Relevance of the alternate conductance states of anthrax toxin channel

In their recent article in PNAS, Das and Krantz (1) attempt to relate the previously described (2, 3) alternate conductance substate of the anthrax toxin protective antigen (PA₆₃) channel to the allosteric helix compression model (4). Although we do not intend to discuss the differences between this model and the extended-chain Brownian ratchet model (5), we believe that there are two experimental observations that should be specifically addressed.

First, the authors hypothesize that the observed small-conductance substate (2, 3) is related to the two states of the PA₆₃ channel, one clamped empty state and one unclamped empty dilated state, with the dilation occurring at the ϕ-clamp (1). Although this interpretation could be relevant, we believe the arguments provided to support it are indirect. In addition to analyzing the so-called long-lived and short-lived closures induced by the lethal factor (LF) peptides, the authors could have also performed a direct statistical comparison of these closures when the channel is in one of the two conductance states.

Second, the authors attribute the fast-flickering closures of PA₆₃, that were previously characterized as a voltage-independent (2) 1/f-noise process (3), to the interaction of “a contaminant small molecule, buffer ion, or peptide” that “momentarily binds and occupies the ϕ-clamp” (1). To support this statement, the authors cite two articles (2, 6) where cationic compounds were shown to reversibly block the channel. We tested the “contaminant” hypothesis performing single PA₆₃ recordings in two different solutions: 1 M 99.0% pure KCl prepared using Milli-Q water and 1 M 99.99995% pure KCl prepared using deionized HPLC-grade water. The power spectral density analysis of PA₆₃ current fluctuations showed no statistically significant difference between these solutions (Fig. 1A). To rule out the possibility of contaminants resulting from protein or lipid addition, we made the measurements while gradually replacing the bathing KCl solutions with fresh KCl; however, no decrease in the density of the current power spectra was detected (Fig. 1B).

• Download figure
• Open in new tab
• Download powerpoint

Fig. 1.

(A) Power spectral densities of single PA₆₃ channel current fluctuations (1-ms resolution inserts) in 1 M 99.0% pure (purple, green, and red spectra) and 99.99995% pure (black spectrum) KCl solutions. The measurements in 99.0% KCl were taken in the same membrane bathing solution on single PA₆₃ channels incorporated into three consecutively formed diphytanoyl phosphatidylcholine bilayer membranes at 50 mV of applied voltage, pH 6. At frequencies <500 Hz, a power spectrum of PA₆₃ current fluctuations taken in the 1 M 99.99995% pure KCl/HPLC-grade water solution is within the limits of the spectral density fluctuations of individual measurements taken in the 1 M 99.0% pure KCl/type I Milli-Q water solution. (B) Power spectral density of current fluctuations through a single PA₆₃ channel formed in 1 M 99.99995% pure KCl solution (black spectrum). No statistically significant difference in spectral density was observed when 15% (magenta spectrum), 30% (orange spectrum), and 60% (blue spectrum) of the starting solution were replaced with fresh 1 M 99.99995% pure KCl. In all solutions, PA₆₃ displays expressed 1/f-noise behavior (fitted by a straight red line in B).

The idea that the anthrax toxin channel structural dynamics can be directly studied on a single-channel level is intriguing. However, consistency in the interpretation of the reported data (1⇓–3) is essential. Unfortunately, the authors (1) do not mention the fact that the heptameric PA₆₃ was also reported to insert directly in the higher conductance substate, switching to the lower conductance state only on occasion (3). Moreover, 7+β-cyclodextrins were shown to reversibly block both types of PA₆₃ insertions with statistically indistinguishable rate constants (3). The authors report that the difference between the conductance states was threefold greater for the F427A mutant (1), but do not mention that the probability of finding PA₆₃ in the “clamped empty state” was higher in phosphatidylserine compared with phosphatidylcholine membranes, with the substate amplitude being close to 30% of PA₆₃ conductance (3).

In addition, 1/f current fluctuations, but not the conductance substates, were reported for channel-forming components of the binary clostridial C2 and iota toxins by Benz et al. (7, 8). These three channels share a high level of amino acid homology and numerous functional similarities related to the intracellular translocation of the enzymatic factors of these toxins.