Nucleic acid vibrational circular dichroism, absorption, and linear dichroism spectra. II. A DeVoe theory approach

The DeVoe polarizability theory is used to calculate vibrational circular dichroism (VCD) and infrared (IR) absorption spectra of four polyribonucleotides: poly(rA) x poly(rU), poly(rU) x poly(rA) x poly(rU), poly(rG) x poly(rC), and poly(rC+) x poly(rI) x poly(rC). This is the first report on the use of the DeVoe theory to calculate VCD, oriented VCD, IR absorption, and IR linear dichroism (LD) spectra of double- and triple-stranded polyribonucleotides. Results are reported for DeVoe theory calculations--within the base-stretching 1750-1550 cm(-1) spectral region--on several proposed multistranded polyribonucleotide geometries. The calculated spectra obtained from these proposed geometries are compared with previously reported measured and calculated VCD and IR spectral results. Base-base hydrogen-bonding effects on the frequencies and magnitudes of the base carbonyl stretching modes are explicitly considered. The good agreements found between calculated and measured spectra are proposed to be further evidence of the usefulness of the DeVoe theory in drawing three-dimensional structural conclusions from measured polyribonucleotide VCD and IR spectra.

Carbethoxylation of coordinated histidine by diethylpyrocarbonate

The metastable, reversible carbethoxylation of histidine in the cobalt(III) complexes (ethylene-diamine)(histidine)chlorocobalt(III) chloride, [Co(III)(en)ClHis]Cl, and (diethylenetriamine) (histidine)cobalt(III) dichloride, [Co(III)(dien)His]Cl2, following reaction with diethylpyrocarbonate, was observed using UV spectroscopy. These observations indicate that diethylpyrocarbonate can react with a coordinated imidazole ring. CD transitions associated with coordinated carbethoxyhistidine in [Co(III)(en)ClHis]Cl and [Co(III)(dien)His]Cl2 were also observed. The molar ellipticities of the CD bands observed for carbethoxy [Co(III)(en)ClHis]Cl or carbethoxy [Co(III) (dien)His]Cl2 are much larger than the molar ellipticities of the CD transition associated with carbethoxy N alpha-acetyl-L-histidine, indicating that loss of rotational freedom of the imidazole ring could be a major factor in the enhanced CD.

CD spectral comparisons of the acid-induced structures of poly[d(A)], poly[r(A)], poly[d(C)], and poly[r(C)]

CD spectra were used to compare the acid-induced structural transitions of poly[d(A)] and poly[d(C)] with those of poly[r(A)] and poly[r(C)], respectively. The types of base pairing were probably the same in the acid self-complexes of both A-containing polymers and in the acid self-complexes of both C-containing polymers. Similar base pairings were indicated by similarities in the difference CD spectra showing the changes during the first major acid-induced transitions of the polymers. Information from the CD spectra and pKa values of the transitions suggested that the transitions for the RNA polymers involved similar structural changes. The two DNA polymers were markedly different. Single-stranded poly[d(A)] was in the most stacked structure and had the lowest pKa for forming an acid self-complex. Single-stranded poly[d(C)] was in the least stacked structure and had the highest pKa for forming a protonated duplex.

The CD of ligand-DNA systems. 2. Poly(dA-dT) B-DNA

A systematic theoretical study of the CD of [poly(dA-dT)]2 and its complexes with achiral small molecules is presented. The CD spectra of [poly(dA-dT)]2 and of poly(dA):poly(dT) are calculated for various DNA structures using the matrix method. The calculated and experimental spectra agree reasonably well for [poly(dA-dT)]2 but less well for poly(dA):poly(dT). The calculated CD spectrum of [poly(dA-dT)]2 fails to reproduce the wavelength region of 205-245 nm of the experimental spectrum. This discrepancy can be explained by a magnetic dipole allowed transition contributing significantly to the CD spectrum in this region. The induced CD of a transition moment of a molecule bound to [poly(dA-dT)]2 is also calculated. As was the case for [poly(dG-dC)]2, the induced CD of a groove bound molecule is one order of magnitude stronger than that of an intercalated molecule. The calculations also show considerable differences between pyrimidine-purine sites and purine-pyrimidine sites. Both signs and magnitudes of the CD induced into ligands bound in the minor groove agree with experimental observations.

Fluorometric analysis of the long-wavelength absorption band of N-7 methylated GMP into the constituent bands of the two electronic states

Steady-state measurements of fluorescence anisotropy are used to resolve the long-wavelength absorption spectrum of 7-methyl guanosine 5'-monophosphate (GMP) in pH 5 buffer at room temperature into component spectra that correspond to the electronic transitions I and II present in that spectral region. We have chosen this derivative of guanine because its fluorescence quantum yield is much greater than that of GMP. It is found that the data are adequately described by a model that involves emission exclusively from state I, with state II converting to it with 100% efficiency. The shape of the absorption spectrum of state II is virtually independent of the angle theta between the absorption transition dipole moments of states I and II, whereas that of state I is dependent on theta. We analyze the data on the basis of the premise that in the short-wavelength region state II is the predominantly absorbing state. This premise is based on studies of single-crystal polarized reflection and linear dichroism from stretched films. The spectral maxima for the two states are found to be at about 290 and 260 nm, respectively. There is also a weak band which is centered at about 245 nm. The oscillator strengths are found to be 0.07, 0.21 and approximately 0.04, for states I, II and that associated with the weak band, respectively. The importance of these findings with regard to the photophysical properties of nucleic acids and calculations of their CD spectra is discussed.

Immunological detection of B-DNA to Z-DNA transition of polynucleotides by immobilization of the DNA conformation on a solid support

We studied the B-DNA to Z-DNA transition of poly(dG-dC).poly(dG-dC) and poly(dG-m5dC).poly(dG-m5dC) in the presence of NaCl using an enzyme immunoassay. The polynucleotides were coated on microtiter plates at varying concentrations of NaCl and treated with a monoclonal anti-Z-DNA antibody, Z22. The plates were subsequently treated with alkaline phosphatase conjugated polyvalent mouse immunoglobulins and the enzyme substrate, p-nitrophenyl phosphate. The color development due to the enzyme-substrate reaction was quantitated using a microplate autoreader. Our results show that the antibody does not recognize the polynucleotides in the B-DNA conformation and binds strongly to the Z-DNA conformation. A smooth transition curve is obtained at intermediate concentrations of the counterions. From the transition curves, we determined the concentration of the counterions at the midpoint of B-DNA to Z-DNA transition. The midpoint concentrations for poly(dG-dC).poly(dG-dC) and poly(dG-m5dC).poly(dG-m5dC) are 2.3 and 0.74 M NaCl, respectively. Using the immunological method, we also examined the B-DNA to Z-DNA transition of poly(dG-m5dC).poly(dG-m5dC) in the presence of naturally occurring polyamines. The midpoint concentrations of the polyamines are as follows: putrescine, 2.5 mM; spermidine, 34 microM; spermine, 1.8 microM. The midpoint values determined by the enzyme immunoassay are in good agreement with those determined by circular dichroism and ultraviolet absorption spectroscopic measurements. These results demonstrate that immobilization of a preexisting conformation or a mixture of conformations of DNA on a solid support followed by a titration of the DNA conformations using a monoclonal anti-DNA antibody is an excellent method to study the conformational dynamics of DNA.