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. 2008 Aug;295(2):F568-84.
doi: 10.1152/ajprenal.00107.2008. Epub 2008 Jun 18.

Mechanisms underlying angiotensin II-induced calcium oscillations

Affiliations

Mechanisms underlying angiotensin II-induced calcium oscillations

Aurélie Edwards et al. Am J Physiol Renal Physiol. 2008 Aug.

Abstract

To gain insight into the mechanisms that underlie angiotensin II (ANG II)-induced cytoplasmic Ca2+ concentration ([Ca]cyt) oscillations in medullary pericytes, we expanded a prior model of ion fluxes. ANG II stimulation was simulated by doubling maximal inositol trisphosphate (IP3) production and imposing a 90% blockade of K+ channels. We investigated two configurations, one in which ryanodine receptors (RyR) and IP3 receptors (IP3R) occupy a common store and a second in which they reside on separate stores. Our results suggest that Ca2+ release from stores and import from the extracellular space are key determinants of oscillations because both raise [Ca] in subplasmalemmal spaces near RyR. When the Ca2+-induced Ca2+ release (CICR) threshold of RyR is exceeded, the ensuing Ca2+ release is limited by Ca2+ reuptake into stores and export across the plasmalemma. If sarco(endo)plasmic reticulum Ca2+-ATPase (SERCA) pumps do not remain saturated and sarcoplasmic reticulum Ca2+ stores are replenished, that phase is followed by a resumption of leak from internal stores that leads either to [Ca]cyt elevation below the CICR threshold (no oscillations) or to elevation above it (oscillations). Our model predicts that oscillations are more prone to occur when IP3R and RyR stores are separate because, in that case, Ca2+ released by RyR during CICR can enhance filling of adjacent IP3 stores to favor a high subsequent leak that generates further CICR events. Moreover, the existence or absence of oscillations depends on the set points of several parameters, so that biological variation might well explain the presence or absence of oscillations in individual pericytes.

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Figures

Fig. 1.
Fig. 1.
Schematic representation of the cell, with its 3 compartments: bulk cytosol (Cyt), microdomains (MD), and sarcoplasmic reticulum (SR). Not shown are KCa, Kir, KATP, and Kv channels and the chelating agents calmodulin and calsequestrin. A: common-store model. B: separate-store model.
Fig. 2.
Fig. 2.
Open probability (Po) of ryanodine receptors (RyR) and inositol trisphosphate receptors (IP3R) at steady state as a function of calcium concentration ([Ca], in M). In these calculations, [IP3] is taken as 240 nM.
Fig. 3.
Fig. 3.
Effects of external KCl elevation on Ca2+ concentrations in cytosol ([Ca]cyt, A), microdomains ([Ca]md, B), and SR ([Ca]SR, C) as a function of time (in s). For clarity of presentation, [K]out is raised from 5.4 to 100 mM at t = 100 s for the common-store model and at t = 120 s for the separate-store model. D: signaling pathway after external KCl elevation.
Fig. 4.
Fig. 4.
Effects of external KCl elevation on microdomain and cytosolic Ca2+ currents as a function of time (in s), using the separate-store model. At t = 120 s, [K]out is raised from 5.4 to 100 mM. A: IP3R current is low because of its inhibition by [Ca]md elevation while RyR current is large because of [Ca]md-mediated stimulation. B: [Ca]md elevation stimulates both IP3R store- and RyR store-sarco(endo)plasmic reticulum Ca2+-ATPase (SERCA) pumps facing the microdomains to the point that they become saturated. NCX, Na+/Ca2+ exchanger. C: the increase in IP3R-SR store Ca2+ leads to reversal of pumping by IP3R-SERCA that face the cytosol (negative values mean flux from the SR to the cytosol). The RyR-SERCA facing the cytosol take up Ca2+ from the cytosol into the RyR-SR store. D: the large increase in [Ca]SR-IP3R leads to elevation of Ca2+ current through those IP3R that face the cytosol, and the rise in [Ca]cyt stimulates elevation of current through the RyR that face the cytosol.
Fig. 5.
Fig. 5.
Effects of 90% and 75% K+ channel inhibition and 100% increase in IP3 production at t = 100 s on [Ca]cyt (A), [Ca]md (B), and [Ca]SR (C), with the common-store model.
Fig. 6.
Fig. 6.
Effects of 90% K+ channel inhibition and 100% increase in IP3 production at t = 100 s on microdomain (A) and cytosolic (B) Ca2+ currents, with the common-store model. The scale in B has been reduced for clarity; the cytosolic SERCA and voltage-operated Ca2+ (VOCa) currents peak at +73 and −103 pA, respectively.
Fig. 7.
Fig. 7.
Effects of 90% K+ channel inhibition and 100% increase in IP3 production at t = 100 s on Ca2+ concentrations in cytosol (A), microdomains (B), and SR stores (C), with the separate-store model. The additional effects of IP3R and RyR block on [Ca]cyt are shown in D.
Fig. 8.
Fig. 8.
Effects of 90% K+ channel inhibition and 100% increase in IP3 production at t = 100 s on [Ca]cyt (nM), [Ca]md (nM), and [Ca]SR (×102 mM), with the separate-store model. Note that the [Ca]md peak is off-scale. Phase A: RyR-mediated Ca2+-induced Ca2+ release (CICR) in microdomains, sharp [Ca]md ascent. Subsequent depletion of RyR stores and filling up of IP3R stores. Rapid membrane depolarization and repolarization, [Ca]cyt peak. Phase B: activation of NCX current, sharp [Ca]md descent. Ca2+ content in RyR and IP3R stores reaches minima and maxima. Phase C: slower [Ca]md descent. Subsequent replenishment of RyR stores and depletion of IP3R stores as IRyRmd and IIP3Rmd-SERCA decrease. Phase D: slowly rising RyR- and IP3R-mediated Ca2+ release into microdomains, progressive [Ca]md increase. Stabilized Ca2+ concentration in cytosol and SR stores.
Fig. 9.
Fig. 9.
Effects of 90% K+ channel inhibition and 100% increase in IP3 production at t = 100 s on microdomain and cytosolic Ca2+ currents, with the separate-store model. A: microdomain RyR current rises up to 60 pA during CICR, whereas microdomain IP3R current remains low because its inhibition by [Ca]md elevation. B: CICR-mediated [Ca]md increase stimulates IP3R store- and RyR store-SERCA pumps facing the microdomains, as well as Ca2+ export from the microdomains via NCX (minimal value, −14 pA). C: immediately after CICR, the IP3R-SERCA and RyR-SERCA that face the cytosol both take up Ca2+ from the cytosol to replenish SR stores. Soon thereafter, the increase in IP3R-SR store Ca2+ leads to reversal of pumping by IP3R-SERCA that face the cytosol. D: cytosolic IP3R current rises and falls in conjunction with [Ca]SR-IP3R. Cytosolic RyR current is stimulated during the depolarization-induced rise in [Ca]cyt.
Fig. 10.
Fig. 10.
Effects of 90% K+ channel inhibition and either 100% or 50% increase in IP3 production at t = 100 s on microdomain Ca2+ (A) and IP3 (B) concentrations, with the separate-store model. Note that the [Ca]md peak is off-scale.
Fig. 11.
Fig. 11.
Effects of parameter variations on the frequency (A) and amplitude (B) of oscillations induced by 90% K+ channel inhibition and 100% increase in IP3 production. Parameters are given relative to their baseline value. Results are obtained for the separate-store configuration. Oscillations persist when Ca2+ conductivity of IP3R (νIP3R) equals up to 18 times its baseline value.
Fig. 12.
Fig. 12.
A and B: frequency histograms of 2,062 spontaneous transient inward currents (STICs) recorded in 73 cells exposed to 10 nM ANG II (52). Most values are well below 1 Hz. The reason that the mean is 1.15 Hz is that a few frequencies are as high as 25, so that SD is very large and the mean is skewed away from the predominant frequency, near 0.09 Hz. C and D: amplitude histograms of the same data from Ref. . The predominant amplitude was near −10 pA, but the mean is much larger because of rare cells that exhibited large currents.
Fig. 13.
Fig. 13.
Predicted membrane current during voltage clamp at −80 mV and exposure to angiotensin II (ANG II), with the separate-store model. We assume that exposure to ANG II results in 90% K+ channel inhibition and 100% increase in IP3 production. A: current above cytosol. B: current above microdomains. C: overall current, calculated as the sum of the currents crossing the cytosol and the microdomains, and the leak current (taken as −8 pA, assuming a 10-GΩ seal).

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