Effect of nifedipine on the ion channels formed by α1 subunits of the cardiac and vascular muscle L-type Ca channels

We investigated the voltage dependence of nifedipine sensitivity of the ion channels formed by α₁ subunits of the cardiac and smooth muscles (CM and SM, respectively) L-type Ca²⁺ channels stably expressed in Chinese hamster ovary (CHO) cells. Equilibrium inhibition of the α₁ subunits, directing Ba²⁺ current (I _α1), by different concentrations of nifedipine was measured at the holding potentials (V _h ) of −100 mV and −50 mV. AtV _h =−100 mV, the SM α₁ subunit was found to be 6-fold more sensitive for nifedipine than the subunit (K ₋₁₀₀=8.3 and 50.4 nM, respectively). Depolarization to −50 mV resulted in about sevenfold increase in the nifedipine potency for both subunits (K ₋₅₀=1.25 and 6.95 nM, respectively). The voltage dependence of steady-state inactivation could be fitted by a sum of two Boltzmann’s equations with slope factors of about 12 and 5 mV. The midpoints of both components in the CM α₁ subunit (−75.6 and −42.8 mV) were more negative than those in the SM subunit (−63.7 and −37.7 mV). The relative contribution of the less sloped component in the control was rather low, being less pronounced in the CM (0.15) than in the SM (0.34) subunits. Nifedipine shifted the midpoints of inactivation curves to more negative potentials. The shift was more pronounced for the SM α₁ subunit (−24.8 mV compared with −11.8 mV for the CM subunit in the presence of 10 nM nifedipine). Nifedipine differentially affected the two Boltzmann components of inactivation curves, more effectively inhibiting the steeper component. In the presence of 10 nM nifedipine, this component completely disappeared in the SM subunit, while its relative contribution in the CM subunit decreased from 0.85 to 0. 57, resulting in an apparent decrease in the steepness. These results are inconsistent with the receptor modulated hypothesis and suggest the existence of two mechanisms of inactivation characterized by different voltage dependence.     

Individual optimization: Mechanisms shaping the optimal reaction norm

In general, optimal reaction norms in heterogeneous populations can be obtained only by iterative numerical procedures (McNamara, 1991; Kawecki and Stearns, 1993). We consider two particular, but biologically plausible and analytically tractable cases of individual optimization to gain insight into the mechanisms which shape the optimal reaction norm of fecundity in relation to an environmental variable or an individual trait. In the first case, we assume that the quality of the environment (e.g. food abundance) or the quality of the individual (e.g. body size) is fixed during its entire life; it may also be a heritable individual trait. In the second case, individual quality is assumed to change randomly such that the probability distribution of quality in the next year is the same for the parent and for her offspring. For these two cases, we obtain analytical expressions for the shape of the optimal reaction norm, which are heuristically interpretable in terms of underlying selective mechanisms. It is shown that better quality may reduce the optimal fecundity. This outcome is particularly likely if better quality increases a fecundity-independent factor of parental survival in a long-lived species with fixed quality. This revised version was published online in July 2006 with corrections to the Cover Date.     

Extremely slow inactivation of the ion channels formed by transfected α2 of L-type Ca2+ channelsof L-type Ca2+ channels

Barium currents through ion channels formed by α1-subunit of L-type Ca²⁺ channel (I _α1) were recorded from cultured chinese hamster ovary (CHO) cells. The cells were stably transfected with either a cardiac or a smooth muscle (SM) variant of α1-subunit. TheI _α1 in both cases exhibited similar fast voltage-dependent activation kinetics and slow apparent inactivation kinetics. With 10 mM Ba²⁺ in the bath solution,I _α1 was activated at potentials more positive than −40 mV, peaked between 0 and +10 mV, and reversed at about +50 mV. In addition to slow apparent inactivation of inward current, both subunits provided an extremely slow voltage-dependent inactivation at potentials more positive than −100 mV, with half-maximum inactivation at −43.4 mV for cardiac and −41.4 mV for SM α1-subunits. The onset of inactivation as well as recovery from this process were within a time range of minutes. The voltage dependence of steady-state inactivation could be fitted by the sum of two Boltzmann's equations with slope factors of about 12 mV and 5 mV. A less sloped component has its midpoints at −75.6 and −63.7 mV, and a steeper component has its midpoints at −42.8 and −37.7 mV for cardiac and SM α1-subunits, respectively. Relative contribution of the steeper component was higher in both subunits (0.86 and 0.66 for cardiac and SM subunits, respectively). For comparison, the inactivation curves for 5-sec-long conditioning prepulses could be fitted by single Boltzmann's distribution with a 20 mV more positive midpoint and a slope factor of about 13 mV. In contrast to the steady-state inactivation curves, they showed considerable overlap with the steady-state activation curve. Our results reflect functional consequences of known sequence differences between α1-subunits of the cardiac and SM L-type Ca²⁺ channels and could be used in structural modeling of Ca²⁺ channel gating. In addition, they show that depolarization-induced window current has a transient nature and decays with the development of extremely slow inactivation. This is the first demonstration that slow inactivation of the L-type Ca²⁺ channel is an intrinsic property of its α1-subunits.