Dependence of 4'-(hydroxymethyl)-4,5',8-trimethylpsoralen photoaddition on the conformation of ribonucleic acid

The photoaddition of 4'-(hydroxymethyl)-4,5',8-trimethylpsoralen (HMT) to different conformational states of RNA was studied. Poly(U), poly(A,U) (random copolymer), poly(A-U) (alternating copolymer), poly(A) . poly(U) (double stranded), and poly(U) . poly(A) . poly(U) (triple stranded) were reacted with HMT at different temperatures and salt concentrations. The conformation of the polymers was monitored by UV absorption and circular dichroism. It was found that the rate of HMT photoaddition changed dramatically at structural transitions in the RNA. The alternating copolymer poly(A-U) was found to have the highest rate of addition. Low salt and temperature produced maximal incorporation.     

Segmental flexibility of single-, double-, and triple-stranded polyribonucleotides from the data of spin label method. Formation of the triple-stranded poly(A.A.U) polynucleotide helix

Segmental mobility dynamic peculiarities of poly(U), poly(A) and poly(C) synthetic polymers and their complexes were investigated by spin-label method. Imidazolide spin-label was introduced into 2'-oxi-groups of polymer ribose in correlation: one spin-label on 18-20 bases. Formation of complexes was observed by ESR spectra at two pH: 4.2 and 7.2. Segmental mobility of only single strand spin-labelled polymer segment and in the complex was evaluated by measuring rotational correlation time (tau) determined by dependence of distances between outer wide extrema in ESR spectra from solvent viscosity at different temperatures. It turned out that correlation time tau of single strand structures in a high degree depend on pH and temperature. For three strand structures abrupt increase of tau because of appearance of rigidity was observed. It is possible to evaluate part of triple complexes poly(U.A.A) and poly(U.U.A) existing in dynamic equilibrium depending on pH and temperature by the form of outer wide extrema. Adding of dye to complex of poly(U).poly(A) causes an increase of rigidity of the supermolecular structure. Quantitative characteristics of formed complexes were obtained by simulation of ESR spectra on computer.     

1H-nmr comparative studies of polynucleotides: Conformation and dynamic structure of polyribo(uridylic) and polyribo(cytidylic) acids in neutral solution

The conformation and the dynamic structure of single-stranded poly(U) and poly(C) in neutral aqueous solution have been investigated by ¹H-nmr at two different frequencies (90 and 250 MHz) and at various temperatures. Measurements of proton chemical shifts, coupling constants J_H-H, and proton relaxation times, T₁, T₂, versus temperature show a striking difference in conformation and in dynamic structure between the two polynucleotides studied. The temperature effect on δ and J_H-H is found to be substantial for poly(C) and insignificant for poly(U). The S conformer is favored in poly(U), whereas the N conformer strongly predominates in poly(C) (?90%), similar to the case for RNAs. These results suggest that single-stranded poly(C) probably possesses a helical or partial helical structure, whereas poly(U) shows a clear preference for the random coil, in agreement with the optical results. The local motions of the ribose and base were studied at various temperatures by measurements on the relaxation times at 90 and 250 MHz. For a given temperature between 22 and 72°C, the ratio T₁(90)/T₁(250) is practically the same for all poly(U) protons, indicating that in this temperature interval the ribose base unit of poly(U) undergoes an isotropic motion characterized by a single correlation time τ_c. Above 52°C, poly(C) exhibits a dynamic structure similar to poly(U). Below this temperature, poly(C) exists in an equilibrium between randomly coiled and single-stranded helix forms. This situation is characterized by a strong cross-relaxation effect and T₁ values corresponding to a relatively short apparent correlation time. An activation energy of 4 kcal/mol was determined for the motion of the ribose–base unit in both single-stranded polynucleotides.     

Concentration and temperature effects in interactions of the dye pyronine G with polynucleotides

The interaction of poly(A) and poly(A).poly(U) with pyronine G dye depending on the concentration of components and temperature was studied spectrophotometrically in the visible and UV ranges at pH (6.86). It was found that the interaction of pyronine G with poly(A) and poly(A).poly(U) results in the formation of two types of complexes. The relation of the equilibrium concentrations of these complexes depends on the initial concentrations of the components in solution. The formation of complex I results in shifting the spectrum towards the short wave range with regard to the monomer band and reflects the aggregation of the dye cations. Complex II is characterized by the shift towards the long wave range. Complex II is formed in considerable amounts for poly(A).pyronine G system at large P/D and for poly(A).poly(U).pyronine G system at P/D = 5-6 and is probably due to the interaction between the dye and polynucleotides of the intercalation type or reflects the interaction between the dye and two negatively charged phosphate groups. Analysis of temperature measurements of spectra confirms the formation of various types of complexes in the system studied.     

Demonstration of G . U wobble base pairs by Raman and IR spectroscopy

When guanine and uracil form hydrogen bonds in the pairing scheme first proposed by Crick one would expect that poly(A,G) will form an unperturbed double helix with poly U at room temperature in a dilute electrolyte solution (0.1 M NaCl). We have demonstrated by Raman- and IR-spectroscopy that the secondary structure of poly(A.G) · poly U is very similar to the structure of poly A · poly U; only the thermal stability of the double helix seems slightly lower than the stability of poly A · poly U, whereas the average helix length is unaffected by the dispersed G · U base pairs. From our input ratio of guanine and adenine we estimate that about every fourth base pair is a wobble pair.     

Calorimetric determination of the heat capacity changes associated with the conformational transitions of polyriboadenylic acid and polyribouridylic acid

The heat capacities of the single-stranded and double-stranded forms of polyadenylic acid, polyuridylic acid, and poly(uridylic and adenylic acid) were determined with a drop heat capacity calorimeter. In addition, the temperature dependence of the apparent partial heat capacity (?Cp) was measured with a newly developed differential scanning calorimeter. The calculated ΔCp at 28°C for the transition poly(A)·poly(A) ? 2 poly(A) was found to be 165 ± 24 cal/Kmol-base pair, compared with a value of 140 ± 28 for the transition poly(A)·poly(U) ? poly(A) + poly(U). The temperature dependence of ?Cp of single-stranded poly(U) was consistent with the conclusion that it is totally unstacked at temperatures above 15°C. The temperature dependence of ?Cp of single-stranded poly(A) was used to determine the base-stacking parameters for poly(A). The experimental results are consistent with a stacking enthalpy change of ?8.5 ± 0.1 kcal/mol bases and a cooperativity parameter σ of 0.57 ± 0.03 for the stacking of adenine bases. These results demonstrate that the heat capacity of single-stranded polynucleotides is greater than that of the double-stranded forms. This increased heat capacity is mainly the result of the temperature dependence of the base-stacking interactions in the single-stranded form.     

Identification of an altered elongation factor in temperature-sensitive mutant ts 7'-14 of Saccharomyces cerevisiae

Postpolysomal extracts from wild-type (wt A364A) and temperature-sensitive (ts 7'-14) yeast cells were preincubated for short periods of time at the nonpermissive temperature (37-41 degrees C) prior to incubations for protein synthesis at 20 degrees C. Whereas wt A364A extracts were relatively unaffected by preincubation at the elevated temperature, mutant extracts lost their ability to translate exogenous natural mRNA and poly(U). Phe-tRNA synthetase and ribosomes from ts 7'-14 cells were not inactivated by preincubation at 37-41 degrees C, but a cytosolic component required for chain elongation, as measured by poly(U) translation, was extensively inactivated. The three elongation factors (EF-1, EF-2, and EF-3) required for chain elongation in yeast were resolved chromatographically. Only one factor, EF-3, was able to restore the poly(U)-translational activity of mutant extracts inactivated at the elevated temperature. Heat-inactivated yeast cytosols, which did not support protein synthesis with yeast ribosomes, were perfectly able to translate poly(U) with rat liver ribosomes, which require only EF-1 and EF-2. These and other experiments indicated that the genetically altered component in 7'-14 mutant cells is EF-3.     

Binding kinetics of mercury(II) TO POLYRIBONUCLEOTIDES.

Kinetic studies of the interaction of Hg(II) with polyribonucleotides have been used to investigate structural fluctuations of the bases in nucleic acids. The reaction of Hg(II) with poly(A)-poly(U) occurs in two phases which differ in time scale by a factor of about 100. The slow phase is first order and exhibits cooperativity or autocatalytic kinetics. The rate is found to increase as decreasing chain length of poly(U) is used to make the double helical complex. The reaction appears to initiate at the ends of poly(U) strands and may be associated with a molecular rearrangement which results in strand separation with Hg(II) being linked only to uridine. The fast reaction phase is second order ans shows little cooperative behavior. Protons are released at this stage indicating alteration of the double helix. The measured second-order rate constant is nearly three orders of magnitude smaller than that found for poly(U) alone. This rate difference suggests that the reactive sites are blocked by double helix formation, and become available for reaction with Hg(II) only through a structural fluctuation. The ratio of rate constants for the reaction of Hg(II) with poly(U) and poly(A)-poly(U) was used to place an upper limit on the equilibrium constant for the structural fluctuation of 2 times 10- minus 3 at 15 degrees and 0.5 M NaClO4. The heat of the "breathing" reaction can be estimated to be similar to 9 kcal/mol from comparison of the temperature coefficient of the reaction with poly(U) to that with poly(A)-poly(U).     

Physical and coding properties of poly(5-methoxyuridylic) acid.

The synthesis of poly(mo5U) requires a high concentration (2.7 mg/ml) of polynucleotide phosphorylase as well as a long reaction time (48 h). The resulting polynucleotide has a chain length of approximately 100 nucleotides. It shows no indication of a stable secondary structure. When poly(mo5U) is mixed with poly(A), a triple-stranded complex poly(A) . 2poly(mo5U) is formed. This complex has a melting temperature of 68.5 +/- 0.5 degrees C at 150 mMNa+ and exhibits a hysteresis loop between melting and reformation of the complex having a delta Tm of 11.5 degrees C. Poly-5-methoxyuridylic acid stimulates the binding of Phe-tRNA to 70-S ribosomes but is inactive in directing poly(Phe) synthesis.     

A.U and G.C base pairs in synthetic RNAS have characteristic vacuum UV CD bands.

The vacuum UV CD spectra of GpC, CpG, GpG, poly[r(A)], poly[r(C)], poly[r(U)], poly[r(A-U)], poly[r(G).r(C)], poly[r(A).r(U)], and poly[r(A-U).r(A-U)] were measured down to at least 174 nm. These spectra, together with the published spectra of poly[r(G-C).r(G-C)], CMP, and GMP, were sufficient to estimate the CD changes upon base pairing for four double-stranded RNAs. The vacuum UV CD bands of poly[r(A)], poly[r(C)], and the dinucleotides GpC and CpG were temperature dependent, suggesting that they were due to intrastrand base stacking. The dinucleotide sequence isomers GpC and CpG had very different vacuum UV CD bands, indicating that the sequence can play a role in the vacuum UV CD of single-stranded RNA. The vacuum UV CD bands of the double-stranded (G.C)-containing RNAs, poly[r(G).r(C)] and poly[r(G-C).r(G-C)], were larger than the measured or estimated vacuum UV CD bands of their constituent single-stranded RNAs and were similar in having an exceptionally large positive band at about 185 nm and negative bands near 176 and 209 nm. These similarities were enhanced in difference-CD spectra, obtained by subtracting the CD spectra of the single strands from the CD spectra of the corresponding double strands. The (A.U)-containing double-stranded RNAs poly[r(A).r(U)] and poly[r(A-U).r(A-U)] were similar only in that their vacuum UV CD spectra had a large positive band at 177 nm. The spectrum of poly[r(A).r(U)] had a shoulder at 188 nm and a negative band at 206 nm, whereas the spectrum of poly[r(A-U).r(A-U)] had a positive band at 201 nm. On the other hand, difference spectra of both of the (A.U)-containing polymers had positive bands at about 177 and 201 nm. Thus, the difference-CD spectra revealed CD bands characteristic of A.U and G.C base pairing. (ABSTRACT TRUNCATED AT 250 WORDS)     

The role of a template sugar-phosphate backbone in the ribosomal decoding mechanism. Comparative study of poly(U) and poly(dT) template activity

To study the role of a template sugar-phosphate backbone in the ribosomal decoding process, poly(U), poly(dT) and poly(dU)-directed cell-free amino acid incorporation was investigated under the influence of neomycin and high concentrations of Mg2+. The specificity of a factor-dependent translation system of Escherichia coli was shown to change according to the principle: "either ribo- or deoxyribopolynucleotide messenger". Poly(dT) is shown to be effectively translated in the absence of elongation factors, both at low (2 degrees C) and high (37 degrees C) temperature. Neomycin inhibits factor-free poly(dT) translation. Little or no poly(U) translation is observed in this system. A chromatographic analysis of the oligophenylalanine residues synthesized seems to show that translocation is the main step responsible for ribosome specificity to the ribo- or deoxyribopolynucleotide template in both factor-dependent and factor-free translation systems.     

Study of salt effects on adenosine–polyuridylic acid interaction

Complex formation between poly(U) and adenosine in solutions of salts that stabilize (Na₂SO₄), destabilize (NaClO₄), or have little effect on the water structure (NaCl), as well as the poly(U)·poly(A) interaction in NaClO₄, was studied by equilibrium dialysis and uv spectroscopy. At 3°C and neutral pH, Ado·2 poly(U) is formed in 1M NaCl and 0.33M Na₂SO₄. In NaClO₄ solutions under the same conditions, an Ado·poly(U) was found over the whole range of salt concentration investigated (10 mM?1M), which has not been previously observed under any conditions. The Ado-poly(U) was also found in a NaCl/NaClO₄ mixture, the transition from the triple- to the double-helical complex occurring within a narrow range of concentration of added NaClO₄. In the presence of 1M NaCl this transition is observed on adding as little as 10 mM NaClO₄, i.e., at a [ClO]/[Cl^?] ratio of about 1:100. However, when NaClO₄ is added to a 1M solution of the stabilizing salt Na₂SO₄, no transition occurs even at a [ClO]/[SO] ratio of 1:4. Investigation of melting curves and uv spectra has shown that in an equimolar mixture of the polynucleotides, only a double-helical poly(U)·poly(A) exists in 1M NaClO₄ at low temperatures; this also holds for 1M NaCl. This changes to a triple-helical 2 poly(U)·poly(A) and then dissociates as the temperature increases. At low temperatures and the poly(U)/poly(A) concentration ratio of 2:1, a mixture of 2 poly(U)·poly(A) and poly(U)·poly(A) was observed in 1M NaClO₄, in contrast to the case of 1M NaCl. Thus, sodium perchlorate, a strong destabilizer of water structure, promotes formation of double-helical complexes both in the polynucleotide–monomer and the polynucleotide–polynucleotide systems. Beginning with a sufficiently high ionic strength (μ ? 0.9), a further increase in the salt molarity results in an increase of the poly(U)·adenosine melting temperature in both stabilizing and neutral salts and a decrease in the destabilizing salt. In Na₂SO₄ concentrations higher than 1.2M Ado·2 poly(U) precipitates at room temperature. Analysis of the binding isotherms and melting profiles of the complexes between poly(U) and adenosine according to Hill's model shows that the cooperativity of binding, due to adenosine stacking on poly(U), increases in the order NaClO₄ < NaCl < Na₂SO₄. The free energy of adenosine stacking on the template is similar to that of hydrogen bonding between adenosine and poly(U) and ranges from ?1 to ?2 kcal/mol. The values of ΔH_t [the effective enthalpy of adenosine binding to poly(U) next to an occupied site, obtained from the relationship between complex melting temperature and free monomer concentration at the midpoint of the transition] are ?14.2, ?18.3, and ?16.8 kcal/mol for 1M solutions of NaClO₄, NaCl, and Na₂SO₄, respectively. The results indicate that the effects of anions of the salts studied are related to water structure alterations rather than to their direct interaction with the complexes between poly(U) and adenosine.     

Fractionation of plant Polyadenylated RNA on the basis of poly(A) size

Polyadenylated RNA from Vicia faba meristematic root cells was fractionated on the basis of mean poly(A) size by a thermal stepwise elution from poly(U) Sepharose. Such a procedure allowed the elimination of contaminating RNA at 30° and the collection of two populations of purified polyadenylated RNA at 40° and 50°, respectively. RNA eluting at the higher temperature carried a poly(A) segment (mean size of 100 nucleotides), twice as large as the RNA eluting at the lower temperature.     

New aspects of the interaction of the antibiotic coralyne with RNA: coralyne induces triple helix formation in poly(rA)?poly(rU)

The interaction of coralyne with poly(A)•poly(U), poly(A)•2poly(U), poly(A) and poly(A)•poly(A) is analysed using spectrophotometric, spectrofluorometric, circular dichroism (CD), viscometric, stopped-flow and temperature-jump techniques. It is shown for the first time that coralyne induces disproportionation of poly(A)•poly(U) to triplex poly(A)•2poly(U) and single-stranded poly(A) under suitable values of the [dye]/[polymer] ratio (C_D/C_P). Kinetic, CD and spectrofluorometric experiments reveal that this process requires that coralyne (D) binds to duplex. The resulting complex (AUD) reacts with free duplex giving triplex (UAUD) and free poly(A); moreover, ligand exchange between duplex and triplex occurs. A reaction mechanism is proposed and the reaction parameters are evaluated. For C_D/C_P> 0.8 poly(A)•poly(U) does not disproportionate at 25°C and dye intercalation into AU to give AUD is the only observed process. Melting experiments as well show that coralyne induces the duplex disproportionation. Effects of temperature, ionic strength and ethanol content are investigated. One concludes that triplex formation requires coralyne be only partially intercalated into AUD. Under suitable concentration conditions, this feature favours the interaction of free AU with AUD to give the AUDAU intermediate which evolves into triplex UAUD and single-stranded poly(A). Duplex poly(A)•poly(A) undergoes aggregation as well, but only at much higher polymer concentrations compared to poly(A)•poly(U).     

Poly(U) binding to ascites cells of the 13762A rat mammary adenocarcinoma: Evidence for a protein receptor on the cell surface

Ascites cells of the 13762 rat mammary adenocarcinoma bind poly(U) in a reaction that is complete within 5 min at 0°C. Poly(U) binding is saturable; the capacity of these cells is 5×10⁷ UMP residues/cell (approx. 2×10⁵ chains/cell). Most [³H]poly(U) bound in the rapid reaction can be recovered in an undergraded state. However, it is rapidly degraded by low concentrations of exogenous pancreatic ribonuclease. The magnitude of binding is independent of temperature and ionic conditions, and is unaffected by metabolic inhibitors or concanavalin A (ConA). Radioactivity presented as [³H]poly(U) tends to co-fractionate with 5′-nucleotidase after homogenization of cells in the media of low ionic strength, but is efficiently released from cells exposed to protein denaturants that effectively fix cellular RNA in situ. Cells pretreated with proteolytic enzymes have sharply reduced capacities to bind poly(U). Autoradiography of cells bearing [³H]poly(U) demonstrates a uniform distribution of radioactivity through the cell population and is consistent with binding to the plasma membrane. These and other results imply that binding of poly(U) to 13762 ascites cells is mediated by protein receptors on the cell surface.     

Electro-optical studies of conformation and interaction of polynucleotides

Measurements by the technique of electric birefringence with pulsed sinusoidal electric fields on polyriboadenylic acid (poly-A) and polyribouridylic acid (poly-U) indicate that the kinetics of the double-stranded helix formation of poly (A + U) in the presence of Mg²⁺ is second order and consists of two steps: nucleation and propagation of base pairs from nuclei. The nucleation involves approximately 7 base pairs. It seems that the requirement of 7 base pairs to start the formation of a double-stranded helix is not peculiar to poly (A + U) but is associated with double-stranded helices of polynucleotides in general. This implies that it may be associated with spatial requirements of the phosphate-sugar backbone, rather than with the particular bases linked to the backbone. The decline in rate of poly (A + U) formation observed above a critical temperature is the consequence of changes in the poly-A conformation setting in at this critical temperature, rather than resulting from an increase in the reversibility of the base-pair propagation step of double-stranded helix formation. The dominant role of the conformation of poly-A in the double-stranded helix formation of poly (A + U) is further borne out by the pH dependence of the rate which completely parallels the conformation changes known to occur in poly-A as a function of pH. This indirectly suggests that at neutral pH poly-A is a single-stranded helix. The rotary diffusion coefficients attest to the flexibility of this helix, while the stacked nature of the base pairs at low temperatures is revealed by the identical increments in the specific Kerr constant on going from poly-A to poly (A + U) and from poly (A + U) to poly (A + 2U) helices. Results suggest that Mg²⁺ binds to the phosphate part of the backbone. Poly-U binds Mg²⁺ more strongly than poly-A; this difference in binding strength is attributed to differences in conformation (random coil versus helix). It is also borne out by the present results that the degree of order in the structure of poly-U, even at low temperatures and neutral pH, is at best an order of magnitude smaller than that of poly-A under similar conditions. Furthermore, the earlier proposed double-stranded structure of poly-U is called into question. A hairpinlike structure seems to agree with results of this investigation. Finally, the results support the contention that the ion atmosphere polarization is responsible for orientation of polyelectrolytes in the presence of alternating electric fields in the neighborhood of 25 kc./sec. frequency.     

Non-snRNP U1A levels decrease during mammalian B-cell differentiation and release the IgM secretory poly(A) site from repression

A regulated shift from the production of membrane to secretory forms of Immunoglobulin M (IgM) mRNA occurs during B cell differentiation due to the activation of an upstream secretory poly(A) site. U1A plays a key role in inhibiting the expression of the secretory poly(A) site by inhibiting both cleavage at the poly(A) site and subsequent poly(A) tail addition. However, how the inhibitory effect of U1A is alleviated in differentiated cells, which express the secretory poly(A) site, is not known. Using B cell lines representing different stages of B cell differentiation, we show that the amount of U1A available to inhibit the secretory poly(A) site is reduced in differentiated cells. Undifferentiated B cells have more total U1A than differentiated cells and a greater proportion of this is not associated with the U1snRNP. We show that this is available to inhibit poly(A) addition at the secretory poly(A) site using cold competitor RNA oligos to de-repress poly(A) addition in nuclear extracts from the respective cell lines. In addition, endogenous non-snRNP associated U1A-immunopurified from the different cell lines-inhibits poly(A) polymerase activity proportional to U1A recovered, suggesting that available U1A level alone is responsible for changes in its inhibitory effect at the secretory IgM poly (A) site.     

Calorimetric study of the complexes between polyuridylic acid and adenylic nucleotides.

Soluble complexes of poly (U) and adenylic nucleotides in NaCl solutions were studied by scanning microcalorimetry. The melting enthalpies, delta Hm, of poly (U) complexes with adenosine, 2',3' -cAMP, 2'(3')-AMP, 5-AMP, ADP, ATP in 1 M NaCl are 50.5; 45.0; 42.9; 28.6; 26.1 and 25.6 kJ/mole triplets, respectively. Delta Hm is independent of the complex melting temperature, Tm. The calorimetric enthalpies are considerably lower than the apparent delta Hv.H. obtained from Tm dependence on free monomer concentration. The enthalpy of complex formation in 1 M NaCl depends neither ob the number nor on the degree of ionization of the phosphate groups but is essentially determined by their 5' - or 2'(3')-position. In contrast to 2'(3')- AMP. 2 poly (U), delta Hm of 5'AMP. 2 poly (U) increases considerably at lowering Na+ concentration. The enthalpy of poly (U) double helix melting in 1 M NaCl is 8.8 kJ/mole pairs which is 2.5 times lower than that in MgCl2 solutions.