ORIGINAL RESEARCH article
Three-Dimensional Model of Sub-Plasmalemmal Ca2+ Microdomains Evoked by T Cell Receptor/CD3 Complex Stimulation
- 1The Calcium Signalling Group, Department of Biochemistry and Molecular Cell Biology, University Medical Center Hamburg-Eppendorf, Hamburg, Germany
- 2Unit of Theoretical Chronobiology, Faculté des Sciences CP231, Université Libre de Bruxelles (ULB), Brussels, Belgium
Ca2+ signalling plays an essential role in T cell activation, which is a key step to start an adaptive immune response. During the transition from a quiescent to a fully activated state, Ca2+ microdomains of reduced spatial and temporal extents develop in the junctions between the plasma membrane and the endoplasmic reticulum (ER). These microdomains rely on Ca2+ entry from the extracellular medium, via the ORAI1/STIM1/STIM2 system that mediates store operated Ca2+ entry Store operated calcium entry. The mechanism leading to local store depletion and subsequent Ca2+ entry depends on the activation state of the cells. The initial, smaller microdomains are triggered by D-myo-inositol 1,4,5-trisphosphate (IP3) signalling in response to T cell adhesion. T cell receptor (TCR)/CD3 stimulation then initiates nicotinic acid adenine dinucleotide phosphate signalling, which activates ryanodine receptors (RYR). We have recently developed a mathematical model to elucidate the spatiotemporal Ca2+ dynamics of the microdomains triggered by IP3 signalling in response to T cell adhesion (Gil et al., 2021). This reaction-diffusion model describes the evolution of the cytosolic and endoplasmic reticulum Ca2+ concentrations in a three-dimensional ER-PM junction and was solved using COMSOL Multiphysics. Modelling predicted that adhesion-dependent microdomains result from the concerted activity of IP3 receptors and pre-formed ORAI1-STIM2 complexes. In the present study, we extend this model to include the role of RYRs rapidly after TCR/CD3 stimulation. The involvement of STIM1, which has a lower KD for Ca2+ than STIM2, is also considered. Detailed 3D spatio-temporal simulations show that these Ca2+ microdomains rely on the concerted opening of ∼7 RYRs that are simultaneously active in response to the increase in NAADP induced by T cell stimulation. Opening of these RYRs provoke a local depletion of ER Ca2+ that triggers Ca2+ flux through the ORAI1 channels. Simulations predict that RYRs are most probably located around the junction and that the increase in junctional Ca2+ concentration results from the combination between diffusion of Ca2+ released through the RYRs and Ca2+ entry through ORAI1 in the junction. The computational model moreover provides a tool allowing to investigate how Ca2+ microdomains occur, extend and interact in various states of T cell activation.
Calcium signaling plays a crucial role in the activation of T cells and the adaptative immune response. In particular, it controls transcriptional activation, proliferation, differentiation or secretion of cytokines (Feske, 2007; Trebak & Kinet, 2019). Increases of the free cytosolic Ca2+ concentration rely on Ca2+ release from the endoplasmic reticulum (ER) and on Ca2+ entry from the extracellular medium. Mobilization of internal Ca2+ follows the increase in d-myo-inositol 1,4,5-trisphosphate (IP3) and in nicotinic acid adenine dinucleotide phosphate (NAADP), via IP3 receptors (IP3R) and type 1 ryanodine receptor (RYR1), respectively (Streb et al., 1983; Wolf et al., 2015). Ca2+ entry relies on the ORAI/STIM system that allows Ca2+ entry in the cytosol, at a rate that is regulated by the concentration of Ca2+ in lumen of the ER (Putney, 2009). When Ca2+ dissociates from the Ca2+ sensors stromal interaction molecules 1 (STIM1) and 2 (STIM2) located in the ER membrane, STIM molecules aggregate and move to so-called “junctional spaces”. These regions correspond to the narrow cytosolic spaces between the ER and PM membranes, at locations where these membranes are separated by distances smaller than 20 nm. There, STIM molecules can recruit ORAI1 to form Ca2+ channels allowing Ca2+ to enter into the cytoplasm. This process is known as capacitative or store operated Ca2+ entry (SOCE). The relation between SOCE and ER Ca2+ concentration is nonlinear, with a KD for half activation of the order of 200 μM when it depends on the dissociation of Ca2+ from STIM1 and of 400 μM when it depends on the dissociation of Ca2+ from STIM2 (Stathopulos et al., 2006; Brandman et al., 2007; Luik et al., 2008).
Upon TCR/CD3 stimulation, second messengers create a substantial release of Ca2+ from the ER which, together with the resulting activation of SOCE, leads to a rise in the free cytosolic Ca2+ concentration in the whole T cell. This global Ca2+ increase contrasts with the locally restricted, sub-plasmalemmal Ca2+ increases of short duration (∼50 ms) that can be observed as a consequence of adhesive interactions (Weiss and Diercks, unpublished results), or in the first seconds following TCR/CD3 stimulation (Wolf et al., 2015; Diercks et al., 2018). The two types of events are known as Ca2+ microdomains and have similar spatio-temporal characteristics. Yet, they have different molecular origins. The adhesion dependent Ca2+ microdomains rely on a pathway involving focal adhesion kinase (FAK), phospholipase C (PLC) and IP3Rs (Weiss and Diercks, unpublished results). Due to IP3R-mediated Ca2+ release and subsequent SOCE, they also rely on ORAI1-mediated Ca2+ entry. Computational simulations of the interplay between ORAI1 and IP3R in a 3D configuration simulating an ER-PM junction have confirmed that the local depletion of ER Ca2+ created by the opening of a few IP3R can trigger the opening of ORAI1 in the junction, even in conditions of a full ER (Gil et al., 2021). Interestingly, these non-TCR/CD3 dependent Ca2+ microdomains require the existence of pre-formed complexes of ORAI1 and STIM2 that were demonstrated experimentally (Diercks et al., 2018). Ca2+ microdomains characterized by somewhat larger amplitude (340 ± 11 nM vs 290 ± 12 nM) are observed during the first ∼15 s following TCR/CD3 stimulation (Wolf et al., 2015; Diercks et al., 2018; reviewed in Guse et al., 2021). As the non-TCR/CD3 dependent microdomains, these signals also involve ORAI1, but in addition they require NAADP signaling and RYR1 dependent Ca2+ release from ER (Wolf et al., 2015; Diercks et al., 2018). As another difference, at this stage, pre-formed ORAI1/STIM complexes involve both STIM1 and STIM2 isoforms (Ahmad et al., 2021).
Ca2+ microdomains represent a crucial step for the successful activation of T cells. Reported durations of the signals triggered by cell adhesion and by formation of NAADP in the first seconds upon TCR/CD3 stimulation are 44 ± 4 ms and 64 ± 3 ms, respectively (Diercks et al., 2018). They extend on 0.216 ± 0.004 μm2. Because of these limited temporal and spatial extents, the investigation of Ca2+ microdomains is technically limited by the resolution of the microscopic imaging system used. The spatial and temporal resolution of the imaging system used to characterize T cell Ca2+ microdomains is approx. 368 nm and 20–25 ms, respectively (Wolf et al., 2015). Mathematical modelling thus represents a useful complementary tool to investigate their molecular origin, in the line of the numerous studies devoted to small scale Ca2+ events (Solovey et al., 2008; Swaminathan et al., 2009; Thul et al., 2009; Rückl & Rüdiger, 2016; Walker et al., 2017).
In a previous study (Gil et al., 2021), we adapted the realistic three-dimensional mathematical description of the ER-PM junction proposed by McIvor et al. (2018) to simulate adhesion-dependent Ca2+ microdomains arising in T cells. This model describes Ca2+ dynamics in a confined 3D configuration corresponding to a junctional cytosolic space and the adjacent sub-PM ER, taking into account Ca2+ influx through ORAI1 and IP3R, Ca2+ pumping into the ER through SERCA, and diffusion within the cytosolic and ER compartment. The IP3Rs are supposed to be located close to the junctional space (Thillaiappan et al., 2017). Simulations using COMSOL Multiphysics showed that the spontaneous activity of ∼3 IP3Rs create a local depletion of ER Ca2+ that suffices to trigger the opening of ORAI1 channels located in the junction and thus, the onset of a microdomain. Because of the presence of pre-formed complexes of ORAI1 and STIM2 in unstimulated cells, opening of ORAI1 indeed rapidly follows the dissociation of Ca2+ from STIM2. Predictions of this model are in agreement with recent observations in HEK293 cells reporting that constitutive STIM2 clusters in ER-PM junctions sense decreases in local ER Ca2+ mediated by IP3Rs (Ahmad et al., 2021). Moreover, IP3R channel activity near the junctions was shown to favour STIM2 clustering in the junction.
In this study, we modified our previous model of the T cell junctions to address the molecular mechanism that underlies the TCR/CD3-evoked and NAADP and RYR-dependent Ca2+ microdomains occurring in the first ∼15 s that follow TCR/CD3 stimulation. We first used modeling to find out whether RYR1 are located inside or around the ER-PM junctions. The analysis was based on comparisons between simulated and experimental results both in WT and ORAI1−/− T cells. The next issue related to the number of RYR1 involved in the formation of the junctional Ca2+ microdomains, which cannot be directly inferred from experimental observations. By contrast, modeling can determine the number of RYR1 that must open simultaneously to create the local depletion of ER Ca2+ triggering the appropriate level of SOCE activation. Conclusions about this number were next validated by an independent estimation of the increase in the RYR1 open probability triggered by the NAADP formation in TCR/CD3 stimulated T cells. Finally, we took advantage of the great flexibility provided by computational modeling to investigate the respective roles played by the ER Ca2+ channels (IP3R or RYR) and the Ca2+ sensors (STIM1 and STIM2) in shaping the characteristics of the Ca2+ microdomains created by the openings of the related ORAI1 channels. This analysis allowed us to propose a unifying description of the molecular mechanism underlying T cells Ca2+ microdomains from adhesion to early TCR/CD3 stimulation.
Description of the Mathematical Model
Because the model was fully described in Gil et al. (2020), we provide a concise description of its main features in this section. The spatial geometry is shown in Figure 1. The junction is a 15 nm-wide (Wu et al., 2006; Hogan, 2015) three-dimensional space between the PM and an ER portion located close to it. The junction communicates with the adjacent cytoplasm, a portion of which is modelled explicitly. The free cytosolic Ca2+ concentration, defined by CC, is initially set at 30 nM (Diercks et al., 2018). In the rest of the cytoplasm, which is not modelled explicitly, CC is fixed at this same value. Similarly, the evolution of ER Ca2+ concentration (CS) is simulated in the sub-PM ER, which is in contact with the bulk of the ER where Ca2+ concentration is fixed at 400 μM (Lewis, 2011). The PM portion located in the junction contains five ORAI channels and the ER membrane, 10 SERCA and nine RYR1s as reported (Hogan, 2015; McIvor et al., 2018; Jayasinghe et al., 2018; Yin et al., 2008). Seen from above (Figure 1C), SERCA pumps form a ring surrounding ORAI1 channels and RYR1s are arranged on a square lattice. Given the large size of these channels (Lanner et al., 2010), the 31 nm distance between the pores of the channels considered in Figure 1 corresponds to a close packing of RYR1.
FIGURE 1. Schematic representation of the model geometry of the ER-PM junction and sub-PM ER used to investigate the origin of the Ca2+ microdomains in T cells with nine RYR1 inside the junction (A) Frontal diagram showing the dimensions of the cone that represents the sub-PM ER, of the junction and of the portion of the cytosol considered in the simulations. ORAI1 channels are in blue, SERCA pumps in orange and RYR1 in green. Plain lines represent membrane boundaries; dashed lines, fictitious limits between the junction and the cytosol and double lines indicate the limits of the simulated system. The resting Ca2+ concentrations considered as initial conditions and boundary conditions in the two compartments are indicated. (B) 3D view of the model geometry (C) Upper view of the positions of the ORAI1 channels on the PM, in blue, and of the SERCA pumps and RYR1 (in a chessboard manner) on the ERM, in orange and green respectively. Not to scale. This geometry is based on McIvor et al. (2018). See text for details.
Membranes, schematized as simple full lines in Figure 1A, correspond to no flux boundary conditions, except across channels and pumps where corresponding fluxes are simulated. The flux through ORAI channels is given by
with IORAI the maximal single channel current, F the Faraday constant, z the charge of a Ca2+ ion and AO the surface of the channel pore.
In the ER membrane, Ca2+ flux from the ER to the cytosol through the RYR is given by
with IRYR the current through the RYR, which takes the value of 0.35 pA (Guo et al., 2012). ARYR is the surface of the channel pore. The second factor in Eq. (2) allows to scale the current to take the actual gradient across the channel pore into account, where CS,0 and CC,0 represent resting concentrations of Ca2+ in the ER and in the cytosol (Mazel et al., 2009).
Finally, SERCA pumps are considered as bidirectional as in McIvor et al. (2018) and described by
with Vmax its maximal velocity, n2 the Hill coefficient and KF and KR the pump affinity for cytosolic (CC) and ER (CS) calcium, respectively. As is the surface of the pore and Q is a temperature coefficient initially introduced by McIvor et al. (2018). To approximate the partial differential equations (PDE), we used the finite element method (FEM) and simulation software COMSOL Multiphysics 5.5 (http://www.comsol.com), more specifically the Transport of Diluted Species interface that is used to compute the concentration field of a dilute solute in a solvent. We chose a backward differentiation formula (BDF) to compute the time steps with a relative tolerance of 0.005 that controls the relative error in each step. The system is solved using the iterative linear solver GMRES (Generalized Minimum Residual). For further details regarding the system discretization and the use of COMSOL Multiphysics, please refer to the authors.
Ca2+ Microdomains Simulated by the Opening of Type 1 Ryanodine Receptors Localized in the ER-PM Junction do Not Rely on ORAI1 Opening
Upon TCR/CD3 stimulation, NAADP-evoked Ca2+ release through RYR1 acts in concert with Ca2+ entry through ORAI1/STIM complexes to create Ca2+ microdomains. These microdomains last for 64 ± 3 ms and reach amplitudes of 340 ± 11 nM (Diercks et al., 2018). Although it is known that ORAI1 and STIM are arranged in pre-formed complexes in the ER-PM junctions of T cells, the exact location of the RYR1s responsible for the decrease in [Ca2+]ER in the sub-PM ER remains to be determined. As described in the presentation of the model and schematized in Figure 1, in the model we first considered that RYR1s are located in the junction, facing the PM as in cardiac dyadic clefts (Jones et al., 2018). In this section, we evaluated if this arrangement allows to reproduce experimental observations.
We simulated the junction schematized in Figure 1 considering an increasing number of open RYR1s during 64 ms. A few milliseconds after RYR1 opening, a stable profile of Ca2+ increase in the junction is observed (Figures 2A–F, Supplementary Figure S2). Although Cc can locally reach concentrations close to 20 μM, the average Ca2+ concentration in the junction ranges from 340 to 2,500 nM depending on the number of open RYR1 (Anim. S1a,b in the Supplementary Information). Thus, in this configuration, opening of a single RYR1 allows to reach the experimentally observed microdomain amplitude in the junction. To assess the relative contributions of Ca2+ entry through ORAI1 and Ca2+ release from the ER through RYR1, we performed the same simulations in the absence of ORAI1 in the PM. As visible in Figure 2H in which Ca2+ microdomains with and without activated ORAI1 are seen to have nearly the same amplitude, the relative contribution of Ca2+ entry is very limited in these conditions. In agreement with this observation, the increase in the amplitude of the Ca2+ signal in the microdomain is not related to significant changes in the opening states of ORAI1 (Figure 2I). For example, when three RYR1s open simultaneously, all five ORAI1 channels are still in their lower state of activity as in the absence of any RYR1 opening. These computational observations indicate that the geometry depicted in Figure 1 does not reflect the situation encountered in T-lymphocytes early after TCR activation, since the number of microdomains decreases significantly in ORAI1−/− T cells (Diercks et al., 2018).
FIGURE 2. Simulated Ca2+ microdomains resulting from the opening of RYR1 inside the junctions, which in turn induces the opening of ORAI1 channels in the junctions as a result of local depletion of ER Ca2+ (A) Upper view of the arrangement of the ORAI1 channels on the PM of the junction (yellow dots) and of the RYR1 on the ERM (red dots) using COMSOL (B–F) Steady-state Ca2+ profiles in the junction when opening 1, 2, 4, 6 and 9 RYR1 simultaneously (B) to (F) respectively. Shown are the profiles 22 ms after opening of the RYR1, but these stabilize very rapidly, after a few ms (G) Extended colour code with marking of the average amplitude of a microdomain in unstimulated T cells (Diercks et al., 2018) (H) Evolution of the amplitude of the simulated Ca2+ microdomains with the number of simultaneously open RYR1 in the junction, showing that experimentally observed microdomains do not agree with the opening of the RYRs inside the junction given the low contribution of the opening of the ORAI1 in conditions of a full ER (see text). Dotted line represents junctional Ca2+ concentration reached in the absence of ORAI1 channels (I) Individual evolution of 1–5 ORAI1 channels open state (Li et al., 2011) as a result of 0–9 RYR1 opening simultaneously. See Supplementary Information and Anim. S1a,b for details.
Ca2+ Microdomains Observed Soon After T Cell Stimulation Are due to the Opening of Type 1 Ryanodine Receptors Localized on Conic ER Around the ER-PM Junction
Because of the small size of the junction, actual Ca2+ concentrations are expected to be highly sensitive to the ER-PM distance. Thus, results obtained in the previous section may depend on this junctional depth, which led us to investigate the influence of this distance on the Ca2+ profile in the junction. Data indicate that the ER-PM spacing is typically 10–20 nm (Hogan, 2015), but we investigated distances up to 50 nm that might be reached locally. As visible in Figure 3, although the amplitude of the Ca2+ microdomain is inversely proportional to the height of the junction, the experimental average is reached with less than three RYR1 simultaneously open even for the largest junction considered (50 nm). Moreover, the amplitudes are not much affected by the absence of ORAI1, as visible by the fact that the Ca2+ microdomain amplitudes without ORAI1 (dashed lines) are close to those with ORAI1 (plain lines). This does not agree with experimental observations showing that in cells that do not express ORAI1, the frequency of occurrence of junctional microdomains is reduced by ∼10, while their amplitude is lowered by ∼25% (Diercks et al., 2018). We thus concluded that RYR1 located inside the junction, whatever its height, cannot account for experimental observations.
FIGURE 3. Influence of the value of the distance between the PM and the ERM on the Ca2+ microdomains in the ER-PM junction. The green curve (15 nm) corresponds to the situation considered in Figure 2. Larger distances, blue curve (30 nm) and orange curve (50 nm) do not influence the low contribution of the opening of the ORAI1 to the Ca2+ concentration increase in the junction. Dotted lines represent junctional Ca2+ concentration reached in the absence of ORAI1 channels.
Another possibility would be that RYR1s are located outside the junction, but close to it, in such a way that they affect sub-PM ER Ca2+ concentration. Thillaiappan et al. (2017) reported clusters of immobile IP3Rs surrounding the ER-PM junctions, with the mouths of the IP3Rs directed towards the PM. In our previous computational study of the IP3R-dependent, adhesion-induced Ca2+ microdomains, we found that simulations based on this configuration agree with experimental observations (Gil et al., 2021). We investigated the possibility that RYR1s are similarly localized around the junction. In this configuration, schematized in Figure 4, a ring of RYR1s located in the sub-PM ER membrane and spaced by 90 nm, are releasing Ca2+ in the cytosolic space adjacent to the junction. The Ca2+ microdomains simulated under this configuration are shown in Figure 5, considering 1 (Figure 5B, Supplementary Figure S2) to 8 (Figure 5I) open RYR1. To reach the experimentally observed average amplitude of around 340 nM, seven or eight RYR1 must open simultaneously (Figure 5J). This number is slightly affected by the distance between the RYR1 and the junction. If a 45 nm distance is considered, instead of 90 nm as considered in Figure 5, opening of five RYR1s simultaneously is sufficient to reach the experimentally observed amplitude in the junction (Supplementary Figure S4). Indeed, a larger amount of the Ca2+ released by RYR1 can diffuse into the junction in this configuration. In the absence of ORAI1, the increase in Ca2+ in the junction due to RYR1 opening is much below the experimentally observed amplitude of the microdomains. Thus, when the RYR1 located in the membrane of the sub-PM ER are not releasing Ca2+ directly in the junctions, the model reproduces the experimental observation that NAADP-induced Ca2+ microdomains rely on both RYR1 and ORAI1 (Diercks et al., 2018).
FIGURE 4. Schematic representation of the model geometry of the ER-PM junction and sub-PM ER used to investigate the origin of the Ca2+ microdomains in T cells with eight RYR1 around the junction (A) Frontal diagram showing the dimensions of the cone that represents the sub-PM ER, of the junction and of the portion of the cytosol considered in the simulations. ORAI1 channels are in blue, SERCA pumps in orange and RYR1 in green. Plain lines represent membrane boundaries; dashed lines, fictitious limits between the junction and the cytosol and double lines indicate the limits of the simulated system. The resting Ca2+ concentrations considered as initial conditions and boundary conditions in the two compartments are indicated. (B) 3D view of the model geometry (C) Upper view of the positions of the ORAI1 channels on the PM, in blue, and of the SERCA pumps and RYR1 on the ERM, in orange and green respectively. Not to scale. This geometry is based on McIvor et al. (2018). See text for details.
FIGURE 5. Simulated Ca2+ microdomains resulting from the opening of the RYR1 adjacent to the junctions, which in turn induces the opening of ORAI1 channels in the junctions as a result of local depletion of ER Ca2+ (A) Upper view of the arrangement of the ORAI1 channels on the PM of the junction (red dots) and of the adjacent RYR1 (yellow lines) using COMSOL (B–I) Steady-state Ca2+ profiles in the junction when opening 1 (B) to 8 (I) RYR1 simultaneously. Shown are the profiles 22 ms after opening of the RYR1. Upon depletion of local Ca2+ in the ER, which is quasi-instantaneous, ORAI1 channels open to an extent that depends on this local concentration, as defined by the function f2/1 (see Supplementary Information). ORAI1 opening is assumed to occur immediately after depletion because ORAI1-STIM1/2 aggregates are pre-formed (Weiss and Diercks, unpublished results). (J) Evolution of the amplitude of the simulated Ca2+ microdomains with the number of simultaneously open RYR1 in the junction, showing that experimentally observed microdomains can in principle result from the opening of ORAI1 channels induced by the spontaneous opening of a few RYR1 near the junction, in conditions of a full ER. Dotted line represents junctional Ca2+ concentration reached in the absence of ORAI1 channels. See Anim. S2a,b,c,d and S3 in Supplementary Information.
Observations in T cells indicate that Ca2+ signals in the junction are rather stereotypic, with a relatively constant amplitude (Diercks et al., 2018). It is thus expected that the microdomain characteristics are not very sensitive to the numbers of RYR1 present around the junction. We next investigated the influence of the number of open RYR1 in more detail, considering the possibility that up to 16 RYR1 are located around the junction. This was done in the simulations by considering another ring of eight receptors 90 nm below the first one. As visible in Figure 6A, the relation between the amplitude of the simulated microdomains and the number of open RYR1 is non-linear with a marked stepwise behaviour. From one to three open RYR1, the increase in amplitude is linear. All five STIM1/2 bound ORAI1 channels are in their lowest conductance state (Figure 6B) and the Ca2+ increase in the junction is due to diffusion from the adjacent cytosol. From four open RYR1 on, local ER Ca2+ depletion is sufficient to further activate ORAI1 creating changes in the slope of the relation between the amplitude of the Ca2+ signal and the number of open receptors. If more than eight RYR1 open simultaneously, additional ones do not activate ORAI1 further. As seen in Supplementary Figure S1, the 54% opening state is reached when the value of CS in the close vicinity of STIM1/2 bound to ORAI1 reaches 260 μM. This would require a Ca2+ decrease at the ER lumen close to RYR1 channel that is not reached under localised Ca2+ signaling because of fast diffusion-mediated replenishment. From 8 to 16 open RYR1, local depletion is not much affected, with a minimal ER Ca2+ concentration that remains around 340 μM as visible in Figure 7 that shows a cross-sectional view of the Ca2+ concentrations in the sub-PM ER and in the cytoplasmic space including the junction (see also Supplementary Figure S3 for cross-sections). Noticeably, Ca2+ concentrations at the cytosolic side of RYR1 slightly decrease with the number of open receptors, from 17.5 to 15.9 μM for 2 and 16 open receptors, respectively. The slight decrease in the Ca2+ gradient at the channel pore indeed reduces the flux through the RYR1. Thus, increasing the number of RYR1 leads to a decrease in the ER Ca2+ concentration around STIM1/2, but this decrease is not sufficient to provoke the passage of ORAI1 channels to a higher conductance state. NAADP-induced Ca2+ microdomains observed early after T cell stimulation thus rely on the simultaneous opening of an average of seven–eight RYR1 located around the ER-PM junction.
FIGURE 6. Simulated Ca2+ microdomains resulting from the opening of up to 16 RYR1 adjacent to the junctions (A) Evolution of the amplitude of the simulated Ca2+ microdomains in the presence (green curve) and in the absence of ORAI1s (dotted green curve) in the junction. Both green curves, up to eight simultaneously open RYR1, correspond to the situation considered in Figure 5. The theoretical situation of a junction that does not contain ORAI1 channels (dotted green curve) allows to appreciate that the contribution of Ca2+ released through the RYR1 to the Ca2+ microdomain is linear and rather limited. At eight simultaneously open RYR1 (green curve), the complete cluster of five ORAI1 channels reach their maximum open state possible, in conditions of a full ER (B) Individual evolution of 1–5 ORAI1 channels open state (Li et al., 2011) as a result of 1–16 RYR1 opening simultaneously. See Supplementary Information for details.
FIGURE 7. Cross-section of the Ca2+ profiles in the junction, in the cytosol adjacent to the junction and in the sub-PM ER during microdomain formation (A–D) microdomains created by the opening of 2, 4, 6 and 8 RYR1. Local depletion of ER Ca2+ provokes the opening of the nearby ORAI1s. This situation corresponds to the one shown in Figure 5. (E,F) microdomains created by the opening of 12 and 16 RYR1, respectively. The second cluster of eight RYR1 is located directly underneath the first cluster. Local depletion of ER Ca2+ is not enough to provoke additional opening of the nearby ORAI1s. This situation corresponds to the one shown in Figure 6. For all panels, the upper right bar indicates the colour code of Ca2+ concentration in the cytosol while the lower right bar indicates the colour code of Ca2+ concentration in the ER. See Anim. S4.
Predicted Type 1 Ryanodine Receptors Involvement in the Formation of Microdomains Agree With Type 1 Ryanodine Receptors Open Probabilities in the Presence of NAADP
Simulation results obtained in the previous section indicate that best agreement between modelled and experimentally observed microdomains occur when most of the eight RYR1 located near the preformed ORAI1/STIM1/STIM2 complexes are open simultaneously during 64 ms. This conclusion stems from a direct comparison between the simulated and experimentally observed Ca2+ signals. To further validate this result, some reasoning based on RYR1 open probability can be proposed. The 64 ms duration of a Ca2+ microdomain corresponds to the average duration of the NAADP-evoked Ca2+ signals arising in the first 15 s after TCR activation (Diercks et al., 2018). Interestingly, 64 ms also fits in the range of the reported durations of Ca2+ sparks (Jaggar et al., 2000). It is thus likely that in response to the TCR/CD3 stimulation-induced NAADP increase, RYR1 undergo repetitive openings maintained by Ca2+-induced Ca2+-release, a process that generates a small amplitude Ca2+ increase in the cytosol, called “spark”. The decrease of ER Ca2+ that accompanies the spark is in turn responsible for the opening of ORAI1, and thus for the Ca2+ microdomain in the junction.
We thus investigated if our conclusions about the molecular mechanism underlying TCR/CD3-induced Ca2+ microdomains are compatible with the dynamics of RYR1 during spark-like activity. Upon TCR/CD3 stimulation, global NAADP concentration in T cells increases from 4.1 ± 1.5 nM to 33.6 ± 7.2 nM (Gasser et al., 2006). Because RYR1 are activated by NAADP in T cells (Wolf et al., 2015; Diercks et al., 2018; Roggenkamp et al., 2021), their Ca2+-releasing activity will increase. Indeed, Hohenegger et al. (2002) have shown that the open probability of these receptors is a highly nonlinear function of NAADP concentration, with an EC50 of 31.2 ± 6.9 nM. Because NAADP synthesis occurs near the ER-PM junctions (Gu et al., 2021), local concentrations in the vicinity of RYR1 are certainly larger than the average values mentioned above and likely exceed the EC50. Thus, the open probability of RYR1 near the junctions must be of the order of 0.7, which is the maximal value measured at 20 μM Ca2+. Given that the mean open time of RYR1 is ∼2 ms (des Georges et al., 2016; Sato & Bers, 2011), the mean closed time in these conditions can be estimated to be 0.86 ms. On the basis of these data, one can obtain a rough approximation of the number of simultaneously open receptors in a spark site when RYR1s are maximally activated by NAADP. Straightforward stochastic simulations of opening and closing of eight RYR1 with average opening and closing times equal to 2 and 0.86 ms, respectively, indicate that most of the time, six receptors are simultaneously open (Figure 8A). This result was obtained by performing 64 ms long stochastic simulations of eight independent RYR1 and determining at each time step how many receptors are open. The maximal frequency at six open receptors is in accordance with the three-dimensional spatio-temporal simulations indicating that best agreement between experimental observations and computational results is obtained when seven to eight RYR1 are simultaneously open during a 64 ms Ca2+ spark, considering the existence of pre-formed STIM1/2 and ORAI1 complexes (Figure 5). In contrast, the same calculations predict that for basal NAADP concentrations, when the open probability of RYR1 equals 0.4, the highest frequency corresponds to three RYR1 open simultaneously (Figure 8B). In the above simulations (Figure 5), this corresponds to a Ca2+ microdomain with an amplitude well below the experimental average. Similar stochastic simulations (Supplementary Figure S5 and related text in the SI) indicate that for the IP3-mediated microdomains corresponding to pre-stimulation conditions, the maximal frequency corresponds to two receptors open simultaneously, in qualitative agreement with our previous results (Gil et al., 2021).
FIGURE 8. Frequency of simultaneously open receptors in a cluster of eight RYR1 during 64 ms that corresponds to the duration of a Ca2+ spark (A) During a spark when RYR1 are maximally activated by NAADP, there are most of the time around five to six simultaneously open RYR1, with a single receptor open probability of 0.7 (Hohenegger et al., 2002). This is in agreement with the results seen in Figure 5. (B) At basal NAADP concentration, the single receptor open probability is around 0.4, and there are continuously around three to four simultaneously open RYR1, which is not enough to reach the experimental Ca2+ amplitude. In the two panels, the stochastic simulations of opening and closing of individual receptors are performed during 64 ms.
In summary, by combining previous observations about NAADP increase upon TCR/CD3 stimulation of T cells and RYR1 open probability, we conclude that the NAADP-induced increase in the open probability of RYR1 triggers the opening of most of the eight RYR1 located around the ER-PM junction. This is in agreement with the spatio-temporal simulations shown in the previous section, which indicate that Ca2+ microdomains observed early after T cell stimulations rely on the simultaneous opening of seven to eight RYR1 located around the junction.
The Isoforms of STIM That Are Bound to ORAI1 Determine the Characteristics of the Ca2+ Microdomains
In the previous sections, we found that the microdomains occurring during the first 15 s after TCR/CD3 stimulation involve a larger number of ER Ca2+ releasing channels than those observed before stimulation. Indeed, the local depletion induced by the opening of six–seven RYR1 is needed to activate ORAI1 and reproduce experimentally observed NAADP-dependent microdomains (Figure 5) while three to six IP3R are involved in the creation of the adhesion-mediated, IP3-dependent microdomains (Gil et al., 2021). At first sight, this is paradoxical as the conductance of RYR1 is about 5 times larger than that of IP3Rs.
We thus studied the characteristics of the Ca2+ increases created by the simultaneous opening of either eight IP3Rs or eight RYR1 (see Table 1). For the two Ca2+ channel types, we considered two possible preformed ORAI1/STIM complexes: STIM2 homotetramers (STIM2/2) and STIM1 and STIM2 heterotetramers (STIM1/2). Simulation results indicate that the nature of the ER Ca2+ release channel does not much influence the characteristics of the Ca2+ microdomains. Indeed, the Ca2+ signal in the junction is determined by the opening state of ORAI1, which is the same when Ca2+ release from the ER is mediated by IP3Rs or RYR1. The Ca2+ concentration sensed by the ORAI1/STIM complex is nearly the same in the two situations. As shown in Figure 9C, once the steady state gradients are established, the fluxes are nearly identical. Because of the slow replenishment around the pore of the receptor channel with DS = 10 μm2/s, the concentration gradient around the two extremities of the pore does not changes drastically and hence the flux remains of the same order for IP3R and RYR1. In contrast, the nature of the STIM isoforms bound to ORAI1 has a drastic influence on the characteristics of the Ca2+ microdomain since it determines their Ca2+ sensitivity, and hence the opening state of ORAI1. Because STIM1/2 has a lower sensitivity to ER Ca2+ depletion than STIM2/2, the open state of ORAI1 is lower and the increase in Ca2+ in the junction has both a smaller amplitude and spatial extent (compare blue to green lines in Figure 9A,B to Figure 6B and Table 1).
TABLE 1. Characteristics of the simulated microdomains relying on the simultaneous opening of eight IP3Rs for 44 ms (first two lines) or of eight RYR1 for 64 ms (lines three and 4). For each case, two situations are considered: the existence of pre-formed clusters of ORAI1 with STIM2/2 homotetramers (lines 1 and 3) and the existence of pre-formed clusters of ORAI1 with STIM2/1 heterotetramers (lines two and 4). Maximal concentrations denote the maximal local concentrations reached in the domains indicated. Spatial extent refers to the area of the junction’s portion in which Ca2+ concentration exceeds 300 μM. The ER [Ca2+] felt by ORAI is the average local concentration of luminal Ca2+ around the mouth of the IP3R or RYR1, computed in a 108 nm3 volume.
FIGURE 9. Influence of the nature of the ER Ca2+ channel inducing the local depletion of ER Ca2+ (IP3R or RYR1) and of the STIM isoforms bound to ORAI1 on the characteristics of Ca2+ microdomains (A) Evolution of Ca2+ microdomains amplitude with the number of simultaneously open RYR1 in the junction. The microdomains observed in conditions of full ER can be induced by the spontaneous opening of a few RYR1 near the junction that in turn trigger the opening of ORAI1 channels bound to STIM2/2 (blue curve) or to STIM1/2 (green curve). ORAI1 channels open to an extent that depends on local ER Ca2+ concentration, as defined by the corresponding function f2 or f2/1 (see Supplementary Information) (B) Individual evolution between the 5 open states of the ORAI1 (Li et al., 2011), as a result of 1–8 RYR1 opening simultaneously. (C) Comparison of Ca2+ fluxes through open IP3Rs and RYR1. Because of the slow replenishment around the pore of the receptor channel with DS = 10 μm2/s, the concentration gradient around the two extremities of the pore does not changes drastically and hence the flux remains of the same order for IP3Rs and RYR1.
Based on these computational observations, the prototypical evolution of Ca2+ microdomains from adherent to TCR/CD3 stimulated T cells is proposed to obey the following scenario. Upon adhesion to proteins of the extracellular matrix, integrin evoked IP3 signaling provokes an increase in the frequency of Ca2+ puffs arising from the clusters of IP3R located near the ER/PM junction. These puffs typically last ∼44 ms during which, in average, two IP3Rs are open simultaneously. On the other hand, five ORAI1 channels are located in the PM of the junction and bound to STIM2/2 homotetramers. In response to the decrease in ER Ca2+ created by the puff, the ORAI1 channels open to ∼21% of their maximal conductance and create the Ca2+ microdomain (Figures 10A, 1st row of Table 2). After the Ca2+ puff, Ca2+ is rapidly replenished in the sub-PM ER and ORAI1 channels shift to their lowest conductance state (∼7% opening) that corresponds to basal Ca2+ entry, but not to a detectable Ca2+ microdomain (Figure 10B, 2nd row of Table 2) when bound to the STIM1/2 isoform, and stay at 21% when bound to STIM2/2. TCR/CD3 stimulation initiates NAADP signaling, which increases the open probability of the RYR1 located around the junction and thus the frequency of Ca2+ sparks (Figure 10C, 3rd row of Table 2). During these events, ∼6 RYR1 are open simultaneously. At this stage, ORAI1 channels are preferably bound to STIM1/2 heterotetramers, which decreases their sensitivity to ER Ca2+ depletion. Thus, as in the case of the IP3-dependent microdomains, they open at ∼21% of their full capacity. However, because more Ca2+ is released in the cytosolic space just around the junction by six RYR1 than by two IP3R, the Ca2+ microdomain in the junction is a bit larger because of diffusion.
FIGURE 10. Simulated most probable Ca2+ microdomains resulting from a T cell transition between quiescent to early activation. (A) Non TCR/CD3-dependent Ca2+ microdomains formed by the opening of two IP3Rs adjacent to the junction and further opening of ORAI1 channels bound to STIM2/2 (B) Basal opening of five ORAI1 channels, one inherently co-localized with STIM2/2 and four inherently co-localized with STIM1/2 leading to small microdomains arising from nano-scale [Ca2+] fluctuations in the sub-PM ER. Artificial construction (C) TCR/CD3-dependent Ca2+ microdomains formed by the opening of six RYR1 adjacent to the junction and further opening of ORAI1 channels bound to STIM1/2. See Anim. S5a,b,c in the Supplementary Information. (D) Ca2+ profiles along the yellow dotted line shown in A that traverses the middle of the junction at a 7.5 nm distance from the PM, corresponding to panels A, B and C.
TABLE 2. Characteristics of the simulated microdomains corresponding to IP3-dependent Ca2+ signaling stimulated by T cell adhesion (line 1), to a spontaneous opening of ORAI in the absence of stimulation (line 2) or to NAADP-dependent Ca2+ signaling in response to TCR/CD3 stimulation (line 3)
Activation of T cells is an essential step to start an adaptive immune response. At this particular point a highly important decision is made: whether a T cell stays quiescent or may develop into an effector T cell carrying out immune effector functions to destroy pathogens, or in case of autoimmune reactions, to attack our own body. Among several signaling processes involved, Ca2+ signaling is fundamental for T cell activation. In a previous study, we resorted to mathematical modeling to gain insight into the early, small scale Ca2+ increases that follow adhesive interactions of T cells, which play a crucial role in T cell migration to inflamed tissue (Weiss and Diercks, unpublished results; Mezu-Ndubuisi & Maheshwari, 2021). Here, we extend this model to investigate the molecular mechanism underlying the early phase of activation following TCR/CD3 stimulation. Although both types of Ca2+ microdomains largely rely on Ca2+ entry through preformed ORAI1/STIM complexes, the former response relies on IP3 signaling while the latter involves NAADP and RYRs. Interestingly, a progressive change in STIM isoforms, from mainly STIM2 homotetramers to STIM1/2 heterotetramers, also accompanies this transition (Figure 11). Computational modeling of the spatio-temporal Ca2+ dynamics in the ER-PM junctions allowed us to reproduce the observation that the microdomains triggered by cell adhesion or by TCR/CD3 stimulation at its early phase appear rather similar, despite the different underlying mechanisms.
FIGURE 11. Schematized representation of the proposed mechanism underlying the spontaneous formation of Ca2+ microdomains in T cells during its transition from quiescent to early activation (A) In an otherwise unstimulated cell, non TCR/CD3 dependent short, spontaneous activation of one or a few IP3Rs close to the junction, releases Ca2+ from the sub-PM ER into the cytosol, leading to further opening of ORAI1 channels most likely bound to STIM2/2 at this stage (Weiss and Diercks, unpublished results) (B) During the first 15 s following TCR/CD3 stimulation, and NAADP driven activation of several RYR1 close to the junction, slightly larger amount of Ca2+ is released from the sub-PM ER into the cytosol. The resulting local Ca2+ depletion close to the RYR1 pore provokes the unbinding of Ca2+ from STIM1/2 heterotetramers, which further activates ORAI1 channels (Diercks et al., 2018). Red spots represent Ca2+ ions.
Simulations of the NAADP dependent microdomains quite forwardly predict that RYR1 are most probably located outside the junction, in a region of the ER membrane that is directly adjacent to the junction. This view contrasts with the well-known arrangement of RYR2 in cardiac cells, where they are facing the PM in dyadic clefts (Jones et al., 2018). In principle, a few RYR1 could be located in the ER-PM junction of T cells because the dimensions of its cytoplasmic part (approx. 28 nm × 28 nm × 12 nm, see Lanner et al., 2010) do not exceed the dimensions of the junction. However, Ca2+ microdomains simulated with such a spatial arrangement are no longer dependent on ORAI1, since the increase in Ca2+ concentration due to the influx mediated by a single RYR into the junction suffices to create a Ca2+ signal of the amplitude observed experimentally, which does not agree with experimental results. It is thus most probable that in T cells RYR1 are arranged around the junction, in the same way as IP3R (Thillaiappan et al., 2017; Taylor and Machaca, 2019).
Computational results indicate that the influx through ORAI1 channels much depends on the STIM isoforms to which it is bound. In the case of local signaling investigated here, the same opening state of ORAI1 is reached after local Ca2+ depletion induced by three IP3R when it is bound to STIM2/2 as after local Ca2+ depletion induced by seven RYR1 when it is bound to STIM1/2. Thus, the change in the nature of the ORAI1/STIM complexes that follow TCR/CD3 stimulation is expected to play a crucial role in maintaining Ca2+ signaling localized despite the stimulation of RYR by NAADP. Along this line, Ahmad et al. (2021) have recently shown in HEK293 cells that while clusters of STIM2 represent the sites of SOCE initiation, STIM1 molecules are progressively recruited when cells are exposed to low stimulation.
In contrast, the nature of the ER-releasing Ca2+ channel that creates the local depletion in the sub-PM ER, subsequently triggering ORAI1 opening does not have a significant effect. This result is a priori surprising given that the RYR1 has a conductance ∼5 times larger than the IP3R. Simulations indicate that the flux is limited by the replenishment of ER Ca2+ at the mouth of the channel rather than by its conductance. Thus, the extent of local depletion is imposed by the value of the diffusion coefficient of Ca2+ in the ER. This computational observation agrees with the major role played by intraluminal diffusion of Ca2+ in setting the responsiveness of Purkinje cells to synaptic inputs (Okubo et al., 2015). It should be kept in mind that the peculiar geometry of the junctional ER is expected to play an important role in decreasing the value of the effective Ca2+ diffusion coefficient because of the tortuosity of the tubular network of the ER (Schaff et al., 1997; Oloveczky and Verkman, 1998). In our simulations, diffusion is however fast enough to avoid decreases in local ER Ca2+ that would trigger the passage of ORAI1 channels in a highly active state. Simulations indicate that during localized Ca2+ signaling in T cells, ORAI1 channels never exceed 21% of their maximal activity.
Together with experimental observations (Diercks et al., 2018; Weiss and Diercks, unpublished results), our computational model ascribes the evolution of Ca2+ microdomains from the adherent/pre-stimulated to the TCR/CD3 early stimulated state as a passage from puff-to spark-triggered SOCE. Indeed, while the two types of localized Ca2+ signaling rely on ORAI1-mediated Ca2+ entry, cell adhesion triggers the synthesis of IP3, and TCR/CD3 stimulation initially that of NAADP. The respective durations of the two types of Ca2+ microdomains (44 ± 4 ms and 64 ± 3 ms) are in the ranges of those reported for puffs (Bootman et al., 1997) and sparks (Jaggar et al., 2000), respectively. In the two cases, the local depletion in ER Ca2+ created by the puff or the spark can trigger ORAI1 opening, with a resulting simulated Ca2+ increase in the ER-PM junction that matches experimental observations. Moreover, straightforward stochastic simulations of channel opening and closing taking into account the channels open probabilities in the presence of ligand and high Ca2+ concentration indicate a number of simultaneously open receptors matching with the results of the 3D spatiotemporal simulations. In the future, more realistic 3D simulations should be performed to take into account the stochastic nature of puffs and sparks to simulate microdomains, instead of the simplified deterministic description of stereotypic IP3R- or RYR1-mediated release of ER Ca2+ used in the present study.
As another perspective, the present model could be used to investigate how the increase in frequency of RYR1 opening observed ∼15 s after TCR/CD3 stimulation affects the spatiotemporal dynamics of junctional Ca2+ during the transition of T cells towards full activation. In these longer time scales, additional aspects of SOCE regulation should be considered, such as slow Ca2+ dependent inactivation (Dagan and Palty, 2021) or the dynamic nature of the ER-PM junctions (Okeke et al., 2016). The extension of the model to several junctions would enable to investigate how microdomains spread and interact to propagate Ca2+ signals deeper into the cell and promote full activation.
Data Availability Statement
The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.
DG, B-PD, AG and GD contributed to the conceptualization and design of the study. DG, AG and GD contributed to the development and analysis of the model. DG performed all numerical simulations. All authors contributed to the article and approved the submitted version.
This work was supported by the Deutsche Forschungsgemeinschaft (DFG) (project number 335447717; SFB1328, project A01 to AG), by the Joachim-Herz-Stiftung (Hamburg), Infectophysics Consortium (project 4; to AG), by NCL-Stiftung Hamburg (to AG), the Hamburg Ministry of Science, Research and Equality (LFF- FV75/0070-134, to AG), and by University Medical Center Hamburg-Eppendorf (M3I consortium, to AG). GD is Research Director at the FNRS.
Conflict of Interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/fmolb.2022.811145/full#supplementary-material
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Keywords: T cells, ER-PM junctions, ryanodine receptors, NAADP, COMSOL, computational model, store operated calcium entry, ca2+ signalling
Citation: Gil D, Diercks B-P, Guse AH and Dupont G (2022) Three-Dimensional Model of Sub-Plasmalemmal Ca2+ Microdomains Evoked by T Cell Receptor/CD3 Complex Stimulation. Front. Mol. Biosci. 9:811145. doi: 10.3389/fmolb.2022.811145
Received: 08 November 2021; Accepted: 24 January 2022;
Published: 23 February 2022.
Edited by:Ernesto Perez-Rueda, Universidad Nacional Autónoma de México, Mexico
Reviewed by:Alexandre Lewalle, King’s College London, United Kingdom
Thomas John Brett, Washington University in St. Louis, United States
Copyright © 2022 Gil, Diercks, Guse and Dupont. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Geneviève Dupont, Genevieve.Dupont@ulb.be