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| Many channels display subconductance levels: | |||||||
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This suggests a strong coupling between 'gating' and permeation : "The permeability structure is dynamic and forms the structural basis for the open/close mechanism" ( VanDongen, 1992 page 438). We have studied these 'sublevels' in the K channel Kv2.1 (drk1): Chapman et al 1997, 2001, 2005, 2006. The results obtained prompted us to propose that the selectivity filter is the gate The main reasons supporting this idea are outlined below: |
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| Structure of the KcsA selectivity filter : | |||||||
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Only 2 of the 4 subunits are shown. The filter contains 2 K ions (purple) and a water molecule (oxygen molecule in red). Each fully dehydrated K ion is coordinated by 8 carbonyl oxygens derived from the peptide backbone, creating two K binding sites. Electrostatic repulsion between the 2 bound K ions is reduced significantly due to the partial negative charges of the carbonyl oxygens and presence of the intervening water molecule. As a result, the two binding sites may have a relatively high affinity for K ions. At physiological temperature, the optimal coordination chemistry of the oxygen cage may degrade due to thermal movement of the backbone. This can significantly decrease affinity and allow the bound K ions to dissociate. The idea that affinity for K ions can vary dramatically due to small alterations of the filter conformation leads us to propose a specific mechanism by which the filter can function as a gate: |
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In this paradigm, the selectivity filter exists in one of two 2 affinity states:
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Monte Carlo simulations of an affinity-switching selectivity filter | ||||||
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| Channel Gating and Affinity Switching. | |||||||
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| A short segment of a single channel recording is shown in which the channel visits the open state twice. The bar above the current trace indicates the behavior of the selectivity filter, which is either locked in the high-affinity state H (filled bars), or it stochastically alternates between the high (H)- and low (L)-affinity states (open bars). Bottom panel: The diagram shows the behavior of the filter during an open interval at an expanded time scale: even when the channel is fully open, the filter spends most of its time in the high-affinity state. | |||||||