Revealing the activation pathway for TMEM16A chloride channels from macroscopic currents and kinetic models Article uri icon

abstract

  • TMEM16A (ANO1), the pore-forming subunit of calcium-activated chloride channels, regulates several physiological and pathophysiological processes such as smooth muscle contraction, cardiac and neuronal excitability, salivary secretion, tumour growth and cancer progression. Gating of TMEM16A is complex because it involves the interplay between increases in intracellular calcium concentration ([Ca2 ]i), membrane depolarization, extracellular Cl− or permeant anions and intracellular protons. Our goal here was to understand how these variables regulate TMEM16A gating and to explain four observations. (a) TMEM16A is activated by voltage in the absence of intracellular Ca2 . (b) The Cl− conductance is decreased after reducing extracellular Cl− concentration ([Cl−]o). (c) ICl is regulated by physiological concentrations of [Cl−]o. (d) In cells dialyzed with 0.2 μM [Ca2 ]i, Cl− has a bimodal effect: at [Cl−]o <30 mM TMEM16A current activates with a monoexponential time course, but above 30 mM, [Cl−]o ICl activation displays fast and slow kinetics. To explain the contribution of Vm, Ca2 and Cl− to gating, we developed a 12-state Markov chain model. This model explains TMEM16A activation as a sequential, direct, and Vm-dependent binding of two Ca2 ions coupled to a Vm-dependent binding of an external Cl− ion, with Vm-dependent transitions between states. Our model predicts that extracellular Cl− does not alter the apparent Ca2 affinity of TMEM16A, which we corroborated experimentally. Rather, extracellular Cl− acts by stabilizing the open configuration induced by Ca2 and by contributing to the Vm dependence of activation. © 2016, Springer-Verlag Berlin Heidelberg.
  • TMEM16A (ANO1), the pore-forming subunit of calcium-activated chloride channels, regulates several physiological and pathophysiological processes such as smooth muscle contraction, cardiac and neuronal excitability, salivary secretion, tumour growth and cancer progression. Gating of TMEM16A is complex because it involves the interplay between increases in intracellular calcium concentration ([Ca2%2b]i), membrane depolarization, extracellular Cl− or permeant anions and intracellular protons. Our goal here was to understand how these variables regulate TMEM16A gating and to explain four observations. (a) TMEM16A is activated by voltage in the absence of intracellular Ca2%2b. (b) The Cl− conductance is decreased after reducing extracellular Cl− concentration ([Cl−]o). (c) ICl is regulated by physiological concentrations of [Cl−]o. (d) In cells dialyzed with 0.2 μM [Ca2%2b]i, Cl− has a bimodal effect: at [Cl−]o <30 mM TMEM16A current activates with a monoexponential time course, but above 30 mM, [Cl−]o ICl activation displays fast and slow kinetics. To explain the contribution of Vm, Ca2%2b and Cl− to gating, we developed a 12-state Markov chain model. This model explains TMEM16A activation as a sequential, direct, and Vm-dependent binding of two Ca2%2b ions coupled to a Vm-dependent binding of an external Cl− ion, with Vm-dependent transitions between states. Our model predicts that extracellular Cl− does not alter the apparent Ca2%2b affinity of TMEM16A, which we corroborated experimentally. Rather, extracellular Cl− acts by stabilizing the open configuration induced by Ca2%2b and by contributing to the Vm dependence of activation. © 2016, Springer-Verlag Berlin Heidelberg.

publication date

  • 2016-01-01