Aman, T. K. | Search bioRxiv

bioRxiv2021

NONCANONICAL ELECTROMECHANICAL COUPLING MECHANISM OF AN HCN CHANNEL

Pacemaker hyperpolarization-activated cyclic nucleotide-gated (HCN) ion channels exhibit a reversed voltage-dependent gating, activating by membrane hyperpolarization instead of depolarization. Sea urchin HCN (spHCN) channels also undergo an inactivation with hyperpolarization which occurs only in the absence of cyclic nucleotide. Here we applied transition metal ion FRET and Rosetta modeling to measure differences in the structural rearrangements between activation and inactivation of spHCN channels. We found that removal of cAMP produced a largely rigid-body rotation of the C-linker relative to transmembrane domain, bringing the A helix in close proximity to the voltage-sensing S4 helix. In addition, rotation of the C-linker was elicited by hyperpolarization in the absence but not in the presence of cAMP. These results suggest the A helix functions like a mechanical clutch to engage inactivation. cAMP binding disengages the clutch, permitting the hyperpolarization-dependent activation mediated by the S5 helix. Furthermore, rearrangement of A helix during recovery from inactivation of spHCN channels was similar to that for the activation of KCNH channels, suggesting a conserved mechanism for this noncanonical electromechanical coupling in the CNBD channel family.

biophysics↗

bioRxiv2019

The HCN Channel Voltage Sensor Undergoes A Large Downward Motion During Hyperpolarization

Voltage-gated ion channels (VGICs) underlie almost all electrical signaling in the body1. They change their open probability in response to changes in transmembrane voltage, allowing permeant ions to flow across the cell membrane. Ion flow through VGICs underlies numerous physiological processes in excitable cells1. In particular, hyperpolarization-activated cyclic nucleotide-gated (HCN) channels, which operate at the threshold of excitability, are essential for pacemaking activity, resting membrane potential, and synaptic integration2. VGICs contain a series of positively-charged residues that are displaced in response to changes in transmembrane voltage, resulting in a conformational change that opens the pore3-6. These voltage-sensing charges, which reside in the S4 transmembrane helix of the voltage-sensor domain (VSD)3 and within the membranes electric field, are thought to move towards the inside of the cell (downwards) during membrane hyperpolarization7. HCN channels are unique among VGICs because their open probability is increased by membrane hyperpolarization rather than depolarization8-10. The mechanism underlying this \"reverse gating\" is still unclear. Moreover, although many X-ray crystal and cryo-EM structures have been solved for the depolarized state of the VSD, including that of HCN channels11, no structures have been solved at hyperpolarized voltages. Here we measure the precise movement of the charged S4 helix of an HCN channel using transition metal ion fluorescence resonance energy transfer (tmFRET). We show that the S4 undergoes a significant (~10 [A]) downward movement in response to membrane hyperpolarization. Furthermore, by applying constraints determined from tmFRET experiments to Rosetta modeling, we reveal that the carboxyl-terminal part of the S4 helix exhibits an unexpected tilting motion during hyperpolarization activation. These data provide a long-sought glimpse of the hyperpolarized state of a functioning VSD and also a framework for understanding the dynamics of reverse gating in HCN channels. Our methods can be broadly applied to probe short-distance rearrangements in other ion channels and membrane proteins.

biophysics↗