The predicted structure has been calculated for a protein-based biosensor for inorganic phosphate (Pi), previously developed by some of us (Okoh et al., Biochemistry, 2006, 45, 14764). This is the phosphate binding protein from Escherichia coli labelled with two rhodamine fluorophores. Classical molecular dynamics and hybrid Car-Parrinello/molecular mechanics simulations allow us to provide molecular models of the biosensor both in the presence and in the absence of Pi. In the latter case, the rhodamine fluorophores maintain a stacked conformation in a 'face A to face B' orientation, which is different from the 'face A to face A' stacked orientation of free fluorophores in aqueous solution (Ilich et al., Spectrochim. Acta, Part A, 1996, 52, 1323). A protein conformation change upon binding Pi prevents significant stacking of the two rhodamines. In both states, the rhodamine fluorophores form hydrophobic contact with LEU291, without establishing significant hydrogen bonds with the protein. The accuracy of the models is established by a comparison between calculated and experimental absorption and circular dichroism spectra.

Binding of small molecules to their targets triggers complex pathways. Computational approaches are keys for predictions of the molecular events involved in such cascades. Here we review current efforts at characterizing the molecular determinants in the largest membrane-bound receptor family, the G-protein-coupled receptors "GPCRs…. We focus on odorant receptors, which constitute more than half GPCRs. The work presented in this review uncovers structural and energetic aspects of components of the cellular cascade. Finally, a computational approach in the context of radioactive boron-based antitumoral therapies is briefly described.

We present Car-Parrinello and Car-Parrinello/molecular mechanics simulations of the structural, vibrational, and electronic properties of formaldehyde in water. The calculated properties of the molecule reproduce experimental values and previous calculations. The n → π* excitation energy, calculated with TDDFT and CASPT2, agrees with experimental data. In particular, it shows a blue shift on going from the gas phase to aqueous solution. Temperature and wave function polarization contributions have been disentangled.