Insights into the Mechanism of Action of Ferroquine. Relationship between Physicochemical Properties and Antiplasmodial Activity

Ferroquine (FQ) is a 4-aminoquinoline antimalarial which contains a quinoline nucleus similar to chloroquine, but a novel ferrocenic group in its side chain. Previous work has demonstrated that this compound has excellent activity against malaria parasites, both in vitro and in vivo, with especially good activity against chloroquine-resistant parasites, but details of its mechanism of action have not previously been reported. In this study, we have investigated the physicochemical properties of FQ for comparison with chloroquine (CQ). Like CQ, FQ forms complexes with hematin in solution (log K = 4.95 ± 0.05). FQ is an even stronger inhibitor of -hematin formation than CQ (IC50 = 0.78 equiv relative to hematin for FQ vs 1.9 for CQ). These data suggest that the mechanism of action of FQ is likely to be similar to that of CQ and probably involves hematin as the drug target and inhibition of hemozoin formation. However, both the basicity and lipophilicity of FQ are significantly different from those of CQ. The lipophilicity of FQ and CQ are similar when protonated at the putative food vacuole pH of 5.2 (log D = -0.77 and -1.2 respectively), but differ markedly at pH 7.4 (log D = 2.95 and 0.85 respectively). In addition, the pKa values of FQ are lower (pKa1 = 8.19 and pKa2 = 6.99) than those of CQ (10.03 and 7.94, respectively). This suggests that there will be somewhat less vacuolar accumulation of FQ compared with CQ. Single crystal structure determination of FQ shows the presence of a strong internal hydrogen bond between the 4-amino group and the terminal N atom. This, together with the electron donating properties of the ferrocene moiety, probably explains the decreased pKa. Interestingly, the decreased accumulation arising from the less basic behavior of this compound is partly compensated for by its stronger -hematin inhibition. Increased lipophilicity, differences in geometric and electronic structure, and changes in the N-N distances in FQ compared to CQ probably explain its activity against CQ-resistant parasites

The HARP detector at the CERN PS

HARP is a high-statistics, large solid angle experiment to measure hadron production using proton and pion beams with momenta between 1.5 and 15 GeV/c impinging on many different solid and liquid targets from low to high Z. The experiment, located in the T9 beam of the CERN PS, took data in 2001 and 2002. For the measurement of momenta of produced particles and for the identification of particle types, the experiment includes a large-angle spectrometer, based on a Time Projection Chamber and a system of Resistive Plate Chambers, and a forward spectrometer equipped with a set of large drift chambers, a threshold Cherenkov detector, a time-of-flight wall and an electromagnetic calorimeter. The large angle system uses a solenoidal magnet, while the forward spectrometer is based on a dipole magnet. Redundancy in particle identification has been sought, to enable the cross-calibration of efficiencies and to obtain a few percent overall accuracy in the cross-section measurements. Detector construction, operation and initial physics performances are reported. In addition, the full chain for data recording and analysis, from trigger to the software framework, is described

The HARP detector at the CERN PS

HARP is a high-statistics, large solid angle experiment to measure hadron production using proton and pion beams with momenta between 1.5 and 15 GeV/c impinging on many different solid and liquid targets from low to high Z. The experiment, located in the T9 beam of the CERN PS, took data in 2001 and 2002. For the measurement of momenta of produced particles and for the identification of particle types, the experiment includes a large-angle spectrometer, based on a Time Projection Chamber and a system of Resistive Plate Chambers, and a forward spectrometer equipped with a set of large drift chambers, a threshold Cherenkov detector, a time-of-flight wall and an electromagnetic calorimeter. The large angle system uses a solenoidal magnet, while the forward spectrometer is based on a dipole magnet. Redundancy in particle identification has been sought, to enable the cross-calibration of efficiencies and to obtain a few percent overall accuracy in the cross-section measurements. Detector construction, operation and initial physics performances are reported. In addition, the full chain for data recording and analysis, from trigger to the software framework, is describe