Integrative structure and functional anatomy of a nuclear pore complex.

Nuclear pore complexes play central roles as gatekeepers of RNA and protein transport between the cytoplasm and nucleoplasm. However, their large size and dynamic nature have impeded a full structural and functional elucidation. Here we determined the structure of the entire 552-protein nuclear pore complex of the yeast Saccharomyces cerevisiae at sub-nanometre precision by satisfying a wide range of data relating to the molecular arrangement of its constituents. The nuclear pore complex incorporates sturdy diagonal columns and connector cables attached to these columns, imbuing the structure with strength and flexibility. These cables also tie together all other elements of the nuclear pore complex, including membrane-interacting regions, outer rings and RNA-processing platforms. Inwardly directed anchors create a high density of transport factor-docking Phe-Gly repeats in the central channel, organized into distinct functional units. This integrative structure enables us to rationalize the architecture, transport mechanism and evolutionary origins of the nuclear pore complex.

Charge detection mass spectrometry of bacteriophage P22 procapsid distributions above 20 MDa.

RATIONALE: Charge state resolution is required to determine the masses of ions in electrospray mass spectrometry, a feat which becomes increasingly difficult as the mass increases. Charge detection mass spectrometry (CDMS) circumvents this limitation by simultaneously measuring the charge and the m/z of individual ions. In this work, we have used electrospray CDMS to determine the number of scaffolding proteins associated with bacteriophage P22 procapsids. METHODS: P22 procapsids containing a native cargo of scaffolding protein were assembled in E. coli and purified via differential centrifugation. Electrospray CDMS was used to measure their mass distribution. RESULTS: The procapsid peak was centered at 23.60 MDa, which indicates that they contain an average of ~112 scaffolding proteins. The distribution is relatively narrow, less than 31 scaffolding proteins wide. In addition, a peak at 19.84 MDa with a relative abundance of ~15% is attributed to empty capsids. Despite having the same sizes in solution, the empty capsid and the procapsid have significantly different average charges. CONCLUSIONS: The detection of empty capsids is unexpected and the process that leads to them is unknown. The average charge on the empty capsids is significantly lower than expected from the charge residue model, which probably indicates that the empty capsids have contracted in the gas phase. The scaffolding protein presumably limits the contraction of the procapsids. This work shows that electrospray CDMS can provide valuable information for masses greater than 20 MDa.

Optimized Electrostatic Linear Ion Trap for Charge Detection Mass Spectrometry.

In charge detection mass spectrometry (CDMS), ions are passed through a detection tube and the m/z ratio and charge are determined for each ion. The uncertainty in the charge and m/z determinations can be dramatically reduced by embedding the detection tube in an electrostatic linear ion trap (ELIT) so that ions oscillate back and forth through the detection tube. The resulting time domain signal can be analyzed by fast Fourier transforms (FFTs). The ion's m/z is proportional to the square of the oscillation frequency, and its charge is derived from the FFT magnitude. The ion oscillation frequency is dependent on the physical dimensions of the trap as well as the ion energy. A new ELIT has been designed for CDMS using the central particle method. In the new design, the kinetic energy dependence of the ion oscillation frequency is reduced by an order of magnitude. An order of magnitude reduction in energy dependence should have led to an order of magnitude reduction in the uncertainty of the m/z determination. In practice, a factor of four improvements was achieved. This discrepancy is probably mainly due to the trajectory dependence of the ion oscillation frequency. The new ELIT design uses a duty cycle of 50%. We show that a 50% duty cycle produces the lowest uncertainty in the charge determination. This is due to the absence of even-numbered harmonics in the FFT, which in turn leads to an increase in the magnitude of the peak at the fundamental frequency. Graphical Abstract ᅟ.