Membrane depolarization, neurotransmitters, and hormones evoke a release of Ca2+ from intracellular Ca(2+)-storing organelles like the endoplasmic reticulum and, in muscle, the sarcoplasmic reticulum (SR). In turn, the released Ca2+ serves to trigger a variety of cellular responses. The presence of Ca2+ pumps to replenish intracellular stores was described more than 20 years ago. The presence of Ca2+ channels, like the ryanodine receptor, which suddenly release the organelle-stored Ca2+, is a more recent finding. This review describes the progress made in the last five years on the structure, function, and regulation of the ryanodine receptor. Numerous reports have described the response of ryanodine receptors to cellular ions and metabolites, kinases and other proteins, and pharmacological agents. In many cases, comparative measurements have been made using Ca2+ fluxes in SR vesicles, single-channel recordings in planar bilayers, and radioligand binding assays using [3H]ryanodine. These techniques have helped to relate the activity of single ryanodine receptors to global changes in the SR Ca2+ permeability. Molecular information on functional domains within the primary structure of the ryanodine receptor is also available. There are at least three ryanodine receptor isoforms in various tissues. Some cells, such as amphibian muscle cells, express more than a single isoform. The diversity of ligands known to modulate gating and the diversity of tissues known to express the protein suggest that the ryanodine receptor has the potential to participate in many types of cell stimulus-Ca(2+)-release coupling mechanisms.

The multisubunit (␣ 1S , ␣ 2 ͞␦, ␤ 1 , and ␥) skeletal muscle dihydropyridine receptor transduces transverse tubule membrane depolarization into release of Ca 2؉ from the sarcoplasmic reticulum, and also acts as an L-type Ca 2؉ channel. The ␣ 1S subunit contains the voltage sensor and channel pore, the kinetics of which are modified by the other subunits. To determine the role of the ␤ 1 subunit in channel activity and excitation-contraction coupling we have used gene targeting to inactivate the ␤ 1 gene. ␤ 1 -null mice die at birth from asphyxia. Electrical stimulation of ␤ 1 -null muscle fails to induce twitches, however, contractures are induced by caffeine. In isolated ␤ 1 -null myotubes, action potentials are normal, but fail to elicit a Ca 2؉ transient. L-type Ca 2؉ current is decreased 10-to 20-fold in the ␤ 1 -null cells compared with littermate controls. Immunohistochemistry of cultured myotubes shows that not only is the ␤ 1 subunit absent, but the amount of ␣ 1S in the membrane also is undetectable. In contrast, the ␤ 1 subunit is localized appropriately in dysgenic, mdg͞mdg, (␣ 1S -null) cells. Therefore, the ␤ 1 subunit may not only play an important role in the transport͞insertion of the ␣ 1S subunit into the membrane, but may be vital for the targeting of the muscle dihydropyridine receptor complex to the transverse tubule͞sarcoplasmic reticulum junction.

In different types of K+ channels the primary activation gate is thought to reside near the intracellular entrance to the ion conduction pore. In the Shaker Kv channel the gate is closed at negative membrane voltages, but can be opened with membrane depolarization. In a previous study of the S6 activation gate in Shaker (Hackos, D.H., T.H. Chang, and K.J. Swartz. 2002. J. Gen. Physiol. 119:521–532.), we found that mutation of Pro 475 to Asp results in a channel that displays a large macroscopic conductance at negative membrane voltages, with only small increases in conductance with membrane depolarization. In the present study we explore the mechanism underlying this constitutively conducting phenotype using both macroscopic and single-channel recordings, and probes that interact with the voltage sensors or the intracellular entrance to the ion conduction pore. Our results suggest that constitutive conduction results from a dramatic perturbation of the closed-open equilibrium, enabling opening of the activation gate without voltage-sensor activation. This mechanism is discussed in the context of allosteric models for activation of Kv channels and what is known about the structure of this critical region in K+ channels.

The primary activation gate in K+ channels is thought to reside near the intracellular entrance to the ion conduction pore. In a previous study of the S6 activation gate in Shaker (Hackos et al., 2002), we found that mutation of V478 to W results in a channel that cannot conduct ions even though the voltage sensors are competent to translocate gating charge in response to membrane depolarization. In the present study we explore the mechanism underlying the nonconducting phenotype in V478W and compare it to that of W434F, a mutation located in an extracellular region of the pore that is nonconducting because the channel is predominantly found in an inactivated state. We began by examining whether the intracellular gate moves using probes that interact with the intracellular pore and by studying the inactivation properties of heterodimeric channels that are competent to conduct ions. The results of these experiments support distinct mechanisms underlying nonconduction in W434F and V478W, suggesting that the gate in V478W either remains closed, or that the mutation has created a large barrier to ion permeation in the open state. Single channel recordings for heterodimeric and double mutant constructs in which ion conduction is rescued suggest that the V478W mutation does not dramatically alter unitary conductance. Taken together, our results suggest that the V478W mutation causes a profound shift of the closed to open equilibrium toward the closed state. This mechanism is discussed in the context of the structure of this critical region in K+ channels.

The Ca2+ currents, charge movements, and intracellular Ca2+ transients of mouse dihydropyridine receptor (DHPR) beta 1-null myotubes expressing a mouse DHPR beta 1 cDNA have been characterized. In beta 1-null myotubes maintained in culture for 10-15 days, the density of the L-type current was approximately 7-fold lower than in normal cells of the same age (Imax was 0.65 +/- 0.05 pA/pF in mutant versus 4.5 +/- 0.8 pA/pF in normal), activation of the L-type current was significantly faster (tau activation at +40 mV was 28 +/- 7 ms in mutant versus 57 +/- 8 ms in normal), charge movements were approximately 2.5-fold lower (Qmax was 2.5 +/- 0.2 nC/microF in mutant versus 6.3 +/- 0.7 nC/microF in normal), Ca2+ transients were not elicited by depolarization, and spontaneous or evoked contractions were absent. Transfection of beta 1-null cells by lipofection with beta 1 cDNA reestablished spontaneous or evoked contractions in approximately 10% of cells after 6 days and approximately 30% of cells after 13 days. In contracting beta 1-transfected myotubes there was a complete recovery of the L-type current density (Imax was 4 +/- 0.9 pA/pF), the kinetics of activation (tau activation at +40 mV was 64 +/- 5 ms), the magnitude of charge movements (Qmax was 6.7 +/- 0.4 nC/microF), and the amplitude and voltage dependence of Ca2+ transients evoked by depolarizations. Ca2+ transients of transfected cells were unaltered by the removal of external Ca2+ or by the block of the L-type Ca2+ current, demonstrating that a skeletal-type excitation-contraction coupling was restored. The recovery of the normal skeletal muscle phenotype in beta 1-transfected beta-null myotubes shows that the beta 1 subunit is essential for the functional expression of the DHPR complex.

The dihydropyridine receptor (DHPR) of skeletal muscle functions as a Ca2+ channel and is required for excitation-contraction (EC) coupling. Here we show that the DHPR beta subunit is involved in the regulation of these two functions. Experiments were performed in skeletal mouse myotubes selectively lacking a functional DHPR beta subunit. These beta-null cells have a low-density L-type current, a low density of charge movements, and lack EC coupling. Transfection of beta-null cells with cDNAs encoding for either the homologous beta1a subunit or the cardiac- and brain-specific beta2a subunit fully restored the L-type Ca2+ current (161 +/- 17 pS/pF and 139 +/- 9 pS/pF, respectively, in 10 mM Ca2+). We compared the Boltzmann parameters of the Ca2+ conductance restored by beta1a and beta2a, the kinetics of activation of the Ca2+ current, and the single channel parameters estimated by ensemble variance analysis and found them to be indistinguishable. In contrast, the maximum density of charge movements in cells expressing beta2a was significantly lower than in cells expressing beta1a (2.7 +/- 0.2 nC/microF and 6.7 +/- 0. 4 nC/microF, respectively). Furthermore, the amplitude of Ca2+ transient measured by confocal line-scans of fluo-3 fluorescence in voltage-clamped cells were 3- to 5-fold lower in myotubes expressing beta2a. In summary, DHPR complexes that included beta2a or beta1a restored L-type Ca2+ channels. However, a DHPR complex with beta1a was required for complete restoration of charge movements and skeletal-type EC coupling. These results suggest that the beta1a subunit participates in key regulatory events required for the EC coupling function of the DHPR.

The origin of Ibetanull, the Ca2+ current of myotubes from mice lacking the skeletal dihydropyridine receptor (DHPR) beta1a subunit, was investigated. The density of Ibetanull was similar to that of Idys, the Ca2+ current of myotubes from dysgenic mice lacking the skeletal DHPR alpha1S subunit (-0.6 +/- 0.1 and -0.7 +/- 0.1 pA/pF, respectively). However, Ibetanull activated at significantly more positive potentials. The midpoints of the GCa-V curves were 16.3 +/- 1.1 mV and 11.7 +/- 1.0 mV for Ibetanull and Idys, respectively. Ibetanull activated significantly more slowly than Idys. At +30 mV, the activation time constant for Ibetanull was 26 +/- 3 ms, and that for Idys was 7 +/- 1 ms. The unitary current of normal L-type and beta1-null Ca2+ channels estimated from the mean variance relationship at +20 mV in 10 mM external Ca2+ was 22 +/- 4 fA and 43 +/- 7 fA, respectively. Both values were significantly smaller than the single-channel current estimated for dysgenic Ca2+ channels, which was 84 +/- 9 fA under the same conditions. Ibetanull and Idys have different gating and permeation characteristics, suggesting that the bulk of the DHPR alpha1 subunits underlying these currents are different. Ibetanull is suggested to originate primarily from Ca2+ channels with a DHPR alpha1S subunit. Dysgenic Ca2+ channels may be a minor component of this current. The expression of DHPR alpha1S in beta1-null myotubes and its absence in dysgenic myotubes was confirmed by immunofluorescence labeling of cells.

We investigated the effect of Cl- on the Ca2+ permeability of rabbit skeletal muscle junctional sarcoplasmic reticulum (SR) using 45Ca2+ fluxes and single channel recordings. In 45Ca2+ efflux experiments, the lumen of the SR was passively loaded with solutions of 150 mM univalent salt containing 5 mM 45Ca2+. Release of 45Ca2+ was measured by rapid filtration in the presence of extravesicular 0.4-0.8 microM free Ca2+ and 150 mM of the same univalent salt loaded into the SR lumen. The rate of release was 5-10 times higher when the univalent salt equilibrated across the SR-contained Cl- (Tris-Cl, choline-Cl, KCl) instead of an organic anion or other halides (gluconate-, methanesulfonate-, acetate-, HEPES-, Br-, I-). Cations (K+, Tris+) could be interchanged without a significant effect on the release rate. To determine whether Cl- stimulated ryanodine receptors, we measured the stimulation of release by ATP (5 mM total) and caffeine (20 mM total) and the inhibition by Mg2+ (0.8 mM estimated free) in Cl(-)-free and Cl(-)-containing solutions. The effects of ATP, caffeine, and Mg2+ were the largest in K-gluconate and Tris-gluconate, intermediate in KCl, and notably poor or absent in choline-Cl and Tris-Cl. Procaine (10 mM) inhibited the caffeine-stimulated release measured in K-gluconate, whereas the Cl- channel blocker clofibric acid (10 mM) but not procaine inhibited the caffeine-insensitive release measured in choline-Cl. Ruthenium red (20 microM) inhibited release in all solutions. In SR fused to planar bilayers we identified a nonselective Cl- channel (PCl: PTris: PCa = 1:0.5:0.3) blocked by ruthenium red and clofibric acid but not by procaine. These conductive and pharmacological properties suggested the channel was likely to mediate Cl(-)-dependent SR Ca2+ release. The absence of a contribution of ryanodine receptors to the Cl(-)-dependent release were indicated by the lack of an effect of Cl- on the open probability of this channel, a complete block by procaine, and a stimulation rather than inhibition by clofibric acid. A plug model of Cl(-)-dependent release, whereby Cl- removed the inhibition of the nonselective channel by large anions, was formulated under the assumption that nonselective channels and ryanodine receptor channels operated separately from each other in the terminal cisternae. The remarkably large contribution of Cl- to the SR Ca2+ permeability suggested that nonselective Cl- channels may control the Ca2+ permeability of the SR in the resting muscle cell.