During sustained depolarization, voltage-gated Ca2+ channels progressively undergo a transition to a nonconducting, inactivated state, preventing Ca2+ overload of the cell. This transition can be triggered either by the membrane potential (voltage-dependent inactivation) or by the consecutive entry of Ca2+(Ca2+-dependent inactivation), depending on the type of Ca2+ channel. These two types of inactivation are suspected to arise from distinct underlying mechanisms, relying on specific molecular sequences of the different pore-forming Ca2+ channel subunits. Here we report that the voltage-dependent inactivation (of the α1ACa2+ channel) and the Ca2+-dependent inactivation (of the α1C Ca2+ channel) are similarly influenced by Ca2+ channel β subunits. The same molecular determinants of the β subunit, and therefore the same subunit interactions, influence both types of inactivation. These results strongly suggest that the voltage and the Ca2+-dependent transitions leading to channel inactivation use homologous structures of the different α1 subunits and occur through the same molecular process. A model of inactivation taking into account these new data is presented.
14 April 2014 in American Journal of Transplantation
The administration of autologous (recipient‐derived) tolerogenic dendritic cells (ATDCs) is under clinical evaluation. However, the molecular mechanisms by which these cells prolong graft survival in a donor‐specific manner is unknown. Here, we tested mouse ATDCs for their therapeutic potential in a skin transplantation model. ATDC injection in combination with anti‐CD3 treatment induced the accumulation of CD8+CD11c+ T cells and significantly prolonged allograft survival. TMEM176B is an intracellular protein expressed in ATDCs and initially identified in allograft tolerance. We show that Tmem176b−/− ATDCs completely failed to trigger both phenomena but recovered their effect when loaded with donor peptides before injection. These results strongly suggested that ATDCs require TMEM176B to cross‐present antigens in a tolerogenic fashion. In agreement with this, Tmem176b−/− ATDCs specifically failed to cross‐present male antigens or ovalbumin to CD8+ T cells. Finally, we observed that a Tmem176b‐dependent cation current controls phagosomal pH, a critical parameter in cross‐presentation. Thus, ATDCs require TMEM176B to cross‐present donor antigens to induce donor‐specific CD8+CD11c+ T cells with regulatory properties and prolong graft survival.
1 The effects of zinc (Zn2+) on excitability and ionic conductances were analysed on RINm5F insulinoma cells under whole-cell and outside-out patch-clamp recording conditions. 2 We found that extracellular application of 10-20 μM Zn2+ induced a reversible abolition of Ca2+ action potential firing, which was accompanied by an hyperpolarisation of the resting membrane potential. 3 Higher concentrations of Zn2+, in the tens to hundreds micromolar range, induced a reversible reduction of voltage-gated Ca2+ and, to a lesser extent, K+ currents. Low-voltage-activated Ca2+ currents were more sensitive to Zn2+ block than high voltage-activated Ca2+ currents. 4 The Zn2+-induced hyperpolarisation arose from a dose-dependent increase in a voltage-independent K+ conductance that was pharmacologically identified as an ATP-sensitive K+ (KATP) conductance. The effect was rapid in onset, readily reversible, voltage independent, and related to intracellular ATP concentration. In the presence of 1 mM intracellular ATP, half-maximal activation of KATP channels was obtained with extracellular application of 1.7 μM Zn2+. 5 Single channel analysis revealed that extracellular Zn2+ increased the KATP channel open-state probability with no change in the single channel conductance. 6 Our data support the hypothesis that Zn2+ binding to KATP protein subunits results in an activation of the channels, therefore regulating the resting membrane potential and decreasing the excitability of RINm5F cells. Taken together, our results suggest that Zn2+ can influence insulin secretion in pancreatic β-cells through a negative feedback loop, involving both KATP and voltage-gated conductances.