Functional properties of a newly identified C-terminal splice variant of Cav1.3 L-type Ca2+ channels

An intramolecular interaction between a distal (DCRD) and a proximal regulatory domain (PCRD) within the C terminus of long Ca(v)1.3 L-type Ca(2+) channels (Ca(v)1.3(L)) is a major determinant of their voltage- and Ca(2+)-dependent gating kinetics. Removal of these regulatory domains by alternative splicing generates Ca(v)1.3(42A) channels that activate at a more negative voltage range and exhibit more pronounced Ca(2+)-dependent inactivation. Here we describe the discovery of a novel short splice variant (Ca(v)1.3(43S)) that is expressed at high levels in the brain but not in the heart. It lacks the DCRD but, in contrast to Ca(v)1.3(42A), still contains PCRD. When expressed together with α2δ1 and β3 subunits in tsA-201 cells, Ca(v)1.3(43S) also activated at more negative voltages like Ca(v)1.3(42A) but Ca(2+)-dependent inactivation was less pronounced. Single channel recordings revealed much higher channel open probabilities for both short splice variants as compared with Ca(v)1.3(L). The presence of the proximal C terminus in Ca(v)1.3(43S) channels preserved their modulation by distal C terminus-containing Ca(v)1.3- and Ca(v)1.2-derived C-terminal peptides. Removal of the C-terminal modulation by alternative splicing also induced a faster decay of Ca(2+) influx during electrical activities mimicking trains of neuronal action potentials. Our findings extend the spectrum of functionally diverse Ca(v)1.3 L-type channels produced by tissue-specific alternative splicing. This diversity may help to fine tune Ca(2+) channel signaling and, in the case of short variants lacking a functional C-terminal modulation, prevent excessive Ca(2+) accumulation during burst firing in neurons. This may be especially important in neurons that are affected by Ca(2+)-induced neurodegenerative processes.     

Gating and conductance properties of BK channels are modulated by the S9-S10 tail domain of the alpha subunit. A study of mSlo1 and mSlo3 wild-type and chimeric channels.

The COOH-terminal S9-S10 tail domain of large conductance Ca(2+)-activated K(+) (BK) channels is a major determinant of Ca(2+) sensitivity (Schreiber, M., A. Wei, A. Yuan, J. Gaut, M. Saito, and L. Salkoff. 1999. Nat. Neurosci. 2:416-421). To investigate whether the tail domain also modulates Ca(2+)-independent properties of BK channels, we explored the functional differences between the BK channel mSlo1 and another member of the Slo family, mSlo3 (Schreiber, M., A. Yuan, and L. Salkoff. 1998. J. Biol. Chem. 273:3509-3516). Compared with mSlo1 channels, mSlo3 channels showed little Ca(2+) sensitivity, and the mean open time, burst duration, gaps between bursts, and single-channel conductance of mSlo3 channels were only 32, 22, 41, and 37% of that for mSlo1 channels, respectively. To examine which channel properties arise from the tail domain, we coexpressed the core of mSlo1 with either the tail domain of mSlo1 or the tail domain of mSlo3 channels, and studied the single-channel currents. Replacing the mSlo1 tail with the mSlo3 tail resulted in the following: increased open probability in the absence of Ca(2+); reduced the Ca(2+) sensitivity greatly by allowing only partial activation by Ca(2+) and by reducing the Hill coefficient for Ca(2+) activation; decreased the voltage dependence approximately 28%; decreased the mean open time two- to threefold; decreased the mean burst duration three- to ninefold; decreased the single-channel conductance approximately 14%; decreased the K(d) for block by TEA(i) approximately 30%; did not change the minimal numbers of three to four open and five to seven closed states entered during gating; and did not change the major features of the dependency between adjacent interval durations. These observations support a modular construction of the BK channel in which the tail domain modulates the gating kinetics and conductance properties of the voltage-dependent core domain, in addition to determining most of the high affinity Ca(2+) sensitivity.     

Voltage and Ca2+ activation of single large-conductance Ca2+-activated K+ channels described by a two-tiered allosteric gating mechanism

The voltage- and Ca2+-dependent gating mechanism of large-conductance Ca2+-activated K+ (BK) channels from cultured rat skeletal muscle was studied using single-channel analysis. Channel open probability (Po) increased with depolarization, as determined by limiting slope measurements (11 mV per e-fold change in Po; effective gating charge, q(eff), of 2.3 +/- 0.6 e(o)). Estimates of q(eff) were little changed for intracellular Ca2+ (Ca2+(i)) ranging from 0.0003 to 1,024 microM. Increasing Ca2+(i) from 0.03 to 1,024 microM shifted the voltage for half maximal activation (V(1/2)) 175 mV in the hyperpolarizing direction. V(1/2) was independent of Ca2+(i) for Ca2+(i) < or = 0.03 microM, indicating that the channel can be activated in the absence of Ca2+(i). Open and closed dwell-time distributions for data obtained at different Ca2+(i) and voltage, but at the same Po, were different, indicating that the major action of voltage is not through concentrating Ca2+ at the binding sites. The voltage dependence of Po arose from a decrease in the mean closing rate with depolarization (q(eff) = -0.5 e(o)) and an increase in the mean opening rate (q(eff) = 1.8 e(o)), consistent with voltage-dependent steps in both the activation and deactivation pathways. A 50-state two-tiered model with separate voltage- and Ca2+-dependent steps was consistent with the major features of the voltage and Ca2+ dependence of the single-channel kinetics over wide ranges of Ca2+(i) (approximately 0 through 1,024 microM), voltage (+80 to -80 mV), and Po (10(-4) to 0.96). In the model, the voltage dependence of the gating arises mainly from voltage-dependent transitions between closed (C-C) and open (O-O) states, with less voltage dependence for transitions between open and closed states (C-O), and with no voltage dependence for Ca2+-binding and unbinding. The two-tiered model can serve as a working hypothesis for the Ca2+- and voltage-dependent gating of the BK channel.     

Allosteric voltage gating of potassium channels I. Mslo ionic currents in the absence of Ca(2+).

Activation of large conductance Ca(2+)-activated K(+) channels is controlled by both cytoplasmic Ca(2+) and membrane potential. To study the mechanism of voltage-dependent gating, we examined mSlo Ca(2+)-activated K(+) currents in excised macropatches from Xenopus oocytes in the virtual absence of Ca(2+) (<1 nM). In response to a voltage step, I(K) activates with an exponential time course, following a brief delay. The delay suggests that rapid transitions precede channel opening. The later exponential time course suggests that activation also involves a slower rate-limiting step. However, the time constant of I(K) relaxation [tau(I(K))] exhibits a complex voltage dependence that is inconsistent with models that contain a single rate limiting step. tau(I(K)) increases weakly with voltage from -500 to -20 mV, with an equivalent charge (z) of only 0.14 e, and displays a stronger voltage dependence from +30 to +140 mV (z = 0.49 e), which then decreases from +180 to +240 mV (z = -0.29 e). Similarly, the steady state G(K)-V relationship exhibits a maximum voltage dependence (z = 2 e) from 0 to +100 mV, and is weakly voltage dependent (z congruent with 0.4 e) at more negative voltages, where P(o) = 10(-5)-10(-6). These results can be understood in terms of a gating scheme where a central transition between a closed and an open conformation is allosterically regulated by the state of four independent and identical voltage sensors. In the absence of Ca(2+), this allosteric mechanism results in a gating scheme with five closed (C) and five open (O) states, where the majority of the channel's voltage dependence results from rapid C-C and O-O transitions, whereas the C-O transitions are rate limiting and weakly voltage dependent. These conclusions not only provide a framework for interpreting studies of large conductance Ca(2+)-activated K(+) channel voltage gating, but also have important implications for understanding the mechanism of Ca(2+) sensitivity.     

Altered Ca2+ sparks and gating properties of ryanodine receptors in aging cardiomyocytes

To investigate the cellular mechanisms for altered cardiac function in senescence, we measured Ca(2+) transients and Ca(2+) sparks in ventricular cardiomyocytes from 6- to 24-month-old Fisher 344 (F344) rat hearts. The single channel properties of ryanodine receptors from adult and senescent hearts were also studied. In senescent myocytes, we observed a decreased peak [Ca(2+)](i) amplitude and an increased time constant for decay (tau), both of which correlated with a reduced Ca(2+) content of the sarcoplasmic reticulum (SR). Our studies also revealed that senescent cardiomyocytes had an increased frequency of Ca(2+) sparks and a slight but statistically significant decrease in average amplitude, full-width-at-half-maximum (FWHM) and full-duration-at-half-maximum (FDHM). Single channel recordings of ryanodine receptors (RyR2) demonstrated that in aging hearts, the open probability (P(o)) of RyR2 was increased but the mean open time was shorter, providing a molecular correlate for the increased frequency of Ca(2+) sparks and decreased size of sparks, respectively. Thus, modifications of normal RyR2 gating properties may play a role in the altered Ca(2+) homeostasis observed in senescent myocytes.     

Electrostatic changes in phosphorylase kinase induced by its obligatory allosteric activator Ca2+

Skeletal muscle phosphorylase kinase (PhK) is a 1.3-MDa hexadecameric complex that catalyzes the phosphorylation and activation of glycogen phosphorylase b. PhK has an absolute requirement for Ca(2+) ions, which couples the cascade activation of glycogenolysis with muscle contraction. Ca(2+) activates PhK by binding to its nondissociable calmodulin subunits; however, specific changes in the structure of the PhK complex associated with its activation by Ca(2+) have been poorly understood. We present herein the first comparative investigation of the physical characteristics of highly purified hexadecameric PhK in the absence and presence of Ca(2+) ions using a battery of biophysical probes as a function of temperature. Ca(2+)-induced differences in the tertiary and secondary structure of PhK measured by fluorescence, UV absorption, FTIR, and CD spectroscopies as low resolution probes of PhK's structure were subtle. In contrast, the surface electrostatic properties of solvent accessible charged and polar groups were altered upon the binding of Ca(2+) ions to PhK, which substantially affected both its diffusion rate and electrophoretic mobility, as measured by dynamic light scattering and zeta potential analyses, respectively. Overall, the observed physicochemical effects of Ca(2+) binding to PhK were numerous, including a decrease in its electrostatic surface charge that reduced particle mobility without inducing a large alteration in secondary structure content or hydrophobic tertiary interactions. Without exception, for all analyses in which the temperature was varied, the presence of Ca(2+) rendered the enzyme increasingly labile to thermal perturbation.     

Modulation of voltage- and Ca2+-dependent gating of CaV1.3 L-type calcium channels by alternative splicing of a C-terminal regulatory domain

Low voltage activation of Ca(V)1.3 L-type Ca(2+) channels controls excitability in sensory cells and central neurons as well as sinoatrial node pacemaking. Ca(V)1.3-mediated pacemaking determines neuronal vulnerability of dopaminergic striatal neurons affected in Parkinson disease. We have previously found that in Ca(V)1.4 L-type Ca(2+) channels, activation, voltage, and calcium-dependent inactivation are controlled by an intrinsic distal C-terminal modulator. Because alternative splicing in the Ca(V)1.3 alpha1 subunit C terminus gives rise to a long (Ca(V)1.3(42)) and a short form (Ca(V)1.3(42A)), we investigated if a C-terminal modulatory mechanism also controls Ca(V)1.3 gating. The biophysical properties of both splice variants were compared after heterologous expression together with beta3 and alpha2delta1 subunits in HEK-293 cells. Activation of calcium current through Ca(V)1.3(42A) channels was more pronounced at negative voltages, and inactivation was faster because of enhanced calcium-dependent inactivation. By investigating several Ca(V)1.3 channel truncations, we restricted the modulator activity to the last 116 amino acids of the C terminus. The resulting Ca(V)1.3(DeltaC116) channels showed gating properties similar to Ca(V)1.3(42A) that were reverted by co-expression of the corresponding C-terminal peptide C(116). Fluorescence resonance energy transfer experiments confirmed an intramolecular protein interaction in the C terminus of Ca(V)1.3 channels that also modulates calmodulin binding. These experiments revealed a novel mechanism of channel modulation enabling cells to tightly control Ca(V)1.3 channel activity by alternative splicing. The absence of the C-terminal modulator in short splice forms facilitates Ca(V)1.3 channel activation at lower voltages expected to favor Ca(V)1.3 activity at threshold voltages as required for modulation of neuronal firing behavior and sinoatrial node pacemaking.     

Mapping the BKCa channel's "Ca2+ bowl": side-chains essential for Ca2+ sensing

There is controversy over whether Ca(2+) binds to the BK(Ca) channel's intracellular domain or its integral-membrane domain and over whether or not mutations that reduce the channel's Ca(2+) sensitivity act at the point of Ca(2+) coordination. One region in the intracellular domain that has been implicated in Ca(2+) sensing is the "Ca(2+) bowl". This region contains many acidic residues, and large Ca(2+)-bowl mutations eliminate Ca(2+) sensing through what appears to be one type of high-affinity Ca(2+)-binding site. Here, through site-directed mutagenesis we have mapped the residues in the Ca(2+) bowl that are most important for Ca(2+) sensing. We find acidic residues, D898 and D900, to be essential, and we find them essential as well for Ca(2+) binding to a fusion protein that contains a portion of the BK(Ca) channel's intracellular domain. Thus, much of our data supports the conclusion that Ca(2+) binds to the BK(Ca) channel's intracellular domain, and they define the Ca(2+) bowl's essential Ca(2+)-sensing motif. Overall, however, we have found that the relationship between mutations that disrupt Ca(2+) sensing and those that disrupt Ca(2+) binding is not as strong as we had expected, a result that raises the possibility that, when examined by gel-overlay, the Ca(2+) bowl may be in a nonnative conformation.     

Functional coupling of the beta(1) subunit to the large conductance Ca(2+)-activated K(+) channel in the absence of Ca(2+). Increased Ca(2+) sensitivity from a Ca(2+)-independent mechanism

Coexpression of the beta(1) subunit with the alpha subunit (mSlo) of BK channels increases the apparent Ca(2+) sensitivity of the channel. This study investigates whether the mechanism underlying the increased Ca(2+) sensitivity requires Ca(2+), by comparing the gating in 0 Ca(2+)(i) of BK channels composed of alpha subunits to those composed of alpha+beta(1) subunits. The beta(1) subunit increased burst duration approximately 20-fold and the duration of gaps between bursts approximately 3-fold, giving an approximately 10-fold increase in open probability (P(o)) in 0 Ca(2+)(i). The effect of the beta(1) subunit on increasing burst duration was little changed over a wide range of P(o) achieved by varying either Ca(2+)(i) or depolarization. The effect of the beta(1) subunit on increasing the durations of the gaps between bursts in 0 Ca(2+)(i) was preserved over a range of voltage, but was switched off as Ca(2+)(i) was increased into the activation range. The Ca(2+)-independent, beta(1) subunit-induced increase in burst duration accounted for 80% of the leftward shift in the P(o) vs. Ca(2+)(i) curve that reflects the increased Ca(2+) sensitivity induced by the beta(1) subunit. The Ca(2+)-dependent effect of the beta(1) subunit on the gaps between bursts accounted for the remaining 20% of the leftward shift. Our observation that the major effects of the beta(1) subunit are independent of Ca(2+)(i) suggests that the beta(1) subunit mainly alters the energy barriers of Ca(2+)-independent transitions. The changes in gating induced by the beta(1) subunit differ from those induced by depolarization, as increasing P(o) by depolarization or by the beta(1) subunit gave different gating kinetics. The complex gating kinetics for both alpha and alpha+beta(1) channels in 0 Ca(2+)(i) arise from transitions among two to three open and three to five closed states and are inconsistent with Monod-Wyman-Changeux type models, which predict gating among only one open and one closed state in 0 Ca(2+)(i).     

Distinct properties of CRAC and MIC channels in RBL cells

In rat basophilic leukemia (RBL) cells and Jurkat T cells, Ca(2+) release-activated Ca(2+) (CRAC) channels open in response to passive Ca(2+) store depletion. Inwardly rectifying CRAC channels admit monovalent cations when external divalent ions are removed. Removal of internal Mg(2+) exposes an outwardly rectifying current (Mg(2+)-inhibited cation [MIC]) that also admits monovalent cations when external divalent ions are removed. Here we demonstrate that CRAC and MIC currents are separable by ion selectivity and rectification properties: by kinetics of activation and susceptibility to run-down and by pharmacological sensitivity to external Mg(2+), spermine, and SKF-96365. Importantly, selective run-down of MIC current allowed CRAC and MIC current to be characterized under identical ionic conditions with low internal Mg(2+). Removal of internal Mg(2+) induced MIC current despite widely varying Ca(2+) and EGTA levels, suggesting that Ca(2+)-store depletion is not involved in activation of MIC channels. Increasing internal Mg(2+) from submicromolar to millimolar levels decreased MIC currents without affecting rectification but did not alter CRAC current rectification or amplitudes. External Mg(2+) and Cs(+) carried current through MIC but not CRAC channels. SKF-96365 blocked CRAC current reversibly but inhibited MIC current irreversibly. At micromolar concentrations, both spermine and extracellular Mg(2+) blocked monovalent MIC current reversibly but not monovalent CRAC current. The biophysical characteristics of MIC current match well with cloned and expressed TRPM7 channels. Previous results are reevaluated in terms of separate CRAC and MIC channels.     

Molecular evolution and structural analysis of the Ca(2+) release-activated Ca(2+) channel subunit, Orai

Depletion of intracellular Ca(2+) stores evokes Ca(2+) entry across the plasma membrane by inducing Ca(2+) release-activated Ca(2+) (CRAC) currents in many cell types. Recently, Orai and STIM proteins were identified as the molecular identities of the CRAC channel subunit and the endoplasmic reticulum Ca(2+) sensor, respectively. Here, extensive database searching and phylogenetic analysis revealed several lineage-specific duplication events in the Orai protein family, which may account for the evolutionary origins of distinct functional properties among mammalian Orai proteins. Based on similarity to key structural domains and essential residues for channel functions in Orai proteins, database searching also identifies a putative primordial Orai sequence in hyperthermophilic archaeons. Furthermore, modern Orai appears to acquire new structural domains as early as Urochodata, before divergence into vertebrates. The evolutionary patterns of structural domains might be related to distinct functional properties of Drosophila and mammalian CRAC currents. Interestingly, Orai proteins display two conserved internal repeats located at transmembrane segments 1 and 3, both of which contain key amino acids essential for channel function. These findings demonstrate biochemical and physiological relevance of Orai proteins in light of different evolutionary origins and will provide novel insights into future structural and functional studies of Orai proteins.     

Effect of SIN-1 in rat ventricular myocytes: interference with beta-adrenergic stimulation

We have examined the effects of the nitric oxide (NO) donor, 3-morpholino-sydnonimine (SIN-1), on Ca(2+) transients, L-type Ca(2+) current (I(Ca,L)), and cGMP/cAMP content in electrically-stimulated rat ventricular myocytes in the absence and presence of the beta-adrenergic stimulation with isoproterenol. SIN-1 had no effect at low concentrations, but decreased the amplitude of electrically-induced Ca(2+) transients at higher concentrations. SIN-1 attenuated the increase in Ca(2+) transients induced by isoproterenol in a concentration-dependent manner. SIN-1 Also reduced the amplitude of caffeine-induced Ca(2+) transients, and the increase in I(Ca,L) induced by isoproterenol. These effects of SIN-1 were associated with an increased cGMP and a decreased cAMP content in ventricular myocytes in either the absence or presence of isoproterenol. These data suggest that the inhibitory effect of SIN-1 on basal and beta-adrenergic stimulated Ca2+ signal in ventricular myocytes could be due to the depression in the SR function and I(Ca,L), possibly mediated by a cGMP/cAMP-dependent mechanism. Taken together, the present study supports the idea that NO acts as an inhibitory modulator of the cardiac function during pathological conditions associated with an abnormal production of NO such as septic shock.     

Biophysical re-equilibration of Ca2+ fluxes as a simple biologically plausible explanation for complex intracellular Ca2+ release patterns

Physiological regulation of Ca(2+) release from the endoplasmic reticulum (ER) is critical for cell function. Recent direct measurements of free [Ca(2+)] inside the ER ([Ca(2+)](ER)) revealed that [Ca(2+)](ER) itself is a key regulator of ER Ca(2+) handling. However, the role of this new regulatory process in generating various patterns of Ca(2+) release remains to be elucidated in detail. Here, we incorporate the recently quantified experimental correlations between [Ca(2+)](ER) and Ca(2+) movements across the ER membrane into a mathematical model ER Ca(2+) handling. The model reproduces basic experimental dynamics of [Ca(2+)](ER). Although this was not goal in model design, the model also exhibits mechanistically unclear experimental phenomena such as "quantal" Ca(2+) release, and "store charging" by increasing resting cytosolic [Ca(2+)]. While more complex explanations cannot be ruled out, on the basis of our data we propose that "quantal release" and "store charging" could be simple re-equilibration phenomena, predicted by the recently quantified biophysical dynamics of Ca(2+) movements across the ER membrane.     

Calcium-induced calcium release in smooth muscle: loose coupling between the action potential and calcium release

Calcium-induced calcium release (CICR) has been observed in cardiac myocytes as elementary calcium release events (calcium sparks) associated with the opening of L-type Ca(2+) channels. In heart cells, a tight coupling between the gating of single L-type Ca(2+) channels and ryanodine receptors (RYRs) underlies calcium release. Here we demonstrate that L-type Ca(2+) channels activate RYRs to produce CICR in smooth muscle cells in the form of Ca(2+) sparks and propagated Ca(2+) waves. However, unlike CICR in cardiac muscle, RYR channel opening is not tightly linked to the gating of L-type Ca(2+) channels. L-type Ca(2+) channels can open without triggering Ca(2+) sparks and triggered Ca(2+) sparks are often observed after channel closure. CICR is a function of the net flux of Ca(2+) ions into the cytosol, rather than the single channel amplitude of L-type Ca(2+) channels. Moreover, unlike CICR in striated muscle, calcium release is completely eliminated by cytosolic calcium buffering. Thus, L-type Ca(2+) channels are loosely coupled to RYR through an increase in global [Ca(2+)] due to an increase in the effective distance between L-type Ca(2+) channels and RYR, resulting in an uncoupling of the obligate relationship that exists in striated muscle between the action potential and calcium release.     

Altered cerebellar function in mice lacking CaV2.3 Ca2+ channel

Voltage-dependent Ca(2+) channels play important roles in cerebellar functions including motor coordination and learning. Since abundant expression of Ca(V)2.3 Ca(2+) channel gene in the cerebellum was detected, we searched for possible deficits in the cerebellar functions in the Ca(V)2.3 mutant mice. Behavioral analysis detected in delayed motor learning in rotarod tests in mice heterozygous and homozygous for the Ca(V)2.3 gene disruption (Ca(V)2.3+/- and Ca(V)2.3-/-, respectively). Electrophysiological analysis of mutant mice revealed perplexing results: deficit in long-term depression (LTD) at the parallel fiber Purkinje cell synapse in Ca(V)2.3+/- mice but apparently normal LTD in Ca(V)2.3-/- mice. On the other hand, the number of spikes evoked by current injection in Purkinje cells under the current-clamp mode decreased in Ca(V)2.3 mutant mice in a gene dosage-dependent manner, suggesting that Ca(V)2.3 channel contributed to spike generation in Purkinje cells. Thus, Ca(V)2.3 channel seems to play some roles in cerebellar functions.     

The biochemical activation of T-type Ca2+ channels in HEK293 cells stably expressing alpha1G and Kir2.1 subunits

In order to investigate the currently unknown cellular signaling pathways of T-type Ca(2+) channels, we decided to construct a new cell line which would stably express alpha(1G) and Kir2.1 subunits in HEK293 cells (HEK293/alpha(1G)/Kir2.1). Compared to cells which only expressed alpha(1G) (HEK293/alpha(1G)), HEK293/alpha(1G)/Kir2.1 cells produced an enormous inward rectifying current which was blocked by external Ba(2+) and Cs(+) in a concentration-dependent manner. The expression of Kir2.1 channels contributed significantly to the shift of membrane potential from -12.2+/-2.8 to -57.3+/-3.7mV. However, biophysical and pharmacological properties of alpha(1G)-mediated Ca(2+) channels remained unaffected by the expression of Kir2.1 subunits, except for the enlarging of the window current region. Biochemical activation of alpha(1G) channels using 150mM KCl brought about an increase in [Ca(2+)](i), which was blocked by mibefradil, the T-type Ca(2+) channel blocker. These data suggest that the HEK293/alpha(1G)/Kir2.1 cell line would have potential uses in the study of T-type Ca(2)(+) channel-mediated signaling pathways and possibly useful in the development of new therapeutic drugs associated with T-type Ca(2)(+) channels.     

Kinetic control of multiple forms of Ca(2+) spikes by inositol trisphosphate in pancreatic acinar cells.

The mechanisms of agonist-induced Ca(2+) spikes have been investigated using a caged inositol 1,4,5-trisphosphate (IP(3)) and a low-affinity Ca(2+) indicator, BTC, in pancreatic acinar cells. Rapid photolysis of caged IP(3) was able to reproduce acetylcholine (ACh)-induced three forms of Ca(2+) spikes: local Ca(2+) spikes and submicromolar (<1 microM) and micromolar (1-15 microM) global Ca(2+) spikes (Ca(2+) waves). These observations indicate that subcellular gradients of IP(3) sensitivity underlie all forms of ACh-induced Ca(2+) spikes, and that the amplitude and extent of Ca(2+) spikes are determined by the concentration of IP(3). IP(3)-induced local Ca(2+) spikes exhibited similar time courses to those generated by ACh, supporting a role for Ca(2+)-induced Ca(2+) release in local Ca(2+) spikes. In contrast, IP(3)- induced global Ca(2+) spikes were consistently faster than those evoked with ACh at all concentrations of IP(3) and ACh, suggesting that production of IP(3) via phospholipase C was slow and limited the spread of the Ca(2+) spikes. Indeed, gradual photolysis of caged IP(3) reproduced ACh-induced slow Ca(2+) spikes. Thus, local and global Ca(2+) spikes involve distinct mechanisms, and the kinetics of global Ca(2+) spikes depends on that of IP(3) production particularly in those cells such as acinar cells where heterogeneity in IP(3) sensitivity plays critical role.