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editorial
. 2013 Jun 18;104(12):2778–2779. doi: 10.1016/j.bpj.2013.05.019

On Phosphate Release in Actin Filaments

Antoine Jégou †,, Thomas Niedermayer ‡,, Reinhard Lipowsky , Marie-France Carlier , Guillaume Romet-Lemonne †,
PMCID: PMC3686342  PMID: 23790388

In their article recently published in the Biophysical Journal, Burnett and Carlsson (1) present a theoretical analysis of experimental data that we have previously published and analyzed (2). Our work provided evidence for a random mechanism of inorganic phosphate (Pi) release subsequent to chemical cleavage of ATP on individual actin filaments. Burnett and Carlsson examine the alternative possibility of cooperativity during Pi release in actin filaments. We find that the presentation of our work by Burnett and Carlsson is misleading or incorrect in several instances, and wish to clarify the following points.

In our article, depolymerization traces of individual filaments were measured, and each individual curve was fitted to investigate the possibility of different Pi release mechanisms. For the sake of comparison with Burnett and Carlsson (1), we focus here on direct fits of depolymerization traces, which are detailed in the Supporting Material of our article, but the same conclusions are drawn when fitting the inverse of the depolymerization velocity, as we have done in the main text (2). The best fits were obtained for a random Pi release model, and the release rates were found to be similar, but not identical (due to experimental noise) for each curve, with an average value of rd = 0.0074 s−1 (0.0068 s−1 with the inverse depolymerization velocity method). Our experimental data used by Burnett and Carlsson (1) consists of the depolymerization trace of one single individual filament, which they have extracted from Fig. 2 B of Jégou et al. (2). When comparing this individual depolymerization trace with traces computed for a random Pi release, Burnett and Carlsson use the average rate constant of rd = 0.0074 s−1 and the resulting curves do not agree well with the data (Fig. 6 D of Burnett and Carlsson (1)). However, this is not a fit of this data. Our fit of this individual trace results in rd = 0.0045 s−1 (or rd = 0.0043 s−1, as stated in the caption of Fig. 2 of Jégou et al. (2), using the inverse depolymerization velocity method), and the quality of this fit is very good, with Δ2 = 1.2 · 10−2 μm2, better in fact than the best fits with cooperativity shown in the inset of Fig. 6 (1).

Measuring the depolymerization traces of individual filaments, as we have done, allows one to look for details that would disappear when curves are averaged. As can be seen in Fig. 6 D of Burnett and Carlsson (1), for a random Pi release there is little difference between individual curves, and it therefore makes sense to compare individual experimental traces to an average theoretical curve. In contrast, for the cooperative model, as shown in Fig. 6 C of Burnett and Carlsson (1), each individual filament displays its own sharp transitions between ADP and ADP-Pi domains, which are smoothed out when averaging several traces. Comparing an individual experimental trace to an average theoretical curve, as done by Burnett and Carlsson—“the average trajectory (…) provides a good fit to the data, as shown in Fig. 6 C” (1)—makes no sense in this case. To argue in favor of cooperativity, Burnett and Carlsson should have demonstrated that sample filament traces (blue curves in Fig. 6 C of Burnett and Carlsson (1)), and not the mean filament time-course (red curve in Fig. 6 C), provide a good fit to our single filament data (black dots in Fig. 6 C).

As suggested by Burnett and Carlsson, comparing the depolymerization traces of filaments elongated at different rates (i.e., using different actin concentrations) is a good way to test whether Pi release is a purely random mechanism or involves cooperativity (Fig. 7 of Burnett and Carlsson (1)). The authors write: “Thus, repeating the experiment of Jégou et al. with varying G should provide additional constraints on the cooperativity.” Our article, however, seems to have been overlooked here too, because this experiment has actually been performed and reported as follows in Jégou et al. (2): “Filaments elongated at different actin concentrations, i.e. different velocities, or for different durations all displayed the same age-dependence of depolymerization rate (Figure 2 F), confirming that the ADP-Pi content depends only on the age of the F-actin, as expected for a random Pi release mechanism.” Further in the article (2), we show (see Fig. 4 E) examples of ADP-Pi profiles obtained with a 10-fold difference in actin concentrations. Experiments over a broader range of actin concentrations might reveal some cooperativity, but our data is in better agreement with a random Phosphate release mechanism than with a vectorial or highly cooperative mechanism.

References

  • 1.Burnett M.M., Carlsson A.E. Quantitative analysis of approaches to measure cooperative phosphate release in polymerized actin. Biophys. J. 2012;103:2369–2378. doi: 10.1016/j.bpj.2012.10.032. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 2.Jégou A., Niedermayer T., Romet-Lemonne G. Individual actin filaments in a microfluidic flow reveal the mechanism of ATP hydrolysis and give insight into the properties of profilin. PLoS Biol. 2011;9:e1001161. doi: 10.1371/journal.pbio.1001161. [DOI] [PMC free article] [PubMed] [Google Scholar]

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