capped CdTe quantum dots

A sensitive and simple method for the determination of enoxacin (ENX) was developed based on the fluorescence quenching effect of ENX for glutathione (GSH)‐capped CdTe quantum dots (QDs). Under optimum conditions, a good linear relationship was obtained from 4.333 × 10^?9 mol?L^?1 to 1.4 × 10^?5 mol?L^?1 with a correlation coefficient (R) of 0.9987, and the detection limit (3σ/K) was 1.313 × 10^?9 mol?L^?1. The corresponding mechanism has been proposed on the basis of electron transfer supported by ultraviolet–visible (UV) light absorption, fluorescence spectroscopy, and the measurement of fluorescence lifetime. The method has been applied to the determination of ENX in pharmaceutical formulations (enoxacin gluconate injections and commercial tablets) with satisfactory results. The proposed method manifested several advantages such as high sensitivity, short analysis time, low cost and ease of operation. Copyright © 2015 John Wiley & Sons, Ltd.     

Fluorescence studies of the binding of a yeast tRNAPhe derivative to Escherichia coli ribosomes.

The equilibrium binding of a highly fluorescent derivative of yeast tRNA^Phe to Escherichia coli 70 S ribosomes was studied fluorimetrically at 7 °C in 25 mm-magnesium. Under these conditions 70 S ribosomes bind two deacylated tRNAs stoichiometrically. An analysis of the binding data using a model in which occupancy of the weaker site requires prior occupancy of the stronger site leads to apparent association constants of (1.00 ± 0.05) × 10⁹m^?1 and (3.4 ± 0.2) × 10⁷m^?1. The use of an independent site model does not change these values appreciably. The observed binding constants do not depend upon the presence or absence of the messenger RNA, poly(U). However, spectroscopic evidence strongly suggests that the anticodons of both bound tRNAs are in contact with the message. This evidence further suggests that in the presence of poly(U) the environment of the hypermodified base adjacent to the anticodon is substantially different in the two sites. This may reflect a difference in the conformation of the anticodon loops or an interaction between the hypermodified base of the weak site tRNA and the anticodon loop of the strong site tRNA.     

Theory of melting of the triple helix poly (A + 2U) for a 1 : 2 mixture of Poly A to Poly U

The Zimm-Bragg theory is extended to treat the melting of the triple helix poly (A + 2U) for a solution with a 1 : 2 mole ratio of poly A to poly U. Only the case for long chains is considered. For a given set of parameters the theory predicts the fraction of segments in the triple helix, double helix, and random coil states as a function of temperature. Four nucleation parameters are introduced to describe the two order–disorder transitions (poly (A + 2U) ? poly A + 2 poly U and poly (A + U) ? poly A + poly U) and the single order–order transition (poly (A + 2U) ? poly (A + U) + poly U). A relation between the nucleation parameters is obtained which reduces the number of independent parameters to three. A method for determining these parameters from experiment is presented. From the previously published data of Blake, Massoulié and Fresco⁸ for [Na⁺] = 0.04, we find σ_T = 6.0 × 10^?4, σ_D = 1.0 × 10^?3, and σσ* = 1.5 × 10^?3. σ_T and σ_D are the nucleation parameters for nucleating a triple helix and double helix, respectively, from a random coil region. σσ* is the nucleation parameter for nucleating a triple helix from a double helix and a single strand. Melting curves are generated from the theory and compared with the experimental melting curves.