Reviews |
From the Departments of Physiology and Medicine, School of Medicine, University of Maryland, 655 W Baltimore St, Baltimore, MD, 21201.
Correspondence to Dr W. Gil Wier, Department of Physiology, University of Maryland, Baltimore, 655 W Baltimore St, Baltimore, MD 21201. E-mail gwier001{at}umaryland.edu
Key Words: Ca2+ spark excitation-contraction coupling L-type Ca2+ channel sarcoplasmic reticulum ryanodine receptor
| Introduction |
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| "Local Control" Theory of Cardiac E-C Coupling |
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Indirect evidence of local control of cardiac SR Ca2+ release was obtained from analysis of the relationship between whole-cell Ca2+ current and whole-cell SR Ca2+ release flux.10 11 Work of the previous years had produced a detailed description and theory of the whole-cell Ca2+ transient, in terms of the various cellular processes determining cytoplasmic free [Ca2+].12 13 14 15 16 Control of SR Ca2+ release by L-type Ca2+ current was established by similarities in the voltage dependence of peak SR Ca2+ release flux and peak Ca2+ current,10 and by the fact that SR Ca2+ release can be turned off by stopping the Ca2+ current rapidly,10 either by repolarization (where current deactivates) or by depolarization to very positive voltages (where driving force for Ca2+ entry is small). SR Ca2+ release can also be triggered by "tails" of Ca2+ current through L-type Ca2+ channels on repolarization from positive pulse potentials.12 (Repolarization would be expected only to deactivate a voltage-dependent release mechanism.) The key observation in suggesting local control, however, was that although both peak SR Ca2+ release and peak L-type Ca2+ current displayed a bell-shaped dependence on membrane voltage during voltage-clamp pulses, the relationships were, in fact, different. Small Ca2+ currents at negative potentials (where single-channel currents are relatively large) were much more efficacious in triggering SR Ca2+ release than Ca2+ currents at positive potentials (where single channel currents are more frequent but smaller). On the basis of these data, we11 postulated that SR Ca2+ release flux was controlled locally, by single L-type Ca2+ channel currents. Local release events could not be resolved, however, with the methods available at that time.
| Visualization of Local SR Ca2+ Release: Ca2+ Sparks |
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Ca2+ Sparks Evoked by Electrical Depolarization:
Relation to L-type Ca2+ Current
After the initial report of spontaneous Ca2+
sparks, several studies appeared in which Ca2+
sparks were evoked by electrical stimulation, thus providing the first
direct evidence that Ca2+ sparks might underlie
SR Ca2+ release during normal E-C coupling. The
first study combining whole-cell voltage clamp and confocal
microscopy17 revealed local, ryanodine-sensitive,
inhomogeneities in Ca2+ during small depolarizing
pulses that evoked only small Ca2+ currents.
These evoked local transients appeared to be identical to spontaneous
Ca2+ sparks, recorded in the same cells.
Spatially averaged [Ca2+], obtained by
integrating line-scan images, was identical to that obtained in the
earlier studies in which whole-cell Ca2+ had been
measured. These results made abundantly clear the fact that
observations of spatially averaged [Ca2+] would
be misleading for the understanding of E-C coupling, given that the
spatially averaged [Ca2+] was clearly different
from that in the region of the RyR. The sparks occurred near
t-tubules.18 Similar results were obtained during action
potentials,19 and cadmium, a blocker of L-type
Ca2+ channels, increased the inhomogeneity of the
Ca2+ transient, suggesting that individual SR
release events were distinguishable.
In a detailed study,3 it was shown that Ca2+ sparks were evoked with a time and voltage dependence similar to that expected for first latency histograms of L-type Ca2+ channels.20 When the probability of L-type Ca2+ channel activation is made extremely low through the use of Ca2+ channel blockers, only a few, widely separated L-type Ca2+ channels will open. Changes in spatial average [Ca2+]i were negligibly small under this condition, rendering it unlikely that the Ca2+ sparks could be triggered by anything other than the opening of a nearby L-type Ca2+ channel. Although single-channel currents could not be recorded or localized, it seems reasonable that the only factors that could explain the voltage and time dependence of the spatially isolated sparks were the voltage and time dependence of single L-type Ca2+ channels. A different study at the same time reached the same conclusion by showing that the number of Ca2+ sparks increased with voltage during ramped depolarization (-70 to -40 mV), similarly to the increase of the Ca2+ current with voltage during the ramp.4 Recently, two new studies21 22 have confirmed the original Ca2+ spark latency histograms3 and presented the experimental relationship between Ca2+ currents and Ca2+ spark probability in much more detail.
Several attempts have been made to describe precisely the mathematical relationship between the probability of evoking Ca2+ sparks and the Ca2+ current. The first of these3 provided the basic equation for the probability (Pi) that a Ca2+ spark will be triggered by the opening of a single L-type Ca2+ channel. A subsequent attempt used a similar analysis23 but failed to take into account the time dependence of the probability of L-type Ca2+ channel opening. This problem has now been recognized and clarified.24 The most detailed analysis of experimental data so far has been that of Collier et al,21 who found that the time constants describing Ca2+ current and Ca2+ spark occurrence were not significantly different at membrane potentials between -30 and +30 mV. From comparison of the experimental results to a simple model, these authors were able to confirm that the opening of a single L-type Ca2+ channel initiates a Ca2+ spark. Thus, the body of experimental and theoretical work, to date, supports the idea that Ca2+ sparks are triggered by the opening of a single L-type Ca2+ channel.
The question of how many Ca2+ ions must bind to an RyR to initiate a Ca2+ spark remains controversial. Mathematical modeling of the dyadic space suggested that the local [Ca2+]i would be proportional to the single L-type Ca2+ channel current, i.25 Some data have been presented23 that spark probability is dependent on the square (ie, power, 2) of the single channel current (and, therefore, possibly, on the square of local [Ca2+]) as might arise if two Ca2+ bind to an RyR to trigger a spark. A recent study26 using whole-cell Ca2+ transients and Ca2+ currents, however, demonstrated a linear relationship between peak Ca2+ currents and the maximum rate of rise of the Ca2+ transient, and the results were interpreted to mean that only one Ca2+ need bind to activate an RyR and Ca2+ release. The use of whole-cell fluorescence transients for this calculation seems inherently less reliable a method, as opposed to observing Ca2+ sparks directly.
Finally, activation of Ca2+ sparks by patch depolarization of cardiac cells has been achieved,27 although the probabilities of activation were lower than would be required for normal E-C coupling. It seems likely that formation of the membrane patch recording disrupted the normal coupling between L-type Ca2+ channel and RyR. Thus, direct evidence, in the form of simultaneous recordings, that a single opening of a single L-type Ca2+ channel can trigger a Ca2+ spark, is still lacking.
Ca2+ Sparks Sum in Space and Time to Produce the
Whole-Cell Ca2+ Transient
The work described above supported the concept that
Ca2+ sparks are activated by L-type
Ca2+ channel currents but did not establish
directly that Ca2+ sparks summed independently to
produce the whole-cell Ca2+ transient. Cannell et
al19 had provided theoretical evidence of the feasibility
of this idea. The fact that the total number of
Ca2+ sparks depended on voltage in the same
manner as the whole-cell Ca2+
transient3 also implied that this was true. Nevertheless,
direct evidence on this point has been lacking, until recently, when
local Ca2+ release has been imaged with fast
confocal microscopes with line scanning28 and with 2D
(full frame) imaging.22 The line-scan
images28 showed local release, at z lines, during the
initial phase of a normal Ca2+ transient.
Furthermore, if a Ca2+ spark had occurred
spontaneously just previously at a particular z line, then release
failed at that z line, indicating directly the role of
Ca2+ sparks in E-C coupling (and that the
processes producing Ca2+ sparks may experience
refractoriness). The fast 2D images22 also showed
localized release, probably at dyadic junctions. It has been suggested
that the nonlinear relationship between single-channel current and SR
Ca2+ release (possibly dependent on
i2) provides a mechanism whereby
relatively small local changes in
[Ca2+]i can increase
spark probability by a factor of 104 during
normal E-C coupling.24
Whole-cell Ca2+ release flux has been measured directly recently29 using a novel fluorescence method, in which cytoplasmic [Ca2+]i is reduced through the use of high concentrations of EGTA, and localized SR Ca2+ release is observed with the low-affinity fast Ca2+ indicator, Oregon Green 488 BAPTA-5N. This method permits visualization of release at specific sites during voltage-clamp pulses. The overall waveform of the release and its absolute value were reported similar to that obtained earlier,10 11 16 through mathematical analysis of the whole-cell Ca2+ transient, in the absence of EGTA. The number of Ca2+ sparks involved in the total release flux remains to be determined.
Molecular Origin and Mechanisms of Cardiac Ca2+
Sparks
The molecule responsible for Ca2+ sparks in
cardiac muscle is the RyR2 isoform of the
ryanodine receptor. Cheng et al2 clearly favored the
hypothesis that Ca2+ sparks arose from the
opening of a single RyR, which would certainly be an "elementary
event," because it would arise from one molecule. Of course, the
possibility that Ca2+ sparks arose from a small
number of RyR "acting in concert" could not be excluded by their
data. The distinction between these possibilities is extremely
important, however, for our understanding of the mechanism of SR
Ca2+ release during E-C coupling. If, in fact, a
Ca2+ spark arises from just one RyR, then we are
left with the very puzzling question of why the others in the group are
not activated by the Ca2+ released from
one. Similarly, if they "act in concert," then the very interesting
question of cooperativity among a large group of macromolecules arises.
Much of the work appearing to establish Ca2+
sparks as elementary events of E-C coupling relied on accurately
counting the numbers of Ca2+ sparks in confocal
line-scan images. Sparks were typically identified subjectively, or on
the basis of some arbitrary criterion, such as minimum spatial
half-width or an amplitude threshold. This enabled counting
Ca2+ sparks, and when such criteria were used, it
appeared that spontaneous and evoked Ca2+ sparks
were identical. Furthermore, the mean amplitude of (counted) evoked
Ca2+ sparks was independent of
voltage,3 a finding confirmed again
recently.21 However, confocal line-scan images invariably
show small changes in fluorescence that are difficult to
categorize. Are these Ca2+ sparks occurring off
the laser scan line, or are they different types of events of SR
Ca2+ release? The possible existence of events of
SR Ca2+ release different from
Ca2+ sparks or yet smaller than
Ca2+ sparks throws into question the notion of
Ca2+ sparks as truly "elementary" events of
E-C coupling. Furthermore, it was recognized early on that the
limitations of confocal imaging will make it difficult to distinguish
out-of-focus Ca2+ sparks from possible small
Ca2+ sparks.30 31 At present,
the question of the number of RyR and their gating pattern underlying
cardiac Ca2+ sparks remains
unresolved.32 Nevertheless, the theory of
Ca2+ spark amplitude distributions is now better
understood, both in cardiac muscle33 and in skeletal
muscle.34 In addition, "automatic
Ca2+ spark detection"
programs29 33 can be used to eliminate bias of the
observer. The best available data from analysis of
Ca2+ spark amplitude distributions suggest that
they represent a distribution of "source
strengths."33 Here, "source strength" refers to the
combination of RyR open time and current amplitude. At present,
however, it cannot be distinguished reliably whether or not such
Ca2+ spark amplitude distributions are fit better
by a gaussian distribution or an exponential distribution of "source
strengths."
The first substantive indication that cardiac Ca2+ sparks may not arise from single RyR came when multiple sites of origin were resolved in ventricular cells35 and in atrial cells.36 In ventricular cells, transverse scanning revealed multiple sites of origin, perhaps corresponding to separate clusters of RyR.
Ca2+ sparks with multiple sites of origin are distinct from the postulated Ca2+ quarks, which may represent release from single RyR. When SR Ca2+ release was evoked by photolysis of caged Ca2+ in the whole cell, Ca2+ sparks were not observed, leading to the suggestion that release occurred as unresolvable events.37 The existence of Ca2+ quarks was postulated, units of SR release smaller than Ca2+ sparks. This release gave rise to spatially uniform changes in Ca2+, a puzzling observation because of the lack of any known uniformly distributed SR Ca2+ release channels. When Ca2+ was released in a small volume by two-photon photolysis,38 small events of SR Ca2+ release were observed directly, for the first time. These were abolished by SR depletion (and therefore not due directly to photolytically released Ca2+) and were smaller in amplitude than typical Ca2+ sparks.
The original computations of the flux of Ca2+
underlying Ca2+ sparks was consistent
with the idea that a Ca2+ spark could arise from
a single RyR, if it was assumed that the flux through a single RyR was
4 pA. However, the most recent data from lipid bilayer experiments
under quasiphysiological conditions39
suggest that the unitary Ca2+ current should be
<0.6 pA. This implies that multiple RyR are involved in the generation
of a Ca2+ spark. Although comparisons between
cardiac Ca2+ sparks and frog skeletal muscle
Ca2+ sparks may not be valid, a detailed model of
E-C coupling in this tissue suggests that Ca2+
sparks arise from multiple RyR.40 Recently, "coupled"
gating of isolated RyR has been demonstrated,41 and the
potential of "coordinated" gating of cardiac RyR to explain cardiac
E-C coupling has been noted.42
Termination of the Ca2+ spark and/or refractoriness in spark generation is expected to be extremely important in E-C coupling. A mechanism must exist by which RyR are inactivated and not available to release Ca2+ again, in order for a Ca2+ transient to be produced. This mechanism appears not to be either SR depletion or "stochastic inactivation."43 44 Ca2+ release appears to be terminated by an "active extinguishing mechanism" such as Ca2+-dependent inactivation or adaptation. The possible roles in terminating release of the accessory proteins, sorcin and FKBP12, have been discussed recently.45
| Other Putative Sources of Ca2+ to Trigger SR Ca2+ Release |
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Recently, a new and functionally distinct Na+ current component (ICa(TTX)) has been identified in rat ventricular cells.49 This new component displays different kinetics, different voltage ranges for both activation and inactivation, and different permeability properties from the classical cardiac Na+ channel. Specifically, ICa(TTX) activates over a more negative voltage range than classical cardiac Na+ channels and is highly permeable to Ca2+. Under nonphysiological experimental conditions (ie, Na+-free external and internal solutions), Ca2+ permeation of ICa(TTX) is capable of triggering SR Ca2+ release.50 These ICa(TTX)-evoked Ca2+ transients are delayed markedly in onset and have slower upstrokes compared with Ca2+ transients elicited by L-type Ca2+ currents of similar current density. It is not yet known whether ICa(TTX) channels are permeable to Ca2+ in the presence of physiological concentrations of Na+. To the extent that ICa(TTX) is relevant to E-C coupling, it will probably have a modulatory role rather than provide a major component of the Ca2+ trigger for SR Ca2+ release and the "gain" of cardiac E-C coupling.
A tetrodotoxin (TTX)-blockable Ca2+ current
has been reported51 in rat ventricular
myocytes after several pharmacological treatments (cAMP, isoproterenol
[ISO], or the cardiotonic steroids, ouabain and digoxin), and this
current appears capable of triggering Ca2+
sparks. This TTX-blockable Ca2+ current was
attributed to a Ca2+ permeability induced in
classical cardiac Na+ channels that are normally
impermeable to Ca2+. Treated
Na+ channels were then said to be
"promiscuous." Although intriguing, these results are as yet
unconfirmed, and two separate lines of experimental evidence challenge
the conclusion of cAMP-induced Ca2+ permeability
of classical cardiac Na+ channels. (1) In
voltage-clamped rat ventricular cells, Balke et
al52 and Goldman et al53 have shown that ISO
substantially increases the TTX-blockable Ca2+
current. Importantly, all of this induced current flows through
ICa(TTX) channels and not through classical
Na+ channels, because the ISO-mediated increase
in ICa(TTX) was not accompanied by a
reduction in INa as would be required.
Therefore, these experiments are not consistent with a change
in selectivity of classical Na+ channels induced
by conditions that promote channel phosphorylation.
These experiments are in agreement with findings in guinea
pig,54 rabbit,55 and canine
ventricular myocytes,56 as well as in rat
cardiac Na+ (SkM2) channels expressed
heterologously in frog oocytes.57 (2) In Chinese hamster
ovary cells overexpressing
subunits of the cardiac
Na+ channels both with and without
ß1 subunits, Nuss and
Marbán58 59 have shown that the well-described
ISO-mediated increase in INa was completely
occluded with removal of external Na+ in the
continued presence of external Ca2+. In cells
expressing both
and ß1 subunits in
Na+- and Ca2+-containing
external solutions, Na+ conductance increased
with ISO but without any changes in reversal potential. In these
experiments, neither ß1 coexpression or the
presence of external Na+ conferred
Ca2+ permeability on classical cardiac
Na+ channels. However, Cruz et
al60 demonstrated a significant shift in reversal
potential with dbcAMP in HEK293 cells expressing either the
and
ß1 subunit or the
,
ß1, and ß2 subunits of
the Na+ channel.
| Putative Protein Kinase ADependent Voltage-Sensitive Ca2+ Release Mechanism (VSRM) |
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The experiments described above are intriguing, but we have several reservations about them. (1) Voltage-activated Ca2+ release should occur in the absence of external Ca2+. This has not been demonstrated adequately in any of the experiments cited above. On the contrary, Nabauer et al64 have already shown (rather convincingly) that contractions elicited by clamp pulses from -60 mV (and more negative) to 0 mV fail completely after switching rapidly to Ca2+ free solutions. Most importantly, neither Na+ nor Ba2+, which do flow through L-type Ca2+ channels and which do support voltage-activated Ca2+ release in skeletal muscle, was capable of eliciting contraction. These elegant and conclusive experiments64 should be repeated in the presence of high concentrations of intracellular cAMP. (2) Ca2+ channels are not totally unavailable at -40 mV and therefore, steps to -40 mV will activate L-type Ca2+ channels, particularly in the highly potentiated state produced by high concentrations of cAMP. The small currents flowing at -40 mV should be identified unequivocally. (3) The VSRM should be studied mainly at positive potentials, where it is well established that Ca2+ entry is not sufficient to trigger contraction, but a VSRM should be fully activated. In fact, recent work65 using similar conditions to those used by Ferrier et al6 failed to show Ca2+ release at very positive membrane potentials. (4) The amount of contraction in the experiments cited above is relatively small. For example, contractions were only about 3 µm at 0 mV from -65 mV with 50 µmol/L cAMP (Figure 10 of Reference 6363 ). Such small contractions, under such highly potentiated conditions, are puzzling. (5) The L-type Ca2+ currents in the presence of 50 µmol/L cAMP are extremely large (eg, 7 nA, Figure 1 of Reference 6363 ). Under these conditions, the SR must be highly loaded, particularly because the SERCA will be highly stimulated. Under these conditions, it may be "trigger happy." Regenerative releases could be stimulated by the opening of just a few Ca2+ channels. (6) It will be difficult to study the putative VSRM selectively, because any release activated by voltage may inevitably be amplified by CICR. In frog skeletal muscle, the voltage-activated release is thought to provide the initial change in Ca2+ that activates the RyR, via CICR, that are not facing voltage sensors.40 It is not possible to separate totally one type of release from the other. (7) Ca2+ transients should be measured, and the rate of SR Ca2+ release flux should be calculated.10 29 Maximum shortening is not a reliable indicator of the peak rate of SR Ca2+ release in mechanically unloaded myocytes. (8) Organic L-type Ca2+ channel blockers should be compared with the inorganic blockers (Cd2+, Ni2+, and Co2+), because the mode of block of these substances is quite different. (9) The experiments demonstrating VSRM in dialyzed cells use cAMP in the intracellular perfusion solution, and L-type Ca2+ currents are very large. We wonder, therefore, whether cells in such a condition are capable of responding further to ß1-agonist stimulation. Within the living organism, the heart is capable of increasing output substantially over basal levels as a result of ß1-agonist stimulation. If cells demonstrating VSRM are not responsive to ß1-agonist stimulation, the implication is that the VSRM is not important in normal E-C coupling in the basal state.
From the above, we conclude that, if VSRM exists in cardiac muscle, it must differ substantially from voltage-activated release in skeletal muscle. Finally, the difficulty of controlling or regulating such a putative mechanism has been pointed out recently.66
| Summary |
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| Footnotes |
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Ca2+ Release Mechanisms, Ca2+ Sparks, and Local Control of Excitation-Contraction Coupling in Normal Heart Muscle
Interactions Between Ca2+ and H+ and Functional Consequences in Vascular Smooth Muscle Cells
Intracellular Calcium Release Channels Calcium Fluxes Involved in Control of Cardiac Myocyte Contraction
C. William Balke, Guest Editor ![]()
Received July 2, 1999; accepted August 25, 1999.
| References |
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