Abstract
The volume-sensitive chloride current (IClVol) exhibit a time-dependent decay presumably due to channel inactivation. In this work, we studied the effects of chloride ions (Cl−) and H+ ions on IClVol decay recorded in HEK-293 and HL-60 cells using the whole-cell patch clamp technique. Under control conditions ([Cl−]e = [Cl−]i = 140 mM and pHi = pHe = 7.3), IClVol in HEK cells shows a large decay at positive voltages but in HL-60 cells IClVol remained constant independently of time. In HEK-293 cells, simultaneously raising the [Cl−]e and [Cl−]i from 25 to 140 mM (with pHe = pHi = 7.3) increased the fraction of inactivated channels (FIC). This effect was reproduced by elevating [Cl−]i while keeping the [Cl−]e constant. Furthermore, a decrease in pHe from 7.3 to 5.5 accelerated current decay and increased FIC when [Cl−] was 140 mM but not 25 mM. In HL-60 cells, a slight IClVol decay was seen when the pHe was reduced from 7.3 to 5.5. Our data show that inactivation of IClVol can be controlled by changing either the Cl− or H+ concentration or both. Based on our results and previously published data, we have built a model that explains VRAC inactivation. In the model the H+ binding site is located outside the electrical field near the extracellular entry whilst the Cl− binding site is intracellular. The model depicts inactivation as a pore constriction that happens by simultaneous binding of H+ and Cl− ions to the channel followed by a voltage-dependent conformational change that ultimately causes inactivation.
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Acknowledgements
This work was supported by grants 79897, 59889, and 45895 (Consejo Nacional de Ciencia y Tecnologia, Mexico) and PO1-HL18208 (National Institutes of Health, USA). TRS and JADSC received a scholarship from Consejo Nacional de Ciencia y Tecnologia, Mexico.
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Supplemental Fig. 1
Hypothetical V m-dependence of volume-sensitive chloride channels. a Simple barrier model representing the energy landscape along the VRAC pore. This energy profile plus the kinetic model shown in Fig. 7 were used to qualitatively explain the V m (a) and external Cl−-dependence (b) of inactivation. The energy profiles depict the landscape along the pore that the permeant anions (with symmetrical [Cl−]i = [Cl−]e = 140 mM) experiment at −100, 0, and +100 mV. At each voltage, the pore occupancy changes and thus the probability that the pore is empty (P U) is greater at positive voltages. Moreover, P U changes as a function of the Cl− gradient across the membrane. b P U becomes larger as the Cl− gradient decreases. P U was calculated using the V m-dependent rate constants \( {\alpha_{\rm{V}}} = {\left[ {{\hbox{C}}{{\hbox{l}}^{-} }} \right]_{\rm{o}}} \times {k_1} + {\left[ {{\hbox{C}}{{\hbox{l}}^{-} }} \right]_{\rm{i}}} \times {k_{ - {2}}}\;{\hbox{and}}\;{\beta_{\rm{V}}} = {k_{ - {1} + }} \times {k_{ - {2}}} \) recorded in Table 2 (PPT 153 kb)
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Hernández-Carballo, C.Y., De Santiago-Castillo, J.A., Rosales-Saavedra, T. et al. Control of volume-sensitive chloride channel inactivation by the coupled action of intracellular chloride and extracellular protons. Pflugers Arch - Eur J Physiol 460, 633–644 (2010). https://doi.org/10.1007/s00424-010-0842-0
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DOI: https://doi.org/10.1007/s00424-010-0842-0