A series of negatively charged alpha-helical peptides of the general formula fluorenylmethoxycarbonyl (Fmoc)-D(x)A(y)K(z) were synthesized, where x and z were 1, 2, or 3 and y was 10, 14, 18, or 22. The translocation of the peptides through single pores, which were self-assembled into lipid membranes, was analyzed by measuring the current blockade i(block) and the duration t(block). The pores were either alpha-hemolysin, which has a wide vestibule leading into the pore, or aerolysin, which has no vestibule but has a longer pore of a similar diameter. Many thousands of events were measured for each peptide with each pore, and they could be assigned to two types: bumping events (type I) have a small i(block) and long t(block), and translocation events (type II) have a larger i(block) and shorter t(block). For type-II events, both i(block) and t(block) increase with the length of the peptides on both pores tested. The dipole moment and the net charge of each peptide has a major effect on the transport characteristics. The ratio of type-II/type-I events increases as the dipole moment increases, and uncharged peptides gave mostly type-I events. The structural differences between the two nanopores were reflected in the characteristic values of i(block), and in particular, the vestibule of alpha-hemolysin helps to orient the peptides for translocation. Overall, the results demonstrate that the nanopore technology can provide useful structural information but peptide sequencing will require further improvements in the design of the pores.

HPr is a small protein that must unfold to translocate the α‐hemolysin pore (see image). Single amino acid substitutions can cause large changes to the translocation parameters. A conservative mutation is sufficient to alter the event profile; either the mutant must unfold differently or it must interact with the pore differently. A negatively charged mutant is driven through the pore, which facilitates unfolding.

In the absence of Zn(II) a single Zn‐finger module such as Zif268 is unfolded and can translocate an α‐hemolysin pore (see image). Upon addition of Zn(II), the protein folds and is too large to translocate so that only bumping events are observed. In contrast, upon addition of Co(II) or Mg(II), there are only small changes to the event profiles.

Peptides of 12 amino acids were tethered via a terminal cysteine to mono-, di-, tri-, and tetrabromomethyl-substituted benzene to produce bundles of one to four peptide strands (CY12-T1 to CY12-T4, respectively). The interaction of the bundles with the α-hemolysin pore was assessed by measuring the blockade currents (I) and times (T) at an applied potential of - 50, - 100, and - 150 mV. Three types of events could be distinguished: bumping events, with small I and short T where the molecule transiently interacts with the pore before diffusing away; translocation events, where the molecule threads through the pore with large I and the value of T decreases with increasing voltage; and intercalation events, where the molecule transiently enters the pore but does not translocate with large I and the value of T increases with increasing voltage. CY12-T1 and CY12-T2 gave only bumping and translocation events; CY12-T3 and CY12-T4 also gave intercalation events, some of which were of very long duration. The results suggest that three uncoiled peptide strands cannot simultaneously thread through the α-hemolysin pore and that proteins must completely unfold in order to translocate.

Nanopore analysis is an emerging technique of structural biology which employs nanopores, such as the α-hemolysin pore, as a biosensor. A voltage applied across a membrane containing a nanopore generates a current, which is partially blocked when a molecule interacts with the pore. The magnitude (I) and the duration (T) of the current blockade provide an event signature for that molecule. Two peptides, CY12(+)T1 and CY12(-)T1 with net charges + 2 and - 2, respectively, were analysed using different applied voltages and all four possible orientations of the electrodes and pore. The four orientations were vestibule downstream (VD), vestibule upstream (VU), stem downstream (SD) and stem upstream (SU) where vestibule and stem refer to the side of the pore on which the peptide was placed and downstream and upstream refer to the application of a positive or negative electrophoretic force, respectively. For CY12(+)T1, the effect of voltage on the event duration was consistent with translocation in the VD and SD configurations, but only intercalation events were observed in the VU and SU configurations. For CY12(-)T1, translocations were only observed in the VD and VU configurations. The results are interpreted in terms of two energy barriers on either side of the lumen of the pore. The difference in height of the barriers determines the preferred direction of exit. Electroosmotic flow and current rectification due to the pore as well as the dipole moment and charge of the peptide also play significant roles. Thus, factors other than simple electrophoresis are important for determining the interaction of small peptides with the pore.

Nanopore analysis can be used to study conformational changes in individual peptide or protein molecules. Under an applied voltage there is a change in the event parameters of blockade current or time when a molecule bumps into or translocates through the pore. If a molecule undergoes a conformational change upon binding a ligand or metal ion the event parameters will be altered. The objective of this research was to demonstrate that the conformation of the prion protein (PrP) and prion peptides can be modulated by binding divalent metal ions. Peptides from the octarepeat region (Octa2, (PHGGGWGQ)2 and Octa 4, (PHGGGWGQ)4), residues 106-126 (PrP106-126), and the full-length Bovine recombinant prion (BrecPrP) were studied with an alpha-hemolysin pore. Octa2 readily translocated the pore but significant bumping events occurred on addition of Cu(II) and to a lesser extent Zn(II), demonstrating that complex formation was occurring with concomitant conformational changes. The binding of Cu(II) to Octa4 was more pronounced and at high concentrations only a small proportion of the complex could translocate. Addition of Zn(II) also caused significant changes to the event parameters but Mg(II) and Mn(II) were inert. Addition of Cu(II) to PrP106-126 caused the formation of a very tight complex, which could not translocate the pore. Small changes were observed with Zn(II), but not with Mg(II) or Mn(II). Analysis of BrecPrP showed that about 37% were translocation events, but on addition of Cu(II) or Zn(II) these disappeared and only bumping events were recorded. Suprisingly, addition of Mn(II) caused an increase in translocation events to about 64%. Thus, conformational changes to prions upon binding metal ions are readily observed by nanopore analysis.

The interaction of three proteins (histidine-containing phosphocarrier protein, HPr, calmodulin, CaM, and maltose binding protein, MBP) with synthetic silicon nitride (SiN(x)) membranes has been studied. The proteins which have a net negative charge were electrophoretically driven into pores of 7 and 5 nm diameter with a nominal length of 15 nm. The % blockade current and event duration were measured at three different voltages. For a translocation event it was expected that the % block would be constant with voltage whilst the event duration would decrease with increasing voltage. On the basis of these criteria, we deduce that MBP whose largest dimension is 6.5 nm does not translocate whereas up to 40% of CaM molecules can translocate the 7 nm pore as can a majority of HPr molecules, with some translocations being observed for the 5 nm pore. For translocation events the magnitude of the % blockade current is consistent with a folded conformation of the proteins surrounded by a hydration shell of 0.5-1.0 nm.

The interaction of two peptides with the α-hemolysin pore was studied in the presence of a MHz AC field. For an α-helical peptide the proportion of bumping events increased with increasing AC field whereas for a linear peptide with no dipole moment only small changes in the event profiles were observed.