We discussed both the forward and
reverse mechanisms of the F1F0 ATP synthase – i.e., both ATP synthesis and
generation of rotary motion from ATP hydrolysis although limited to the F1
domain. (Previously, Michael Grabe led
our discussion of the F0 domain.) Our
discussion was based on the schematic model depicted in Berg’s textbook (http://www.ncbi.nlm.nih.gov/books/NBK22388/figure/A2538/). While the schematic did provide a lot of
qualitative insight, I think most of us felt unsatisfied with the attempt to
understand a machine without at least a semi-quantitative basis. Specifically, we know there are
thermodynamically constrained relations among the various rates (for catalysis,
binding, and conformational change) that would provide a much more concrete
picture. We will attempt to pursue this
approach next time.
Some questions raised that we
would like to address:
- What is the importance of the three-fold symmetry? Would two sub-units be enough? An initial answer is that only with three subunits can the directionality be ensured in the hydrolysis process.
- What is the minimal kinetic model that can explain ATP synthesis using mechanical force? Are two subunits sufficient?
- What is the minimal kinetic model need for rotary motion?
- What insights can thermodynamically consistent kinetic models provide?
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