Accumulation of amyloid-beta (Aβ) is associated with synaptic dysfunction and destabilization of astrocytic calcium homeostasis. A growing body of evidence support astrocytes as active modulators of synaptic transmission via calcium-mediated gliotransmission. However, the details of mechanisms linking Aβ signaling, astrocytic calcium dynamics, and gliotransmission are not known. We developed a biophysical model that describes calcium signaling and the ensuing gliotransmitter release from a single astrocytic process when stimulated by glutamate release from hippocampal neurons. The model accurately captures the temporal dynamics of microdomain calcium signaling and glutamate release via both kiss-and-run and full-fusion exocytosis. We investigate the roles of two crucial calcium regulating machineries affected by Aβ: plasma-membrane calcium pumps (PMCA) and metabotropic glutamate receptors (mGluRs). When we implemented these Aβ-affected molecular changes in our astrocyte model, it led to an increase in the rate and synchrony of calcium events. Our model also reproduces several previous findings of Aβ associated aberrant calcium activity, such as increased intracellular calcium level and increased spontaneous calcium activity, and synchronous calcium events. The study establishes a causal link between previous observations of hyperactive astrocytes in Alzheimer's disease (AD) and Aβ-induced modifications in mGluR and PMCA functions. Analogous to neurotransmitter release, gliotransmitter exocytosis closely tracks calcium changes in astrocyte processes, thereby guaranteeing tight control of synaptic signaling by astrocytes. However, the downstream effects of AD-related calcium changes in astrocytes on gliotransmitter release are not known. Our results show that enhanced rate of exocytosis resulting from modified calcium signaling in astrocytes leads to a rapid depletion of docked vesicles that disrupts the crucial temporal correspondence between a calcium event and vesicular release. We propose that the loss of temporal correspondence between calcium events and gliotransmission in astrocytes pathologically alters astrocytic modulation of synaptic transmission in the presence of Aβ accumulation.
Accumulation of amyloid-beta (Aβ) is associated with synaptic dysfunction and destabilization of astrocytic calcium homeostasis. A growing body of evidence support astrocytes as active modulators of synaptic transmission via calcium-mediated gliotransmission. However, the details of mechanisms linking Aβ signaling, astrocytic calcium dynamics, and gliotransmission are not known. We developed a biophysical model that describes calcium signaling and the ensuing gliotransmitter release from a single astrocytic process when stimulated by glutamate release from hippocampal neurons. The model accurately captures the temporal dynamics of microdomain calcium signaling and glutamate release via both kiss-and-run and full-fusion exocytosis. We investigate the roles of two crucial calcium regulating machineries affected by Aβ: plasma-membrane calcium pumps (PMCA) and metabotropic glutamate receptors (mGluRs). When we implemented these Aβ-affected molecular changes in our astrocyte model, it led to an increase in the rate and synchrony of calcium events. Our model also reproduces several previous findings of Aβ associated aberrant calcium activity, such as increased intracellular calcium level and increased spontaneous calcium activity, and synchronous calcium events. The study establishes a causal link between previous observations of hyperactive astrocytes in Alzheimer's disease (AD) and Aβ-induced modifications in mGluR and PMCA functions. Analogous to neurotransmitter release, gliotransmitter exocytosis closely tracks calcium changes in astrocyte processes, thereby guaranteeing tight control of synaptic signaling by astrocytes. However, the downstream effects of AD-related calcium changes in astrocytes on gliotransmitter release are not known. Our results show that enhanced rate of exocytosis resulting from modified calcium signaling in astrocytes leads to a rapid depletion of docked vesicles that disrupts the crucial temporal correspondence between a calcium event and vesicular release. We propose that the loss of temporal correspondence between calcium events and gliotransmission in astrocytes pathologically alters astrocytic modulation of synaptic transmission in the presence of Aβ accumulation.
Astrocytes, the most abundant glial cells, are now recognized for their role in maintaining normal brain functioning [1,2]. Apart from providing structural and energy support to neurons, these densely connected cells send ramified processes to neighboring synapses and form nonoverlapping synaptic islands [3,4]. A plethora of receptors are found on the astrocytic membrane; amongst them, metabotropic glutamate receptors (mGluRs) are specifically juxtaposed to the endoplasmic reticulum (ER) tubules and are expressed in high densities on compartments adjacent to synapses [5-7]. This remarkable configuration and the presence of inositol 1,4,5-trisphosphate receptor (IP3Rs) clusters on the ER allow fast and high amplitude calcium transients in the ramified processes of the astrocytes [8,9]. Along with these molecular components for Ca2+ signaling and their placement [10,11], astrocytes are also equipped with an elaborate apparatus for fast Ca2+-dependent release of gliotransmitters, which is comparable to neurons [12,13]. The link between calcium signaling and gliotransmission from astrocytic microdomains was established by a study that quantified Ca2+ transients using near-field imaging of astrocytic terminals loaded with a low-affinity calcium indicator in combination with a pH-sensitive vesicular glutamate transporter [5]. This technique allowed them to track subcellular Ca2+ events and the corresponding gliotransmitter release events simultaneously with good temporal resolution and brought to light several novel features of gliotransmission at subcellular compartments near synapses. First, the application of a short pulse of mGluR agonist evoked fast and stochastic Ca2+ events whose time course perfectly matched the ensuing gliotransmitter release events. The study also revealed tight spatial and temporal correlations between Ca2+ and exocytic fusion events. These results strongly indicate that gliotransmitter release events are coupled to microdomain Ca2+ events in individual astrocytic compartments. The study further reports the presence of two distinct classes of vesicle populations that differ in their fusion modes (kiss-and-run versus full-fusion) and in the timescales of endocytosis and reacidification. Several synaptotagmin (Syt) isoforms (calcium sensors for vesicle release) have been reported in astrocytes; amongst the subtypes, Syt4 and Syt7 are specifically associated with fast synchronous kiss-and-run and slow asynchronous full-fusion releases, respectively [14-17]. Several other studies also provide compelling evidence on the existence of dual release pathways and the ability of astrocytes to modulate synaptic strength in neuronal circuits [18-21].The intimate spatial association between astrocytic compartments and synaptic junctions, together with the presence of a fast Ca2+ signaling machinery and multiple pathways for gliotransmitter release, provide the necessary framework for astrocytes to engage in bidirectional communication with neurons [22,23]. However, this pathway, an intrinsic component of communication by astrocytes, is heavily compromised under calcium overload, leading to excitotoxicity, loss of spines, and network connectivity [24,25]. Of relevance to the present study is the correlation between Aβ plaques seen in AD and the disruption of glutamate-mediated excitatory transmission [26]. Multiple lines of evidence point to a link between Aβ toxicity and calcium dysregulation in astrocytes [27]. Not only is Aβ a direct modulator of astrocytic Ca2+ [28], but it also elevates resting Ca2+ levels and synchronous Ca2+ events [29].Even though several studies report on abnormal Ca2+ regulation in astrocytes exposed to Aβ, not much is known about the chronology of events and molecular mechanisms that disrupt the calcium signaling [30]. Nevertheless, both in vitro and post-mortem studies in AD brains highlight the role of two important Ca2+ regulating pathways, namely mGluRs [31,32] and PMCAs [33,34]. It has also been suggested that a significant part of the excess glutamate observed in AD brains has an astrocytic origin and is a consequence of Aβ signaling [35]. Again, the underlying biophysical links are not clear. These studies underscore that cellular degeneration in AD is orchestrated by a chain of signaling cascades extending all the way from Aβ to alterations in Ca2+ signaling and synaptic signaling by astrocytes [36]. Understanding the astrocytic mechanisms that are derailed under the influence Aβ is, therefore, crucial for advancing our knowledge of the pathogenesis of synaptic dysfunction that underlies the cognitive decline in AD [37].Synergistic crosstalk between theory and experiments has led to some of the most profound insights in neuroscience and, more specifically into neurotransmitter release machinery and organization [38-40]. However, an equivalent biophysical modeling framework for calcium-dependent vesicle release and recycling does not exist, despite extensive knowledge on the calcium-binding kinetics of synaptotagmins [41], their different modes of vesicle release [18,42] and localization and lastly, calcium signaling [5] in the ramified processes that envelop synapses. Previous computational models have focused on global Ca2+ signals in astrocytes [43-45] and proposed phenomenological models to capture feedback to neurons via gliotransmission at a tripartite synapse [46-48]. Recently, studies have also shed light on the microscale mechanisms at fine astrocytic processes [49-52]. These models have made several valuable predictions on the contribution of astrocytes to brain function. The present study builds on this literature to fill the conspicuous gap (biophysical model of vesicle release and recycling) in the models and extend the existing computational modeling framework [53,54].The primary route for Ca2+ excitability in astrocytes in our model is through the activation of mGluRs that are expressed in high levels on astrocytic compartments around synapses [2,55,56]. A limited number of IP3Rs on the ER generate fast but noisy Ca2+ transients in the astrocytic process [5]. We implement stochastic opening and closing of a small cluster of IP3Rs consistent with experimental studies. Our model also accounts for the high luminal Ca2+ concentration and ER/cytosol volume ratio in the process compared to the cell body [5,57,58]. The elaborate machinery available to astrocytes for fast Ca2+-dependent release of gliotransmitters has been reported extensively [12,13]. We model molecular details as well as the timescales of calcium-binding for Syt4 and Syt7 isoforms of Synaptotagmins (Syt) that trigger fast synchronous kiss-and-run and slow asynchronous full-fusion releases, respectively, in astrocytes [14-17]. Our biophysical model accurately chronicles experimentally observed temporal dynamics of high amplitude and fast Ca2+ events when stimulated by mGluR agonist and exo-endocytosis steps for Ca2+-mediated gliotransmitter release [1,2,5,11,13,58-60]. We use this validated biophysical model for calcium signaling and the resulting gliotransmitter release by an astrocyte at a tripartite synapse to examine the functional interplay between two key Ca2+ regulating mechanisms that are altered by Aβ. Furthermore, we predict the consequences of altered Ca2+ signaling on gliotransmission at astrocytic microdomains for a wide range of stimuli and describe the underlying mechanism.
Methods
The governing equations for Ca2+ and IP3R signaling components of the model (Fig 1A) are presented in S1 Appendix. Our choice of parameter values (S1 Table) are based on published literature and were adjusted, if necessary, to reproduce the fast kinetics of mGluR-dependent Ca2+ transients reported by previous studies [5,10,61].
Fig 1
Description and characterization of Ca2+ signaling in the astrocytic compartment.
(A) Schematic of the astrocytic compartment along with all the molecular components. (B) Representative Ca2+ events from an astrocytic compartment stimulated with DHPG (100 μM, 2 sec). (C) Raster plot of Ca2+ events. (D) Distribution of Ca2+ event peak amplitudes from 400 trials. (E) Distribution of Ca2+ event rise times. (F) Histogram of full width at half maximum (FWHM). (G) Decay time histogram. (H) Temporal distributions of Ca2+ events from the model and experimental data (Marchaland et al., 2008a). Error bars indicate the standard error of the mean computed from 6 independent datasets.
Description and characterization of Ca2+ signaling in the astrocytic compartment.
(A) Schematic of the astrocytic compartment along with all the molecular components. (B) Representative Ca2+ events from an astrocytic compartment stimulated with DHPG (100 μM, 2 sec). (C) Raster plot of Ca2+ events. (D) Distribution of Ca2+ event peak amplitudes from 400 trials. (E) Distribution of Ca2+ event rise times. (F) Histogram of full width at half maximum (FWHM). (G) Decay time histogram. (H) Temporal distributions of Ca2+ events from the model and experimental data (Marchaland et al., 2008a). Error bars indicate the standard error of the mean computed from 6 independent datasets.
Glutamate stimulation
Glutamate evoked Ca2+ events, and gliotransmission at a single astrocytic compartment was examined by stimulating with either steady-state pulses (2s & 30s) or by a time varying profile of glutamate concentration (see below) as observed at the perisynaptic region close to astrocytic compartments, which was kept the same for both control and Aβ conditions [62-64]. Following each presynaptic spike, a pulse of glutamate was released, whose time course was implemented using a simple first-order reaction equation that captured both the sharp peak (~200μM) and decay (6.25ms) of glutamate concentration (S1 Appendix and S1 Table and S1A Fig). The effective glutamate concentration ([Glu](t)) was modelled using the below equation whose parameters were adjusted to consider changes in the glutamate concentration due to mechanisms such as receptor binding and reuptake.
IP3 dynamics
While the major IP3 generation pathway was through the activation of mGluRs by glutamate spillover from adjacent presynaptic terminals, IP3 was also generated in a Ca2+-dependent manner through PLCδ activity. The model also included two IP3 degradation pathways, namely, inositol polyphosphate 5-phosphatase and IP3 3-kinase [65-67] that are described in S1 Appendix, and the parameters are in S1 Table.
Modeling Ca2+-mediated gliotransmission
Both fast kiss-and-run confined releases and slow-spreading full-fusions events have been reported by studies that imaged the release of fluorescent labeled vesicles from astrocytic processes [18,20]. Among the important molecular components that govern Ca2+-mediated release, two synaptotagmins (Syts), namely Syt4 and Syt7, have been associated with rapid kiss-and-run and slow full-fusion exocytosis, respectively, have been found in astrocytes [14,15,17,68]. Moreover, Syt4, which is known to specifically promote kiss-and-run exocytosis [69], has a single low-affinity (k ~ 22 μM) domain that binds Ca2+ ions with fast forward calcium-binding rates, making it a detector of fast and high amplitude Ca2+ events. Whereas, Syt7, has five high affinity (k ~ 15 μM) binding sites that bind Ca2+ at a much slower rate [41] and is thought to mediate full-fusion release when activated by slow and low amplitude Ca2+events. The involvement of Syt7 in slow full-fusion exocytosis is further in agreement with data from an experiment that measured changes in cell capacitance following slow full-fusion release events [70]. Taking these studies into account, we modeled Ca2+-dependent gliotransmitter release using detailed kinetics schemes of two distinct synaptotagmins (Syt4 and Syt7). We also incorporated detailed kinetics of endocytosis, vesicle recycling, and vesicle docking as reported experimentally [5,71,72] (Fig 2B and S1 Table). Moreover, as suggested by one study [73], we considered two pools of vesicles (docked and mobile) that are distinctly targeted by Syt4 & Syt7. Our model assumes newly recycled vesicles to remain as mobile vesicles until they are transported to the docking site. Accordingly, we introduced a docking rate that controls the transfer of vesicles from the mobile pool to the docked vesicle pool (Fig 2B). Modeling the distinct Ca2+ binding sites and reaction rates of the two synaptotagmins (Syt4 & Syt7) and their target vesicle pools was crucial for reproducing the time courses of kiss-and-run and full-fusion releases as observed experimentally (Fig 2B and S1 Table). In summary, high-affinity binding sites in Syt7 promote slow full-fusion releases when activated by low amplitude Ca2+ elevations, while fast low-affinity binding sites in Syt4 promote rapid kiss-and-run release of docked vesicles in the presence of high amplitude Ca2+ rises. Each of these pathways also follows different rates of endocytosis and recycling and has been modeled accordingly [74].
Fig 2
Description and characterization of the Ca2+-dependent gliotransmitter release machinery.
(A) Schematic of the gliotransmitter release machinery. (B) Pathways of release, endocytosis, and recycling of docked and mobile vesicles. (C) Vesicular release rate through Synaptotagmin 4 (Syt4) in response to a range of steady state Ca2+ concentrations. (D) Peak release rates of Syt4 are fitted to a Hill function to estimate the dissociation constant (k). (E) Time to peak release rate of Syt4 decays exponentially with Ca2+ concentration. (F) Release rates of Synaptotagmin 7 (Syt7) in response to a range of steady state Ca2+ concentrations. (G) Peak release rates of Syt7. (H) Time to peak release rate of Syt7.
Description and characterization of the Ca2+-dependent gliotransmitter release machinery.
(A) Schematic of the gliotransmitter release machinery. (B) Pathways of release, endocytosis, and recycling of docked and mobile vesicles. (C) Vesicular release rate through Synaptotagmin 4 (Syt4) in response to a range of steady state Ca2+ concentrations. (D) Peak release rates of Syt4 are fitted to a Hill function to estimate the dissociation constant (k). (E) Time to peak release rate of Syt4 decays exponentially with Ca2+ concentration. (F) Release rates of Synaptotagmin 7 (Syt7) in response to a range of steady state Ca2+ concentrations. (G) Peak release rates of Syt7. (H) Time to peak release rate of Syt7.A typical chain of events starts with a presynaptic release followed by: (1) rise in extracellular glutamate levels, (2) activation of mGluRs on the astrocytic compartment, (3) increase in intracellular IP3, and (4) stochastic opening of IP3Rs on the ER membrane to generate fast Ca2+ transients (S1 Fig). These Ca2+ events have low peak amplitudes (5–20 nM) when stimulated with presynaptic glutamate release at low frequencies. However, IP3 concentration quickly builds up when the stimulation frequency is increased, leading to high amplitude Ca2+ events (5–10 μM) that can trigger gliotransmission. A release event gets triggered (either via Syt4 or Syt7) every time the release probability, computed by multiplying the instantaneous release rate and the integration time step (50 μs), is greater than a uniform random number over the open interval (0,1). The Ca2+-dependence of the release machinery was subsequently characterized by clamping intracellular Ca2+ level and fitting the peak release rate to the below equation with V, k and n as free parameters [75].
Quantifying the percentage of calcium response
The percentage of Ca2+ responses (r) from different stimulation regimes was quantified by normalizing the area under the curve using the equation described below, where t and t refer to stimulation onset and duration, respectively.
Detection and measurement of calcium events
The full width at half maximum (FWHM) of Ca2+ events whose peak amplitude crossed the threshold value (300 nM) was identified using the ‘find_peaks’ and ‘peak_widths’ functions available from SciPy-1.7.3. The choice of the threshold for identifying Ca2+ events was based on a previous report on the physiological minimum to evoke glutamate release from astrocytes [76]. Rise time was measured as the time between 20% and 80% of the signal peak, and decay time was measured as the time between peak and 36.8% of the peak amplitude.
Synchrony measure
Synchrony of discrete Ca2+ and release events evoked by glutamate application at different rates was computed using the Pinsky-Rinzel method [77,78]. The data set comprised of 1000 independent trials (j) each for stimulation frequencies ranging from 0.4 to 100 Hz. Firstly, (1) a vector of inter-event intervals (k) was computed, with respect to each event, for all the events in the event matrix (events x trials). (2) The vector of inter-event intervals was normalized by the maximum interval to obtain the phase vector (ϕ). (3) The phase vector was projected to a complex plane, and synchrony was computed from the (4) variance as given by the equations below. The above steps (1–4) were repeated by choosing another event as the reference event and the values were averaged. Synchrony (s) was computed for each stimulation frequency and inter-event interval pair, where a value of 1 corresponds to perfect alignment of event times across all the trials and, 0 means that the events are completely random.
Computation of cross-correlation between Ca2+ and release events
Cross-correlations within a fixed time window (100ms) were computed from the diagonal elements of the normalized joint peristimulus time histogram of Ca2+ and release event times [79,80]. Peak cross-correlations were extracted from the signal duration (11s) starting from the time of glutamate stimulation at frequencies ranging from 0.4 to 100 Hz. The standard error of the mean was estimated by sampling with replacement from a set of 1000 simulation trials.
Numerical simulation and code
Simulation codes written in C++ were compiled and computed on the high-performance computing cluster (1500 nodes) at the Indian Institute of Science Education and Research Pune. Part of the simulations and data analysis were carried out on a desktop computer running Linux kernel 5.16.11 with custom Python scripts using Python-3.10.2. State variables were updated at fixed time steps (50μs) using the Euler–Maruyama method for integrating stochastic differential equations. Standard errors in the plots were computed from independent sets of simulation runs or by sampling with replacement (bootstrapping) from a large set. Students t test and ANOVA were used to determine the statistical significance of the difference between means; P < 0.05 was considered statistically significant. P < 0.05, 0.01 and 0.001 are indicated in the figure by single, double and triple asterisks, respectively. Averaged values are reported as mean ± SEM. All the simulation and data analysis codes are available from the author’s GitHub page (https://github.com/anupgp/astron).
Results
A single-compartment model for astrocytic Ca2+ signaling and gliotransmission
We first describe local calcium dynamics in an astrocytic microdomain that envelops a typical hippocampal CA1 synapse (Fig 1A). Distinct molecular components on the plasma and ER membranes, Ca2+ buffers in the cytoplasm and ER collectively regulate the fast and slow Ca2+ events. Specifically, the stochastic opening of IP3Rs on the ER membrane generates rapid Ca2+ events whose rise time and decay kinetics are modulated by PMCA pumps on the plasma membrane, Ca2+ buffers, and SERCAs.A single pulse of DHPG (100 μM, 2 secs), a highly specific group 1 mGluR agonist, generates sharp and high amplitude Ca2+ events during the stimulus duration (Fig 1B). Stochastic Ca2+ events from independent trials are described in the raster plot in Fig 1C. The distributions of peak amplitude, rise time, FWHM, and decay time, are in good agreement with previous experimental observations (Fig 1D–1G) [11,61]. We next examined the temporal characteristics of these events from a set of 400 independent trials to validate our model findings with a previous study by Marchaland et al. that examined Ca2+ signals from individual microdomains [6]. Our choice of the number of independent trials for comparing our results is based on a rough estimate of the number of microdomains included in the experimental data (S2 Appendix). The close overlap between the Ca2+event histogram of the model and the experimental data (Fig 1H), and the good agreement with experimental data on Ca2+ events characteristics described above, validates our model for a single astrocytic compartment.We next describe the biophysical model for Ca2+-mediated gliotransmitter release in a single astrocyte compartment, drawing on existing insights on Ca2+-sensors (synaptotagmins), vesicle distribution, and recycling times (Fig 2A and S3 Appendix). The model incorporates two separate Ca2+ sensors, namely Syt4 and Syt7, each with distinct Ca2+ binding affinities and forward reaction rates to mediate fast kiss-and-run and slow full-fusion releases, respectively. Analogous to vesicle recycling at the presynaptic terminal, following a release, vesicles are endocytosed, reacidified, and added to the mobile vesicle pool before they become available in the docked vesicle pool (Fig 2A and 2B). A detailed description of the release machinery is included in the Methods section (Modeling Ca).We first characterize the temporal dynamics of the two synaptotagmins that differed in their (1) binding affinities, (2) forward reaction rates, and (3) target vesicle pools by characterizing their release rates at various steady-state intracellular Ca2+ levels. The Syt4 activation led to large release rates that rapidly decayed in tens of milliseconds. In comparison, the peak release rate of Syt7 is much lower and takes hundreds of milliseconds to get back to baseline (Fig 2C and 2F). We further quantify their decay kinetics and estimate equilibrium constants (k) from fits to double exponentials (Fig 2E and 2H) and Hill equations (Fig 2D and 2G), respectively. Our estimates of k for Syt7 agree with a previous study [59]. Our results also showcase substantial differences between Syt4 and Syt7 in their (1) binding affinities, (2) rise times, and (3) decay kinetics.We next examine the temporal features of gliotransmission when activated by a short pulse of DHPG (100 μM, 2 secs) (Fig 3A). Here, the gliotransmitter release event is probabilistically determined by the release rate of the two synaptotagmins, which in turn is influenced by both the amplitude and decay kinetics of individual Ca2+ events, which are stochastic in nature. We find that kiss-and-run (KR) exocytosis, which is mediated through Syt4 and triggered by high amplitude and fast Ca2+ events, shows much less variability when compared to full-fusions (FF) through Syt7 (Fig 3A). This was also evident from the temporal profile of KR releases which displays faster dynamics compared to FF exocytosis (Fig 3B and 3C). The population of docked vesicles declines shortly after the stimulus and gets replenished to initial levels in a timespan of about 15–20 seconds (Fig 3D). In contrast, the population of mobile vesicles increases and remains high even after the stimulus is removed (Fig 3E). Apart from vesicle replenishment rates, the differences between KR and FF exocytosis are also evident in the dynamics of endocytosis and reacidification of docked and mobile vesicles (Fig 3D and 3E). To validate the model, we compared the temporal profile of the simulated gliotransmitter release with published experimental data on gliotransmission from several studies for similar stimulus protocols [5,61,81,82]. To make this comparison, we pooled data from 400 independent simulation trials which corresponds to the number of microdomains in the experimental data (S2 Appendix). Evidently, the temporal distribution of Ca2+-mediated release events evoked by DHPG stimulation is in good agreement with the experimental data (Fig 3F). It is also interesting to note that the temporal profile of gliotransmission is remarkably similar across studies that used different agonists and concentrations, suggesting that all these stimuli produced saturating responses and resulted in a complete depletion of the vesicles. (S2 Fig).
Fig 3
Validation of the gliotransmitter release model.
(A) Raster plot of kiss-and-run and full fusion releases from an astrocytic compartment stimulated with DHPG (100 μM, 2 sec). (B) Distribution of kiss-an-run release times shows the rapid rise in release events that decay exponentially within the stimulus duration. (C) Temporal distribution indicates the comparatively slow and low number of full-fusion events that extends beyond the stimulus duration. (D) Time courses indicate the dynamics of docked vesicle release, endocytosis and reacidification. (E) Time courses indicate the dynamics of mobile vesicle release, endocytosis and reacidification. (F) Temporal distribution of total release events is in good agreement with experimental data from Marchaland et al. (Marchaland et al., 2008a). Error bars indicate the standard error of the mean computed from 6 independent sets of simulation trials.
Validation of the gliotransmitter release model.
(A) Raster plot of kiss-and-run and full fusion releases from an astrocytic compartment stimulated with DHPG (100 μM, 2 sec). (B) Distribution of kiss-an-run release times shows the rapid rise in release events that decay exponentially within the stimulus duration. (C) Temporal distribution indicates the comparatively slow and low number of full-fusion events that extends beyond the stimulus duration. (D) Time courses indicate the dynamics of docked vesicle release, endocytosis and reacidification. (E) Time courses indicate the dynamics of mobile vesicle release, endocytosis and reacidification. (F) Temporal distribution of total release events is in good agreement with experimental data from Marchaland et al. (Marchaland et al., 2008a). Error bars indicate the standard error of the mean computed from 6 independent sets of simulation trials.
Modeling Aβ conditions in astrocytes
We next examine signaling by astrocytes in the presence of Aβ induced molecular alterations. It has been shown that the application of Aβ enhances mGluR5 activation when stimulated by DHPG to result in roughly 50% reduction in the half-activation concentration and a near doubling of the maximal response in the dose-response curve, thereby suggesting an increase in mGluR5 expression [31,83]. However, the functional consequences of enhanced Ca2+ signaling through this route is not clear. We incorporated these experimentally observed changes in mGluR signaling by adjusting the parameters of the mGluR model (S1 Table) that appropriately shifted the dose-response curve for maximal IP3 production. Our estimates of dissociation constant (k) and peak IP3 response clearly capture the halving and doubling of these quantities, respectively, as reported by previous experimental studies (Fig 4A). Independently, Aβ is also seen to inhibit PMCA function by direct binding to the calmodulin binding site [84]. Accordingly, we adjusted the backward reaction rate of the PMCA model (S1 Table) to shift the dose-response curve rightward (Fig 4B). This led to an almost 50% reduction in the Ca2+ binding affinity of the PMCA, which is in good agreement with in vitro findings [84]. An interesting corollary to this Aβ-induced PMCA alteration is the accompanying shift in the Ca2+ concentration that corresponds to zero net Ca2+ flux across the PMCA. As a result of which, both resting cytosol and ER Ca2+ concentrations are higher in astrocytic compartments with impaired PMCA activity (Fig 4C). We, therefore, propose that Aβ-induced alterations in PMCA functionality is the underlying mechanism for the observed shift in intracellular resting Ca2+ levels in astrocytes in AD animal models [27].
Fig 4
Characterization of the astrocytic compartmental models with Aβ-induced molecular alterations.
(A) Peak amplitudes of IP3 generated by DHPG stimulation from control and an astrocytic compartment with altered mGluR function are fitted to Hill functions for estimating dissociation constants (k). (B) Steady-state PMCA fluxes from control and Aβ-PMCA conditions fitted to Hill functions. (C) Resting cytosolic Ca2+, IP3, and ER Ca2+ levels in control and Aβ-conditions. (D) Representative heat maps of Ca2+ signaling from control and Aβ conditions stimulated with DHPG. (E) Peak amplitude of Ca2+ event evoked with different DHPG concentrations. (F) Rate of Ca2+ events evoked by different DHPG concentrations. (G) Percentage Ca2+ response evoked by DHPG stimulation is higher the presence of Aβ conditions. Error bars indicate the standard error of the mean computed from 6 independent sets of simulation trials.
Characterization of the astrocytic compartmental models with Aβ-induced molecular alterations.
(A) Peak amplitudes of IP3 generated by DHPG stimulation from control and an astrocytic compartment with altered mGluR function are fitted to Hill functions for estimating dissociation constants (k). (B) Steady-state PMCA fluxes from control and Aβ-PMCA conditions fitted to Hill functions. (C) Resting cytosolic Ca2+, IP3, and ER Ca2+ levels in control and Aβ-conditions. (D) Representative heat maps of Ca2+ signaling from control and Aβ conditions stimulated with DHPG. (E) Peak amplitude of Ca2+ event evoked with different DHPG concentrations. (F) Rate of Ca2+ events evoked by different DHPG concentrations. (G) Percentage Ca2+ response evoked by DHPG stimulation is higher the presence of Aβ conditions. Error bars indicate the standard error of the mean computed from 6 independent sets of simulation trials.We next examine the consequences of these two Aβ conditions on astrocytic Ca2+ signaling activated by the mGluR agonist, DHPG, at different concentrations. It is clear from the heat maps (representative traces of independent simulation trials) that in the presence of DHPG (100μM, 10s), Ca2+ signaling is considerably elevated in all Aβ conditions (Fig 4D). Quantification of three important metrics of astrocytic Ca2+ signaling that affect gliotransmission, namely peak, event rate, and % Ca2+ response (defined in methods), also indicated an overall increase (leftward and upward shifts in the dose-response curves) in Ca2+ influx (Fig 4E–4G), and is in good agreement with previous experimental results, both in vivo and in vitro [85,86]. Finally, it is also evident that the presence of PMCA alteration specifically led to an upward shift in all the dose-response curves due to an increase in spontaneous Ca2+ activity (Fig 4E–4G). We, therefore propose Aβ-induced alteration in PMCA functionality as a molecular mechanism for the experimentally reported increase in spontaneous Ca2+ activity in astrocytes treated with Aβ [87].
Aβ modifies astrocytic Ca2+ signaling, gliotransmission, and the temporal relationship between them
Given the elevated Ca2+ activity in astrocytes associated with Aβ accumulation [27,76] we investigate the Ca2+ response to a range of stimuli that incorporates physiological concentration and decay profile of glutamate in the extracellular space (S1 Fig). Not surprisingly, Ca2+ signaling is enhanced in astrocytic compartments with Aβ conditions. This is described in the heat maps of Ca2+ events evoked by glutamate stimulation at 10Hz (Fig 5A). The analysis reveals interesting differences in Ca2+signaling that depend on the provenance of the Aβ condition. Firstly, we show that peak amplitudes of Ca2+ events are exclusively higher in the presence of the Aβ-mGluR condition. In comparison, parameters that control temporal features of Ca2+ signaling such as rise time, FWHM, and decay time are specifically affected by the Aβ-PMCA condition and are surprisingly insensitive to the frequency of glutamate stimulation (Fig 5D–5F). Lastly, both Aβ conditions lead to an increase in the rate of Ca2+ events (Fig 5C). In general, the model predicts several alterations in astrocytic microdomain Ca2+ signaling in the presence of Aβ conditions that is also highly dependent on the target molecular mechanism.
Fig 5
Quantification of the dynamics and kinetics of Ca2+ events from astrocytic compartments stimulated with glutamate vesicles.
(A) Representative heat maps highlight the differences in Ca2+ dynamics in the presence of Aβ conditions. (B) Peak Ca2+ amplitude averaged across different ranges of stimulation frequencies. (C) Glutamate-evoked Ca2+ events are more frequent in astrocytes with Aβ conditions when compared to control. (D) The presence of Aβ-PMCA condition increases the (E) rise time, (F) decay time and (F) Full width at half maximum of astrocytic Ca2+ events. Error bars indicate the standard error of the mean from 6 independent datasets.
Quantification of the dynamics and kinetics of Ca2+ events from astrocytic compartments stimulated with glutamate vesicles.
(A) Representative heat maps highlight the differences in Ca2+ dynamics in the presence of Aβ conditions. (B) Peak Ca2+ amplitude averaged across different ranges of stimulation frequencies. (C) Glutamate-evoked Ca2+ events are more frequent in astrocytes with Aβ conditions when compared to control. (D) The presence of Aβ-PMCA condition increases the (E) rise time, (F) decay time and (F) Full width at half maximum of astrocytic Ca2+ events. Error bars indicate the standard error of the mean from 6 independent datasets.We then ask how the changes in Ca2+ signaling because of Aβ impact vesicular release by astrocytes. The raster plot of release events activated by a 10 Hz stimulus indicates that both kiss-and-run and full-fusion are elevated by Aβ conditions (Fig 6A). Full-fusion exocytosis is substantially elevated by the Aβ-PMCA condition (Fig 6B). In contrast, at higher stimulation rates, the Aβ-PMCA condition, but not the Aβ-mGluR condition, decreases kiss-and-run exocytosis (Fig 6C). The distinct effects of the two Aβ conditions on vesicular exocytosis are also captured in the bar graphs for a wide range of glutamate stimulation rates.
Fig 6
Quantification of gliotransmission in astrocytic compartments stimulated with glutamate.
(A) Raster plots of kiss-and-run and full-fusion releases in control astrocyte and in the presence of Aβ conditions. Top: temporal histograms. (B) Rate of full fusions for different glutamate stimulation rates. Right: release rates for the three stimulus groups (C) Rate of kiss-and-run exocytosis. Right: release rates pooled into three simulation groups. Error bars indicate the standard error of the mean computed from 6 independent datasets.
Quantification of gliotransmission in astrocytic compartments stimulated with glutamate.
(A) Raster plots of kiss-and-run and full-fusion releases in control astrocyte and in the presence of Aβ conditions. Top: temporal histograms. (B) Rate of full fusions for different glutamate stimulation rates. Right: release rates for the three stimulus groups (C) Rate of kiss-and-run exocytosis. Right: release rates pooled into three simulation groups. Error bars indicate the standard error of the mean computed from 6 independent datasets.Synchronous Ca2+ activity between astrocytic subpopulations is observed in animal models of AD [29]. Locally synchronized astrocytic Ca2+ rises are also thought to play an important role in the manifestation of seizure-like events [88]. Therefore, we investigated the impact of Aβ conditions on the timing of Ca2+ and gliotransmitter release events across independent simulation trials by computing temporal synchrony between events at different interevent intervals (see Methods). In the absence of Aβ conditions, Ca2+ events are not synchronized when the frequency of stimulation is low but gets moderately synchronized at higher stimulation rates (Fig 7A). However, this pattern is altered in the presence of Aβ conditions. Particularly, we show that the presence of the Aβ-PMCA condition is associated with highly synchronous Ca2+ events at low frequencies of glutamate stimulation but promotes desynchrony at higher rates (Fig 7B). This shift in synchronicity by Aβ conditions under different stimulation rates is also evident in the bar plots that show synchrony averaged across three different stimulation regimes. While global Ca2+ activity between astrocytes becomes synchronous in the presence of Aβ accumulation [29], the molecular mechanism is not clear. Our results indicate Aβ-mediated changes in PMCA functionality as a potential mechanism.
Fig 7
Synchrony of Ca2+ and gliotransmitter release events from astrocytic compartments stimulated with glutamate.
(A) Heat maps of Ca2+ event synchrony at different inter-event intervals and stimulation frequencies in the presence and absence of Aβ conditions. (B) Ca2+ synchrony averaged across event intervals at different glutamate stimulation rates is different between control and Aβ conditions. Right: at low stimulation regime, synchrony is high with the Aβ-PMCA condition, whereas at high stimulation rates, synchrony is more in the Aβ-mGluR condition (C) Heat maps of release event synchrony at different inter-event intervals and stimulation frequencies in the presence and absence of Aβ conditions. (D) synchrony of release averaged across event intervals at different glutamate stimulation rates is different between control and Aβ conditions. Right: bar graph indicates the increase in release synchrony at different stimulation regimes in all the Aβ conditions. Error bars indicate the standard error of the mean computed by bootstrapping 100 times with a sample size of 1000.
Synchrony of Ca2+ and gliotransmitter release events from astrocytic compartments stimulated with glutamate.
(A) Heat maps of Ca2+ event synchrony at different inter-event intervals and stimulation frequencies in the presence and absence of Aβ conditions. (B) Ca2+ synchrony averaged across event intervals at different glutamate stimulation rates is different between control and Aβ conditions. Right: at low stimulation regime, synchrony is high with the Aβ-PMCA condition, whereas at high stimulation rates, synchrony is more in the Aβ-mGluR condition (C) Heat maps of release event synchrony at different inter-event intervals and stimulation frequencies in the presence and absence of Aβ conditions. (D) synchrony of release averaged across event intervals at different glutamate stimulation rates is different between control and Aβ conditions. Right: bar graph indicates the increase in release synchrony at different stimulation regimes in all the Aβ conditions. Error bars indicate the standard error of the mean computed by bootstrapping 100 times with a sample size of 1000.The synchrony of vesicular release events is also affected by Aβ conditions (Fig 7C). Namely, peak synchrony of vesicular release is shifted leftward towards low the frequency regime in the presence of the Aβ-PMCA condition (Fig 7D).The temporal correlation between Ca2+ and gliotransmitter events is critical for astrocytic modulation of synaptic activity at short timescales [23,89,90]. Our simulations clearly demonstrate that Aβ is a modulator of both Ca2+ signaling and gliotransmission (Figs 5 and 6). How does the precise temporal correlation that was reported by experimental studies and reproduced by our model affected by Aβ conditions [5]? We investigate this by computing the correlation between Ca2+ and release events across independent simulation trials. As expected, cross-correlation is high in the control condition at low to moderate levels of stimulation rates (Fig 8A). In striking contrast, cross-correlation is low in the presence of Aβ-PMCA condition, and it is at the lowest in the presence of both PMCA and mGluR conditions. This is surprising because independently both the Aβ conditions increase Ca2+ events and gliotransmitter release events.
Fig 8
Cross-correlation between individual Ca2+ and gliotransmitter release events are disrupted in astrocytic compartments with Aβ pathology.
(A) Peak cross-correlations between Ca2+ and release events become low at higher stimulation rates in astrocytes with Aβ conditions when compared to control. (B) Higher stimulation rates decrease population of docked vesicles in astrocytes with Aβ conditions when compared to control. (C) The presence of Aβ conditions shifts the relationship between peak cross-correlation and docked vesicle population.
Cross-correlation between individual Ca2+ and gliotransmitter release events are disrupted in astrocytic compartments with Aβ pathology.
(A) Peak cross-correlations between Ca2+ and release events become low at higher stimulation rates in astrocytes with Aβ conditions when compared to control. (B) Higher stimulation rates decrease population of docked vesicles in astrocytes with Aβ conditions when compared to control. (C) The presence of Aβ conditions shifts the relationship between peak cross-correlation and docked vesicle population.Apart from Ca2+ event amplitudes, gliotransmission is also dependent on the availability of vesicles. We, therefore, examined changes in the vesicle resource as the root cause of decrease in cross-correlation. We see that the presence of Aβ conditions lowers the population of docked vesicles at high stimulation frequencies (Fig 8B) and mimics the trend of decrease in cross-correlation (Fig 8A). Thus, we show that the presence of Aβ conditions, despite causing an increase in both Ca2+ and release events, leads to the loss in the temporal relationship due to the rapid depletion of docked vesicles. Further quantification indicates the exponential relationship between peak cross-correlation and docked vesicles that is most catastrophic for the Aβ-PMCA condition (Fig 8C). In line with our speculation on the mechanism for the loss of the temporal correlation between Ca2+ and gliotransmitter release events, we have also shown that kiss-and-run exocytosis of docked vesicles is heavily impacted by the Aβ-PMCA condition (Fig 6C).
Discussion
The model of a single compartment of an astrocyte described here accurately captures the temporal characteristics of Ca2+ signaling and the resulting gliotransmission as observed in experimental studies [5,11]. To the best of our knowledge, it is the first model to include a biophysical description of two calcium sensors (Syt4 and Syt7), two release modes (full-fusion and kiss-and-run), and vesicle recycling (Figs 1–3). Aβ modulates Ca2+ signaling in astrocytes both in vivo [29] and in vitro [31,34,83]. Aβ is also a well-known regulator of presynaptic release probability [91]. However, mechanistic links between Aβ, astrocytic Ca2+ signaling, and gliotransmission are not known. The model reveals the distinct effect of two calcium signaling mechanisms, namely mGluR and PMCA, when modulated by Aβ on (1) characteristics of Ca2+ spikes, (2) Ca2+-mediated gliotransmission, (3) populations of docked and mobile vesicles, and (4) synchrony of Ca2+ and release events between trials. While both mechanisms increase the rate of Ca2+ events, changes in the mGluR signaling pathway elevate the amplitude of the Ca2+ events, whereas alteration in PMCA function increases the duration of the Ca2+ events (Fig 5). Further, the underlying high amplitude and fast Ca2+ events in the Aβ-mGluR condition favor kiss-and-run exocytosis through Syt4. This is because the Ca2+ affinity for Syt4 is low compared to Syt7. In contrast, the long-lasting Ca2+ events in Aβ-PMCA condition promote full-fusion releases through Syt7 (Fig 6). The complete model with both PMCA and mGluR pathology captures the increase in synchrony of Ca2+ events between trials (Figs 6 and 7), consistent with experimental observation [29].The correspondence between a calcium event and a vesicle release event is a characterizing feature of gliotransmission under physiological conditions. One of the most interesting observations from the model is the breakdown of this tight temporal relationship between Ca2+ and release events under the conditions of modified calcium signaling corresponding to the presence of Aβ (Fig 8). Our study predicts Aβ-induced depletion of docked vesicles as the possible mechanism for this disruption in signaling by astrocytes.
Building a control model
We build on previous models of intracellular calcium signaling to seek an accurate description of synaptically-activated gliotransmission at individual perisynaptic astrocytic processes. The model includes realistic descriptions of Ca2+ buffers and pumps, both within the cytoplasm and ER, and a stochastic activity of IP3Rs that generate physiologically realistic Ca2+ events. The model further incorporates available experimental data on (1) the number of calcium-binding sites and the calcium-binding affinities of each of the two calcium sensors, (2) the presence of two distinct vesicle populations, (3) the two distinct pathways of vesicle recycling and associated timescales (S1 Table and S1 Appendix). We have illustrated here the value of a biologically realistic model to investigate and quantify the link between Aβ-induced molecular mechanisms and their functional implications. It is widely accepted that astrocytic compartments next to synapses are equipped with several unique features such as (1) increased ER presence near docked vesicles, (2) high levels of mGluRs expression, and (3) IP3Rs that together allow the generation of Ca2+ events with high amplitudes and fast kinetics [5,6,92]. Other studies also suggest that Ca2+ dynamics in microdomains are several orders faster when compared to global somatic Ca2+ signals [22,60,93]. Notably, our model predictions on characterizing features of Ca2+ events such as peak amplitude, rise time, decay time, and full width at half maximum are in line with these experimental findings [5,10].
Predicting AD-associated changes in calcium signaling
Our model reproduces an increase in resting Ca2+ levels and a rise in spontaneous and synchronous high amplitude Ca2+ events, all in good agreement with experimental findings on Aβ-induced alterations [11,29]. Additionally, our findings also suggest Aβ-induced changes in PMCA functionality as an underlying mechanism for the above effects (Fig 4). Aberrations in the activity of PMCAs, apart from elevating cytosolic Ca2+, also sequesters Ca2+ into the ER, thereby increasing resting ER Ca2+ concentration. Ca2+ responses in astrocytes have a critical role in arterial blood flow regulation [94], and separately, amyloid depositions also impair blood flow [95], however, the underlying mechanisms are not clear. An increase in intracellular Ca2+ by Aβ-PMCA condition as described here can potentially impact cerebral blood flow and hence brain function. Our study also supports the proposed role of the Aβ-PMCA condition (and not Aβ-mGluR) in the generation of spontaneous Ca2+ activity in astrocytes [11]. Like neurons, astrocytes can also dynamically, as per need, switch their mode of exocytosis consistently, from kiss-and-run to full-fusion in response to different stimuli [20,96]. Although the underlying mechanism is not clear, it highlights the specific function of each mode of release. We show that the Aβ-PMCA condition drastically reallocates the rates of full-fusion and kiss-and-run. Specifically, there is a shift to full-fusion mode from kiss-and-run mode, and this shift decorrelates gliotransmitter release from the underlying Ca2+ events. The Aβ-PMCA condition generates Ca2+ events that are long-lasting with comparatively large rise time, full-width, and decay time. This results in increased Syt7 activation as the reaction kinetics of this sensor are slower than Syt4. These results, apart from highlighting the importance of Ca2+ dynamics in shaping gliotransmission, also shed light on the distinct ways by which the two Aβ conditions affect both Ca2+ signaling and gliotransmitter release.
Other insights from the model
While gliotransmitter releases have been observed at highly ramified astrocytic processes, they are still experimentally difficult to study. Despite this challenge, several studies have provided excellent data on the characteristics of Ca2+ and release events from single microdomains. It has been shown that at single processes, there is a remarkable temporal correlation between individual Ca2+ and release events [5]. However, it is important to note that these processes have a ninefold lower capacity of docked vesicles when compared to their presynaptic counterparts–the axon terminals [89]. This suggests that vesicles in astrocyte processes are extremely valuable ‘commodities’. While several studies have reported on the increase in Ca2+ signaling and, to a lesser extent, on the gliotransmission because of Aβ accumulation, the implications of having a low population of docked vesicles have not been considered either for normal physiology or disease conditions. We show that the temporal correlation between vesicle releases and calcium events is heavily dependent on the population of docked vesicles, and their non-linear relationship is altered in the presence of a disease condition–the Aβ pathology. Another aspect that is less understood is the presence of mobile vesicles in astrocytes [97,98] and their temporal dynamics. We show that the population of mobile vesicles increases shortly after the stimulus and takes tens of seconds to return to baseline levels. It has also been shown that the mobility of astrocytic vesicles increases with changes in astrocytic Ca2+ levels; our simulation corroborates this observation [99].
Justification for modeling framework
Multiple evidence supports our model for gliotransmission with two synaptotagmins (Syt4 and Syt7), that differ in both their reaction kinetics and Ca2+ affinities (details are in S3 Appendix) [15,68]. As suggested by experiments, the model includes separate pools of docked and mobile vesicles that are distinctly targeted by Syt4 and Syt7, respectively [5,19,73]. Our choice of model parameters that control the timescales of exocytosis, endocytosis, and reacidification rates are based on experimental measurements of kiss-and-run and full-fusion exocytosis [5,18]. The synaptotagmin Syt4 is exclusively activated by fast and high amplitude Ca2+ signals and primarily triggers fast temporally correlated release (synchronous release) of docked vesicles via kiss-and-run mode. This is in line with the suggestion that the ER membrane is juxtaposed onto docked vesicles to allow kiss-and-run release by fast and high amplitude Ca2+ events [5]. On the other hand, Syt7, which has high Ca2+ affinity but slow kinetics, is activated by low amplitude and slow Ca2+ events to cause release events that are temporally decorrelated with calcium events (asynchronous release). Also, unlike other synaptotagmins that are attached to the vesicle itself, Syt7 is diffusely expressed on the plasma membrane [100]. These features allow Syt7 to target mobile vesicles, which are not only reported in astrocytes but are also known to be transported in an activity-dependent manner [97,99]. A considerable portion of these vesicles become immobile once they reach the distal end of processes, suggesting vesicle docking [73,101]. Our model, in line with these findings, implements fast synchronous release of docked vesicles and slow, the asynchronous release of mobile vesicles through Syt4 and Syt7, respectively [20,102].Glutamate, the major excitatory neurotransmitter in the brain, has also been heavily implicated in the neuropathology of AD. While the bulk of the studies examining the synaptic component of Aβ pathology is focused on neurons, there is growing evidence that shows astrocytes contribute to the excitotoxicity observed in AD brains [103]. Astrocytes are primarily responsible for the clearance and metabolism of synaptically-released glutamate, and interestingly enough, both glutamate and glutamine levels are altered in AD brains [104]. Since astrocytes outnumber neurons in most brain regions, an increase in gliotransmission through the Aβ toxicity can cause major imbalances in glutamate levels and accelerate synaptic loss through excitotoxicity [105]. Increases in extracellular glutamate via gliotransmission are also implicated in the generation of Ca2+ waves owing to the tightly interconnected network architecture [106]. Modified gliotransmitter release, as predicted by our model, can alter the spatial extent of the Ca2+ waves. Interestingly Ca2+ waves are known to specifically originate from sites near Aβ plaques [29]. Since astrocytes are electrically silent, the tight temporal correlation of Ca2+ events with the gliotransmitter release is critical for astrocytic feedback [107]. The prediction from our study that describes disruption of the temporal correlation between Ca2+ and gliotransmission by Aβ mechanisms can have severe downstream consequences on astrocyte-neuron signaling. This also strengthens the idea that modified signaling by astrocytes contributes to AD pathology. It has been suggested that one of the roles of asynchronous release in neurons is to desynchronize the activity of downstream neurons [108]. Considering that astrocytic compartments near synapses modulate neural firing through gliotransmitters, the observed loss in a temporal relationship can alter synaptic signaling and negatively impact information transfer across synapses in AD.In summary, we developed a biophysical model that accurately describes Ca2+ signaling and concomitant gliotransmitter release in a single astrocytic compartment. We show that Aβ, by acting on the astrocytic Ca2+ signaling and gliotransmission machinery, derails astrocyte to neuron communication. Future experiments are necessary to test whether this is one of the mechanisms through which Aβ deposits impair cognitive function in AD patients.
Details of the model.
(DOCX)Click here for additional data file.
Estimation of the number of astrocytic compartments in the experimental data.
(DOCX)Click here for additional data file.
Calcium sensors in the gliotransmitter release model.
(DOCX)Click here for additional data file.
Time courses of glutamate, IP3 and Ca2+ concentrations.
(DOCX)Click here for additional data file.
Temporal profiles of vesicle release from astrocytic domains in response to various stimuli.
(DOCX)Click here for additional data file.
Kinetic schemes of astrocytic calcium sensors (synaptotagmins).
(DOCX)Click here for additional data file.
Model parameters.
(DOCX)Click here for additional data file.25 Aug 2020Dear Dr Nadkarni,Thank you very much for submitting your manuscript "Amyloid pathology disrupts gliotransmitter release in astrocytes" for consideration at PLOS Computational Biology.As with all papers reviewed by the journal, your manuscript was reviewed by members of the editorial board and by several independent reviewers. In light of the reviews (below this email), we would like to invite the resubmission of a significantly-revised version that takes into account the reviewers' comments. This revised version should take into account all the issues pointed by the 4 reviewers, including those by reviewer 1 in their detailed comments provided as an attached pdf file (regarding the statement of the research goal, the use of references or the quality of English).Moreover, since your article was submitted within the Reproducibility Modelling Pilot scheme, it is crucial that your code be made available to the reviewers in order for them to check the reproducibility of your results.We cannot make any decision about publication until we have seen the revised manuscript and your response to the reviewers' comments. Your revised manuscript is also likely to be sent to reviewers for further evaluation.When you are ready to resubmit, please upload the following:[1] A letter containing a detailed list of your responses to the review comments and a description of the changes you have made in the manuscript. Please note while forming your response, if your article is accepted, you may have the opportunity to make the peer review history publicly available. The record will include editor decision letters (with reviews) and your responses to reviewer comments. If eligible, we will contact you to opt in or out.[2] Two versions of the revised manuscript: one with either highlights or tracked changes denoting where the text has been changed; the other a clean version (uploaded as the manuscript file).Important additional instructions are given below your reviewer comments.Please prepare and submit your revised manuscript within 60 days. If you anticipate any delay, please let us know the expected resubmission date by replying to this email. Please note that revised manuscripts received after the 60-day due date may require evaluation and peer review similar to newly submitted manuscripts.Thank you again for your submission. We hope that our editorial process has been constructive so far, and we welcome your feedback at any time. Please don't hesitate to contact us if you have any questions or comments.Sincerely,Hugues BerryAssociate EditorPLOS Computational BiologyDaniele MarinazzoDeputy EditorPLOS Computational Biology***********************Reviewer's Responses to QuestionsComments to the Authors:Please note here if the review is uploaded as an attachment.Reviewer #1: Pillai and Nadkarni introduce a novel model of astrocyte-synapse interactions that revolves around the biophysical description of calcium-dependent glutamate release from astrocytes. In particular, they distinguish between different mechanisms of glutamate exocytosis – kiss-and-run vs. full-fusion – by considering the Ca2+-dependent dynamics of different synaptotagmins. Then, they proceed to mimic amyloid-like pathology changing values to model parameters, and documenting, through numerical simulations, how amyloid-beta could affect astrocytic physiology, and astrocytic glutamate release in particular. The study is original and of interest to PLoS Computational Biology, with the potential to reach out to a broad audience, comprising both experimentalists and computationalists. Nonetheless, there is ample space for improvement of the manuscript in its present version. There are at least three main issues with the present paper. First, the research question is not clear, and the way the material is exposed is not exhaustive and somehow lousy. Second, there is a critical issue with the references cited by the authors, which often do not support the authors’ claims. Third, the writing style is poor, making the reading of the manuscript hard for several broken sentences, ambiguous terminology, and logical flow that is not consistent. For these reasons, I am advising for major revisions, which I am detailing in the attachment.Reviewer #2: Pillai and Nadkarni develop a computational model to link Ca2+ signaling in the processes of astrocytes with the gliotransmitter release by these cells. The model has two main components: (1) Ca2+ dynamics in astrocytes and (2) gliotransmitter release. A rise in Ca2+ concentration in the processes of astrocytes leads to transmitter release through a fast release pathway (termed kiss-and-run mechanism) and slow release pathway. The model reproduces key observations about Ca2+ signals and distribution of transmitter release events. The model is then used to explore the effect of changes in two Ca2+ pathways observed on in Alzheimer’s disease on Ca2+ dynamics. These include reduced plasma membrane Ca2+ ATPase (PMCA) and gain-of-function enhancement of metabotropic glutamate receptors (mGluRs). The model provides some useful insights into how these two pathways affect Ca2+ signaling and gliotransmitter release in Alzheimer’s disease-affected astrocytes.In my view the main contribution of this study is the development of gliotranmistter release model. Overall, I find the study very interesting as it is addressing an important topic. However, there are some key issues that needs to be addressed before accepting the paper for publication.Page 5: In the Introduction section, the authors state “While extensive experimental data and computational studies exist on somatic Ca2+ dynamics in astrocytes [26,27], a quantitative formulation of Ca2+ dynamics at a single astrocytic process and its relationship to Ca2+ mediated kiss-and-run and full fusion exocytosis has not been described”. I find this statement a little tricky. The second part of the statement is true, i.e. “a quantitative formulation of Ca2+ dynamics at a single astrocytic process and its relationship to Ca2+ mediated kiss-and-run and full fusion exocytosis has not been described”. However, the first part of the statement makes it sounds like the authors are doing something completely different with the Ca2+ dynamics to model Ca2+ signaling in the process. The fact is, both the “somatic Ca2+ dynamics in astrocytes” models developed before and the model presented in this paper are point models and none pay attention to the spatial structure. Thus the notion that their Ca2+ model is a radical departure from the previous models is technically not correct.Page 6: Before equation 1 “….therefore on included in the present model” should be “….therefore not included in the present model”Page 8-10: There is a disconnect between the description of Ca2+ model and gliotransmitter model. A clear description is needed explaining how the kinetic scheme in Figure 2B is related to the release and recycling scheme. For example, how do the “Docked vesicles” or “Release vesicles” relate to the scheme “S0 <->S1 <->S2”? Same applies to Syt7 scheme.Similarly, what does the statement “We characterized the release machinery by clamping intracellular Ca2+ levels and measuring peak release (R) rate, which was fitted to a Hill equation (4) with Vmax, Kd and coeff as free parameters” mean for the model? And how is equation (4) connected to the gliotransmitter model?How were the rate equations and parameters in the gliotransmitter model optimized? Were they optimized using trial and error method using the full model (i.e. Ca2+ and gliotransmitter dynamics together)? Or some kind of automated optimization method employing modular approach was used?Page 10-12: I believe the stochasticity in the synchrony between Ca2+ events and release come from the stochastic modeling of gliotranmission. However, this hasn’t been explicitly mentioned in the paper.Page 14, Figure 1: More details about the implementation of DHPG in the model are needed. How is DHPG related to glutamate or mGluR?Was glutamate raised to a fixed value for 2 sec or was raised for 2 sec and allow to decay according to first order kinetics? Was the rise a single event or multiple events applied periodically over 2 seconds?Page 14, 15, Figure 2B: The statement “Syt4 has a single low-affinity domain (C2B) that binds 2 Ca2+ ions with fast forward rates” is consistent with the kinetic scheme in Figure 2B. However, it is not clear if the mechanism described by the statement “It is also established that Syt4 with a single Ca2+ binding domain can only promote kiss-and-run exocytosis [16]” has been implemented in the model or not. If it is, how? Do states S1 and S2 in the Syt4 scheme both lead to vesicles release? Are the release probabilities in both S1 and S2 states the same or different?Overall, I believe it would make it easier to follow the model if all the rate equations for the gloitransmitter model are listed in a new table.Page 18 and Figure 5: What was the amplitude and life time (duration for which glutamate was raised) of each glutamate release (spillover)? I believe the amplitude of each individual glutamate release (spillover) event was ~200 uM and was modeled as first order rate equation with a 6.25 ms rise time and 10 ms decay time throughout the paper? If so, this should be explicitly stated on page 9.Page 20: The reference (kuchibhotla2008) needs to be fixed.Line 1, page 24: “ER Ca2+ levels (400 mM)” should be “ER Ca2+ levels (400 uM)”?Reviewer #3: Reproducibility report has been uploaded as an attachment.Reviewer #4: This work is a model study of cellular mechanisms associated with Alzheimer's disease.Elucidation of the causes of excessive accumulation of beta-amyloid and the mechanisms of cleansing brain tissue is currently a hot topic in brain physiology . At the same time, another important part in the area is to establish the cellular mechanisms that accompany the accumulation of beta-amyloids. On this basis, we can conclude that the problem solved in this work is of interest as a small puzzle piece that contributes to a general understanding of the problems associated with Alzheimer's disease. It is valuable for the specialists in the field, while might be less understandable for the general public.The manuscript contains a very detailed, even meticulous, description of the modeled cellular pathways and the rationale for the choice of parameters. This allows me to agree with the authors' assertion that they "presented a detailed biophysical model" of the processes under consideration. According to my knowledge, this is the first model to quantitatively predict the release of gliotransmitter in response to beta-amyloid accumulation.From the results obtained, I would single out two. The first is the answer to the question of what shifts in calcium dynamics are caused by the changes characteristic of the accumulation of beta amyloid. On a qualitative level, this answer could be obtained using a simpler model.The second result is a aberration of the causal relationship (worsening correlation) by bursts of calcium and the release of gliotransmitter.In line with the above, my assessment of the work presented is positive. I have no serious comments, and I think that the workcan be accepted for publication.Nevertheless, I recommend that the authors consider the following comment: the discussion of the discussion is quite lengthy, and in the absence of short Conclusions is difficult to read. I would suggest either split the discussion into subsections with subtitles, or add conclusions with a really short summary.**********Have all data underlying the figures and results presented in the manuscript been provided?Large-scale datasets should be made available via a public repository as described in the PLOS Computational Biology
data availability policy, and numerical data that underlies graphs or summary statistics should be provided in spreadsheet form as supporting information.Reviewer #1: No: There are at least three instances where relevant data were not shown.Reviewer #2: YesReviewer #3: NoneReviewer #4: Yes**********PLOS authors have the option to publish the peer review history of their article (what does this mean?). If published, this will include your full peer review and any attached files.If you choose “no”, your identity will remain anonymous but your review may still be made public.Do you want your identity to be public for this peer review? For information about this choice, including consent withdrawal, please see our Privacy Policy.Reviewer #1: NoReviewer #2: Yes: Ghanim UllahReviewer #3: Yes: Anand K. RampadarathReviewer #4: NoFigure Files:While revising your submission, please upload your figure files to the Preflight Analysis and Conversion Engine (PACE) digital diagnostic tool, . PACE helps ensure that figures meet PLOS requirements. To use PACE, you must first register as a user. Then, login and navigate to the UPLOAD tab, where you will find detailed instructions on how to use the tool. If you encounter any issues or have any questions when using PACE, please email us at .Data Requirements:Please note that, as a condition of publication, PLOS' data policy requires that you make available all data used to draw the conclusions outlined in your manuscript. Data must be deposited in an appropriate repository, included within the body of the manuscript, or uploaded as supporting information. This includes all numerical values that were used to generate graphs, histograms etc.. For an example in PLOS Biology see here: http://www.plosbiology.org/article/info%3Adoi%2F10.1371%2Fjournal.pbio.1001908#s5.Reproducibility:To enhance the reproducibility of your results, PLOS recommends that you deposit laboratory protocols in protocols.io, where a protocol can be assigned its own identifier (DOI) such that it can be cited independently in the future. For instructions, please seeSubmitted filename: Pillai.PCOMPBIOL-D-20-01194.pdfClick here for additional data file.Submitted filename: Reproducible_report_PCOMPBIOL_D_20_01194.pdfClick here for additional data file.21 Sep 2021Submitted filename: Pillai_et_al_2021_response_to_reviewers.docxClick here for additional data file.19 Nov 2021Dear Dr Nadkarni,Thank you very much for submitting your manuscript "Amyloid pathology disrupts gliotransmitter release in astrocytes" for consideration at PLOS Computational Biology.As with all papers reviewed by the journal, your manuscript was reviewed by members of the editorial board and by several independent reviewers. In light of the reviews (below this email), we would like to invite the resubmission of a significantly-revised version that takes into account the reviewers' comments.As you will see in these reviews, Reviewer#1 still points a number of issues with your manuscript. We feel that the sarcastic and sometimes aggressive tone of this review is counterproductive and does not contribute to create the serenity that one expects in a review process. This being said, we must admit that we agree with the substance (though not the form) of several of the points raised. In particular, the absence of line or page numbers or of change tracking methods in your revised manuscript makes the reviewer's task quite painful (and change tracking was explicitly required in the decision email). We also agree with the need to tone down some of the affirmations made in the text, in order to not present as consolidated facts in the literature what is actually only current possible interpretations of experimental results (for instance, the link between gliotransmission and amyloid beta, or the hypothesis that astrocytes are critical for information processing at synapses etc). Please take also into account the reviewer's comments about the title or the pertinence of the citations and make sure that your mathematical notations are consistent throughout the text. It is important that all the reviewer's comments are addressed in your revision. You are not expected to agree and conform with every and all of these comments, but you have to address them all.We cannot make any decision about publication until we have seen the revised manuscript and your response to the reviewers' comments. Your revised manuscript is also likely to be sent to reviewers for further evaluation.When you are ready to resubmit, please upload the following:[1] A letter containing a detailed list of your point-by-point responses to the review comments and a description of the changes you have made in the manuscript. Please note while forming your response, if your article is accepted, you may have the opportunity to make the peer review history publicly available. The record will include editor decision letters (with reviews) and your responses to reviewer comments. If eligible, we will contact you to opt in or out.[2] Two versions of the revised manuscript: one with either highlights or tracked changes denoting where the text has been changed; the other a clean version (uploaded as the manuscript file).Important additional instructions are given below your reviewer comments.Please prepare and submit your revised manuscript within 60 days. If you anticipate any delay, please let us know the expected resubmission date by replying to this email. Please note that revised manuscripts received after the 60-day due date may require evaluation and peer review similar to newly submitted manuscripts.Thank you again for your submission. We hope that our editorial process has been constructive so far, and we welcome your feedback at any time. Please don't hesitate to contact us if you have any questions or comments.Sincerely,Hugues BerryAssociate EditorPLOS Computational BiologyDaniele MarinazzoDeputy EditorPLOS Computational Biology***********************Reviewer's Responses to QuestionsComments to the Authors:Please note here if the review is uploaded as an attachment.Reviewer #1: I appreciate the effort put by the authors in improving their manuscript with respect to the original submission. However, while I found improved figures and Result's exposition, I am dismayed by the pervasive sense of carelessness still emerging from the writing style. Again, Citations appear to be often made superficially and lack a clear rationale with the cited work. The logical flow in crucial sections like Introduction and Discussion remains fragmented. This is nerving. Very often, when I read your new manuscript, I came to wonder if you were aware of what you mean in English or not since, on several occasions, your sentences do not make any sense, and your reasoning is flawed. We are reaching a stage in the computational glioscience literature where we are in charge of keeping the field rigorous and prioritizing quality and scientific rigor over bombastic statements and lousy material. While your editing would go towards the former, what still emerges from your manuscript is the latter. I am once more asking for major editings. The hope is that, since the first round took you about a year to be addressed with debatable results in terms of quality, this second occasion could instead be managed more effectively with the maximal outcome: i.e., we could finally go into publication. If not, frankly, my level of frustration with this work is reaching saturation.On a side note, on this round, not only do you not provide a manuscript with numbered lines making exact referencing to parts of the text impossible, but also you do not number pages, making the whole reviewing effort an even more daunting task. Thank you for showing respect and appreciation for your reviewers' time and effort. In your response to the reviewers and me, I also appreciated how you replied to several points by literally pasting the same answer.Reviewer #2: No more comments.Reviewer #3: Reproducibility report has been uploaded as an attachment.**********Have the authors made all data and (if applicable) computational code underlying the findings in their manuscript fully available?The PLOS Data policy requires authors to make all data and code underlying the findings described in their manuscript fully available without restriction, with rare exception (please refer to the Data Availability Statement in the manuscript PDF file). The data and code should be provided as part of the manuscript or its supporting information, or deposited to a public repository. For example, in addition to summary statistics, the data points behind means, medians and variance measures should be available. If there are restrictions on publicly sharing data or code —e.g. participant privacy or use of data from a third party—those must be specified.Reviewer #1: YesReviewer #2: YesReviewer #3: Yes**********PLOS authors have the option to publish the peer review history of their article (what does this mean?). If published, this will include your full peer review and any attached files.If you choose “no”, your identity will remain anonymous but your review may still be made public.Do you want your identity to be public for this peer review? For information about this choice, including consent withdrawal, please see our Privacy Policy.Reviewer #1: NoReviewer #2: Yes: Ghanim UllahReviewer #3: Yes: Anand K. RampadarathFigure Files:While revising your submission, please upload your figure files to the Preflight Analysis and Conversion Engine (PACE) digital diagnostic tool, . PACE helps ensure that figures meet PLOS requirements. To use PACE, you must first register as a user. Then, login and navigate to the UPLOAD tab, where you will find detailed instructions on how to use the tool. If you encounter any issues or have any questions when using PACE, please email us at .Data Requirements:Please note that, as a condition of publication, PLOS' data policy requires that you make available all data used to draw the conclusions outlined in your manuscript. Data must be deposited in an appropriate repository, included within the body of the manuscript, or uploaded as supporting information. This includes all numerical values that were used to generate graphs, histograms etc.. For an example in PLOS Biology see here: http://www.plosbiology.org/article/info%3Adoi%2F10.1371%2Fjournal.pbio.1001908#s5.Reproducibility:To enhance the reproducibility of your results, we recommend that you deposit your laboratory protocols in protocols.io, where a protocol can be assigned its own identifier (DOI) such that it can be cited independently in the future. Additionally, PLOS ONE offers an option to publish peer-reviewed clinical study protocols. Read more information on sharing protocols at https://plos.org/protocols?utm_medium=editorial-email&utm_source=authorletters&utm_campaign=protocolsSubmitted filename: Reproducible_report_PCOMPBIOL_D_20_01194R1.pdfClick here for additional data file.Submitted filename: PCOMPBIOL-D-20-01194R1.pdfClick here for additional data file.22 Jun 2022Submitted filename: Pillai_et_al_2022_response_to reviewers.docxClick here for additional data file.28 Jun 2022Dear Dr. Nadkarni,We are pleased to inform you that your manuscript 'Amyloid pathology disrupts gliotransmitter release in astrocytes' has been provisionally accepted for publication in PLOS Computational Biology.We would like to apologize again for the unprofessional, contemptuous and unacceptable tone of reviewer #1. We agree with a large part of the points you mention regarding the issue; actually this Associate Editor has decided to ban this reviewer from the list of reviewers he will send manuscripts to in the future.Before your manuscript can be formally accepted you will need to complete some formatting changes, which you will receive in a follow up email. A member of our team will be in touch with a set of requests.Please note that your manuscript will not be scheduled for publication until you have made the required changes, so a swift response is appreciated.IMPORTANT: The editorial review process is now complete. PLOS will only permit corrections to spelling, formatting or significant scientific errors from this point onwards. Requests for major changes, or any which affect the scientific understanding of your work, will cause delays to the publication date of your manuscript.Should you, your institution's press office or the journal office choose to press release your paper, you will automatically be opted out of early publication. We ask that you notify us now if you or your institution is planning to press release the article. All press must be co-ordinated with PLOS.Thank you again for supporting Open Access publishing; we are looking forward to publishing your work in PLOS Computational Biology.Best regards,Hugues BerryAssociate EditorPLOS Computational BiologyDaniele MarinazzoDeputy EditorPLOS Computational Biology***********************************************************24 Jul 2022PCOMPBIOL-D-20-01194R2Amyloid pathology disrupts gliotransmitter release in astrocytesDear Dr Nadkarni,I am pleased to inform you that your manuscript has been formally accepted for publication in PLOS Computational Biology. Your manuscript is now with our production department and you will be notified of the publication date in due course.The corresponding author will soon be receiving a typeset proof for review, to ensure errors have not been introduced during production. Please review the PDF proof of your manuscript carefully, as this is the last chance to correct any errors. Please note that major changes, or those which affect the scientific understanding of the work, will likely cause delays to the publication date of your manuscript.Soon after your final files are uploaded, unless you have opted out, the early version of your manuscript will be published online. The date of the early version will be your article's publication date. The final article will be published to the same URL, and all versions of the paper will be accessible to readers.Thank you again for supporting PLOS Computational Biology and open-access publishing. We are looking forward to publishing your work!With kind regards,Olena SzaboPLOS Computational Biology | Carlyle House, Carlyle Road, Cambridge CB4 3DN | United Kingdom ploscompbiol@plos.org | Phone +44 (0) 1223-442824 | ploscompbiol.org | @PLOSCompBiol
Authors: Marko Kreft; Matjaz Stenovec; Marjan Rupnik; Sonja Grilc; Mojca Krzan; Maja Potokar; Tina Pangrsic; Philip G Haydon; Robert Zorec Journal: Glia Date: 2004-05 Impact factor: 7.452
Authors: Matjaz Stenovec; Marko Kreft; Sonja Grilc; Maja Potokar; Mateja Erdani Kreft; Tina Pangrsic; Robert Zorec Journal: Exp Cell Res Date: 2007-08-31 Impact factor: 3.905
Authors: Iaroslav Savtchouk; Maria Amalia Di Castro; Rugina Ali; Hiltrud Stubbe; Rafael Luján; Andrea Volterra Journal: Proc Natl Acad Sci U S A Date: 2019-05-31 Impact factor: 11.205
Authors: Jun Nagai; Xinzhu Yu; Thomas Papouin; Eunji Cheong; Marc R Freeman; Kelly R Monk; Michael H Hastings; Philip G Haydon; David Rowitch; Shai Shaham; Baljit S Khakh Journal: Neuron Date: 2020-12-31 Impact factor: 17.173