Key result
KVbeta1.2 negatively shifts KV1.2 current activation via progressive open channel block at depolarized potentials.
Why the study?
The mechanisms underlying the effects of K(V)beta1.2 subunits on K(V)1.2 channel activation, deactivation, and inactivation were not known.
The study elucidates the structural and functional interactions between KVbeta1.2 and KV1.2 channels, explaining the mechanisms behind the negative shift in activation and slowed deactivation.
Cytosolic K(V)beta1 subunits co-assemble with transmembrane K(V)1 channel alpha-subunits and have complex effects on channel function. Fast inactivation, the most obvious effect conferred, is due to fast open channel block resulting from the binding of the N-terminus within the inner mouth of the pore. K(V)beta1 subunits also slow current deactivation, enhance slow inactivation and shift channel activation to more negative voltages, but the mechanisms underlying these actions are not known. Here we use voltage clamp fluorimetry at sites near the extracellular end of the S4 helix, the channel's primary voltage sensor, in combination with voltage clamp electrophysiology, to independently track the movement of the S4 helix along with ionic current, and thus identify the structural and mechanistic means by which the K(V)beta1.2 subunit confers its actions on the K(V)1.2 channel. We show that the negative shift in current activation is not due to direct actions of K(V)beta1.2 on the S4 segment. Instead, this shift results from an apparent saturation of channel activation at depolarized potentials as the extent of open channel block by the K(V)beta1.2 N-terminus progressively increases. The return of fluorescence to baseline is slowed along with current deactivation. According to our data, this is due to an inability of the activation gate to close while the K(V)beta1.2 N-terminus occupies the pore and strong coupling of the gate with the S4 segment. Together with data from previous studies, our findings provide a complete and coherent picture of the functional and structural interactions between K(V)beta1.2 and K(V)1.2.
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Peters et al. (2009) studied this question. KVbeta1.2 subunit was evaluated on Structural and mechanistic means by which KVbeta1.2 confers actions on KV1.2. The negative shift in current activation caused by KVbeta1.2 is due to an apparent saturation of channel activation at depolarized potentials as open channel block progressively increases.
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