Mass spectrometric analysis of recombinant human α-2 interferon

Mass spectrometry (MS) was used for the characterization of recombinant human α-2 interferon (α-2 IFN) produced in E. coli. After purification by monoclonal antibody affinity chromatography, α-2 IFN showed two major peaks in reversed-phase liquid chromatography (RP- LC). Each component was digested with trypsin and Staphylococcus aureus protease V8, separately or in tandem, and the peptide mixture was analysed by MS without further purification. The first peak corresponded to the 165 amino acid sequence of human α-2 IFN and the main component of the second peak was the acetylated Cys₁ α-2 IFN. It was also possible to verify by MS the location of the SS bonds in α-2 IFN and the occurrence of incorrect SS bridges in the products of some renaturation processes. The best renaturation process for obtaining a product without adducts or scrambling of disulphide bonds could be found by using RP-LC and fast atom bombardment MS.     

Anion-pi interactions in cyanuric acids: a combined crystallographic and computational study

Several structures of pi complexes of isocyanuric acid and of several thio derivatives with anions have been computed by using high level ab initio calculations. The nature of the complexes has been studied by means of the method of molecular interaction potential with polarization (MIPp) and Bader's theory of atoms-in-molecules. These molecules form favorable complexes with anions and can be used as binding units for building receptors for the molecular recognition of anions. In several cases, the anion-pi interaction has been demonstrated experimentally by means of X-ray crystallography.     

Dissociation of sulfur dioxide by ultraviolet multiphoton absorption between 224 and 232 nm

Multiphoton excitation and dissociation of SO(2) have been investigated in the wavelength range from 224 to 232 nm. Strong evidence is found for two-photon excitation to the H Rydberg state, followed by dissociation to SO + O and ionization of the SO product by absorption of a third photon. The two-photon excitation is resonantly enhanced via the C (1)B(2) intermediate state, and the two-photon yield spectrum thus bears a strong resemblance to the spectrum of this intermediate. Imaging of the O((3)P(2)), S((1)D(2)), and SO products suggests that, following dissociation of SO(2) from the H state, SO is produced in the A and B electronic states. S((1)D(2)) is produced both from two-photon dissociation of SO(2) to give S((1)D(2)) + O(2) and by single-photon dissociation of SO(+). In the former process, the O(2) is likely formed in all of its lowest three electronic states.