Secretion of pulmonary surfactant by alveolar epithelial type II cells is vital for the reduction of interfacial surface tension, thus preventing lung collapse. To study secretion dynamics, rat alveolar epithelial type II cells were cultured on elastic membranes and cyclically stretched. The amounts of phosphatidylcholine, the primary lipid component of surfactant, inside and outside the cells, were measured using radiolabeled choline. During and immediately after stretch, cells secreted less surfactant than unstretched cells; however, stretched cells secreted significantly more surfactant than unstretched cells after an extended lag period. We developed a model based on the hypothesis that stretching leads to jamming of surfactant traffic escaping the cell, similar to vehicular traffic jams. In the model, stretch increases surfactant transport from the interior to the exterior of the cell. This transport is mediated by a surface layer with a finite capacity due to the limited number of fusion pores through which secretion occurs. When the amount of surfactant in the surface layer approaches this capacity, interference among lamellar bodies carrying surfactant reduces the rate of secretion, effectively creating a jam. When the stretch stops, the jam takes an extended time to clear, and subsequently the amount of secreted surfactant increases. We solved the model analytically and show that its dynamics are consistent with experimental observations, implying that surfactant secretion is a fundamentally nonlinear process with memory representing collective behavior at the level of single cells. Our results thus highlight the importance of a jamming dynamics in stretch-induced cellular secretory processes.
- mathematical model
- fusion pore
secretion of various molecules by cells is a fundamental process of life that helps maintain an appropriate cellular microenvironment (6, 22). In the lung, the secretion of surfactant, a complex lipid-protein mixture, by alveolar epithelial type II (AEII) cells plays a pivotal role in enabling gas exchange by lowering the surface tension at the air-liquid interface (5, 10). The secretion of pulmonary surfactant has been found to be a slow stochastic process that involves packing the constituent lipids and proteins into lamellar bodies (LBs) and releasing the LB content into the extracellular space through fusion pores (9, 15). Among the many secretory stimulants, mechanical stretching of AEII cells appears to be the most potent (12, 27). However, little is known about the stretch-induced temporal dynamics of surfactant secretion and the associated mechanisms.
In this study, we present experimental evidence that, contrary to the current view, certain stretch patterns are temporarily inhibitory and delay the secretion of surfactant. To interpret these results, we developed a simple model of stretch-induced secretion based on the hypothesis that excessive stretch leads to jamming of activated LBs trying to escape the cell through a limited number of fusion pores. We solved the model analytically and show that its dynamics are in agreement with the experimental observations.
The protocol was approved by the Institutional Animal Care and Use Committee at Boston University. AEII cells were isolated from Sprague-Dawley rats using a technique adapted from Dobbs et al. (11). The details of the protocol are described in detail by Arold et al. (3). Briefly, the rats were anesthetized, and the pulmonary artery was perfused to remove blood. The lungs were then excised and lavaged with phosphate-buffered saline and digested with 8 ml elastase solution (5 U/ml, Sigma, St. Louis, MO) for 30 min. Following digestion, the lungs were finely minced and filtered. The resulting supernatant was incubated for 1 h on Petri dishes coated with immunoglobulin G (Sigma) for differential adhesion. The nonadherent cells were removed and centrifuged, then resuspended in media, and seeded at 106 cells/cm2 on bioflex elastic membranes (Flexcell International, Hillsborough, NC) precoated with 50 μg/ml human fibronectin (Roche Diagnostics) for 24 h. Cell seeding was limited to a circular area of 0.9 cm2 in the center of the membrane. The yield of AEII cells was in the range of 30–40 × 106 cells per rat, with >95% purity per isolation.
The seeded cells were immediately incubated in the presence of radioactive 3H-labeled choline (1 μCi/ml) to label phosphatidylcholine (PC), the primary lipid constituent of pulmonary surfactant. Following incubation, the elastic membranes were placed directly above cylindrical indenter posts, and the membranes were vertically displaced by a computer-controlled linear actuator (4). The downward pulling of each membrane over the indenter post resulted in radial, as well as circumferential, expansion of the elastic membrane, causing the membrane and hence the adhered cells to receive equi-biaxial changes in surface area.
The cell populations were divided into several groups. The first group was left unstretched and served as the control group with baseline secretion. The remaining groups were cyclically stretched at a rate of 3 cycles/min with an amplitude of 50% change in surface area for stretch periods T of 15, 30, or 60 min. Samples were collected immediately at the end of the stretch period, as well as at subsequent times up to 60 min. For example, the cell populations that received 15 min of stretch were divided into three subgroups in which the samples were collected at 15, 30, or 60 min. This allowed us to track the effect of stretch on secretion after the stretch stopped. At the designated time points, the media was removed, the cells were lifted, and the lipids from both the media and the cells were isolated using the Folch partitioning (4). The percent 3H-labeled PC secretion was defined as the radioactive counts per minute of the media normalized by the total detections per minute of the cells and media averaged over six samples.
To make sure that the surfactant detected in the media was a result of secretion rather than due to cell membrane injury caused by stretching, the live and dead or injured cells were fluorescently labeled for each stretch condition using three additional groups. The three groups of cells were stretched for 15, 30, or 60 min, and the live/dead assay was carried out at 60 in each group. Cells were first incubated in the presence of ethidium homodimer-1 and calcein AM. Ethidium homodimer-1 only enters cells with a compromised plasma membrane and fluoresces bright red, whereas calcein AM fluoresces bright green within live cells. After labeling, the cells were examined using an upright fluorescent microscope, and images were captured from five random locations in each well. The fractions of dead and/or injured cells were calculated as the ratio of dead and injured cells to the total number of cells. The total count of live and dead cells showed no significant difference between groups, indicating that there was little cell detachment as in the previous study (3).
To determine whether stretch had any effect on surfactant uptake, unlabeled cells were placed in serum-free DMEM containing 1 μCi/ml 3H-labeled PC (3). The cells were then stretched according to the prescribed protocol. Following the 1-h treatment period, the cells underwent the Folch partition. The uptake was calculated as the ratio of detections per minute in the stretched cells, normalized to the detections per minute in unstretched control cells.
Part of the experimental data was reported earlier (2). An example of cells adhered to the membrane containing LBs is shown in Fig. 1. Figure 2 shows the fraction of surfactant secreted by the AEII cells for different stretching times T. At 15 min, cells undergoing stretch secreted significantly less (one-way ANOVA, P < 0.05) surfactant compared with unstretched cells (circles in Fig. 2). This indicates that the stretch pattern inhibited surfactant secretion at this time point. Similarly, at 30 min, all cell populations that experienced stretch secreted less surfactant than the unstretched cells; however, this decrease was not statistically significant. The secretion by cells that were stretched for the first 15 min and were unstretched for the next 15 min (squares in Fig. 2) was indistinguishable from cells that were stretched for the entire 30 min. At 60 min, cells that only experienced 15 min of stretch demonstrated a remarkable increase in secretion, surpassing the amount secreted by the unstretched cells (one-way ANOVA, P < 0.05). However, the cells that experienced longer durations of stretch (diamonds and triangles in Fig. 2) continued to secrete less than the unstretched cells (one-way ANOVA, P < 0.05).
The percent dead cells showed no difference, indicating that these observations were not a result of cell death or injury (Table 1). Stretch for any duration had no significant effect on surfactant uptake, suggesting that surfactant re-uptake by AEII cells did not play a significant role in the mechanism of stretch-induced PC secretion (Table 2).
Our model is based on the hypothesis that, when the cells are sufficiently stimulated by stretch, the surfactant traffic from the inside of the cell to the extracellular environment can become jammed. The model consists of a large number of identical cells adhered to an elastic membrane. The secretion of LBs in a typical cell involves a two-step process demonstrated schematically in Fig. 3A. We assume that a large pool of surfactant is available inside the cells separated from the outside by a membrane, or surface layer, which can store LBs. The surfactant inside the cells is continually packaged into LBs and driven up to the surface layer, resulting in an LB transport with current ϕ(t), which is a function of the instantaneous stretch experienced by the cells at time t. In the absence of stretch, the cells maintain a constant baseline current ϕ0. At any given time, the surface layer contains a number of LBs of total mass mS waiting to be secreted. The outflow current Q from the surface to the extracellular space is a function of mS, similar to the fundamental diagram in the dynamics of vehicular traffic (7, 21). We define mP as a threshold value of mS, beyond which jamming occurs in the outflow process. For mS < mP, Q increases with mS up to a maximum outflow Q = Qmax, when mS = mP. For mS > mP, we assume that the LBs at the surface begin to exhibit jamming, and Q decreases as mS increases until Q = 0 at mS = M, the maximum capacity of the surface. For simplicity, we assume that the function Q(mS) to be piecewise linear, as shown in Fig. 3B, allowing an analytic treatment of the model. Thus, (1) Note that the finite mass mS of surfactant retained at the surface provides the system with memory.
In addition to jamming in Q(mS), we assume that, when mS > mP, the overloaded surface reflects part of ϕ(t), which we model as a backflow current ϕb(mS, t), such that (2) This ensures that mS never exceeds M, since as mS → M the net inflow to the surface ϕ(t) − ϕb(mS, t) → 0, as well as the net outflow Q(mS) → 0.
The differential equations that govern the dynamics of mS and mOut, the mass of surfactant outside the cell, are (3a) (3b) as illustrated in Fig. 3A. As in the experiments, at t = 0, the mass at the surface mS(0) = m0 < mP and the mass outside mOut(0) = 0. Cells are then stretched for time T, such that ϕ(t) = Φ for t < T, and ϕ(t) = ϕ0 for t > T when stretching ceases.
In the absence of stretch, ϕ(t) = ϕ0 < Qmax, and we assume that no jamming occurs, mS (t) < mP. Thus the solutions to Eqs. 1–3 are given by (4a) (4b) where λ = Qmax/mP. The thin solid lines in Fig. 4 show plots of mS(t) and mOut(t), respectively. Note that 1/λ provides a natural time constant for this system. For t >> 1/λ, the surfactant content of the surface approaches a constant mS → ϕ0/λ, while the mass of secreted surfactant increases linearly, mOut → (m0 − ϕ0/λ) + ϕ0t.
When the cells are cyclically stretched, we assume that the time period of stretch is much smaller than the system time constant 1/λ, and thus ϕ(t) can be approximated to have a constant value Φ during the time of stretch T. We mimic the experimental protocol by setting ϕ(t) = Φ, corresponding to stretching, for 0 < t ≤ T followed by ϕ(t) = ϕ0, corresponding to no stretching, for t > T, (5) We define Φ* as the stretched activation rate beyond which jamming occurs after stretching for t = T. Thus, for Φ < Φ*, there is no jamming and Eq. 3 can be solved for mS(t) and mOut(t) yielding, (6a) (6b) where ΔΦ = Φ − ϕ0. The dashed lines in Fig. 4A show that mS increases to a steady state for t < T, followed by an exponential decrease back to the baseline value for t > T. Similarly, Fig. 4B shows that mOut increases at a greater rate than Φ increases for t < T, subsequently becoming parallel to the baseline curve for t > T. The critical current Φ* for which jamming occurs can be evaluated by requiring that mS(T) = mP for Φ = Φ*, which gives Φ* = λ (mP − m0e−λT)/(1 −e−λT). Since m0 < mP, the critical current Φ* > Qmax. For long stretching periods, T >> 1/λ, Φ* → Qmax. The thick solid line in Fig. 4B shows that mOut(t) is the largest in this case for t > T.
For Φ > Φ*, the dynamics of surfactant release can be divided into four distinct phases. Since the outflow Q(t) < Φ, mS increases from m0 at t = 0. We define T1 < T as the time of onset of jamming such that mS (T1) = mP. Thus, for 0 ≤ t ≤ T1, the solutions of Eq. 3 are (7a) (7b) Solving mS(T1) = mP in Eq. 7a gives T1 = λ−1 log [(Φ − λ m0)/(Φ − Qmax)].
For T1 < t ≤ T, the system is jammed, while ϕ(t) = Φ continues to drive mS toward M. In this phase, the solutions to Eq. 3 yields (8a) (8b) where λ1 = (Φ − Qmax)/(M − mP) provides a second time constant.
For t > T, stretching ceases, the current ϕ(t) = ϕ0, and, although the system is jammed, mS begins to decrease. We define T2 as the time when the jamming ends, such that mS (T2) = mP. Thus, for T < t ≤ T2, the solution of Eq. 3 is (9a) (9b) where λ2 = (Qmax − ϕ0)/(M − mP). The time T2 can be calculated as the point when jamming ends, mS(T2) = mP, giving T2 = (1 + λ1/λ2) T − (λ1/λ2) T1. The time constants 1/λ1 and 1/λ2 provide the time scales for increasing and decreasing surface mass in the jammed state.
Finally, for t > T2, the system gets out of the jammed state, and the solutions can be written as (10a) (10b) The dashed lines in Fig. 5 show the dynamics of mS and mOut for Φ > Φ*. With increasing Φ, mS → M during the stretching phase t ≤ T and takes increasingly longer times to recover from jamming after stretching stops. The secreted mass mOut shows a characteristic flat region during the jammed phase and quickly increases after jamming ceases.
The above expressions for mOut(t) allow us to fit the experimental data in Fig. 2 to obtain model parameters m0, λ, M, ϕ0, and Φ. We note that, since all parameters contain mP as a multiplicative factor, the value of mP cannot be obtained from the fitting procedures. First, m0, λ, and ϕ0 are obtained by fitting the unstretched data (Fig. 2, circles) using Eq. 4 and assuming that no jamming occurs in the unstretched case. Next, the same parameters are used for the curves corresponding to T = 15, 30, and 60 min (Fig. 2, squares, diamonds, and triangles) to obtain fitted values for M and Φ. Figure 2 shows the fitted curves thus obtained (solid lines).
To relax the assumption that our model consists of identical cells releasing surfactant in response to identical stretch, we numerically investigated the separate effects of 1) heterogeneous distribution of stretch in the system, and 2) heterogeneous cell sizes. To investigate the effect of a heterogeneous stretch distribution, we assume that stretch is directly related to Φ, and thus we assign distinct values of Φi for each cell i (11) where ξi are time-independent random numbers drawn from a uniform distribution with zero mean and standard deviation σ1 < 1, and the operator <…> represents the average over a large sample of the appropriate random variable. Similarly, when cell sizes are heterogeneous, we assume that the parameters mP, M, and Qmax are directly proportional to cell size. Thus we assign a different value of these parameters for each cell i (12a) (12b) (12c) where ηi are time-independent random numbers that are distributed uniformly with zero mean and standard deviation σ2 < 1. The values of <Φ>, <mP>, <M>, and <Qmax> are identical to the ones obtained from the model fits, such that, in the limit σ → 0, the heterogeneous model reproduces the homogeneous one. Since our model ignores cell-cell interactions, the normalized secretion of a population of cells is identical to the average of the secretion by individual cells. We thus solve Eq. 3 for each cell and compute <mS(t)> and <mOut(t)>.
Figure 6 shows the effects of simulated heterogeneity on the secretion dynamics for cells stretched up to T = 15 min. The parameters m0, λ, and ϕ0, as well as the mean values <Φ>, <mP>, <M>, and <Qmax> were identical to those obtained from the model fits in Fig. 2. In the absence of heterogeneity, σ1 = 0 and σ2 = 0, the time course of secreted surfactant outside the cell <mOut> as shown by solid lines in Fig. 6, B and D, are identical to the fitted results obtained for T = 15 min (dash-dotted lines in Fig. 2). With increasing heterogeneity in stretch amplitude (Fig. 6, A and B), as well as cell size (Fig. 6, C and D), the release of the jammed surfactant stored at the surface starts earlier, while, at the same time, it takes longer to completely release the excess surfactant. This results in a less pronounced shoulder in <mS> or knee in <mOut>. However, the general shape of the surfactant secretion curves remains the same.
Secretory processes by various cells are studied either at the level of a population of cells using molecular biology (27) or at the level of individual surfactant molecules passing through fusion-pores using biophysical methods (16). While it is possible to visualize individual LBs, one would need an enormous number of observations at the microscopic level to average out the fluctuations of individual molecules passing through the fusion pores. In this study, we used radioactive labeling and directly measured the bulk secreted surfactant from tens of thousands of cells, which allows us to observe and quantify the stretch-induced dynamics of surfactant secretion by AEII cells already in a smooth and averaged fashion. Specifically, using this approach, we found that the secretion of surfactant by AEII cells exhibits a collective behavior at the level of single cells.
The experimental observations in this study are in qualitative agreement with previous results, which indicated that a significant increase in extracellular surfactant was only observed long after the stretch stopped (12, 27). Our data not only quantify this delayed increase in stretch-induced secretion, but also demonstrate that large-amplitude cyclic stretch serves to inhibit surfactant secretion in AEII cells during and immediately after the stretching phase.
In selected groups, Western blot analysis of surfactant protein B, which is packed and secreted together with PC, demonstrated similar results to the lipids (2). This indicated that the measured radioactivity was of surfactant rather than cell membrane origin. Cells with damaged membranes, which were subsequently repaired by the 60-min time point, would also cause an increase in extracellular PC without indicating the damage during the live-to-dead ratio test. We note, however, that, if plasma membrane damage was a significant contributor to the increased PC secretion, this would also enhance the secretion during the longer term stretching protocols (30 and 60 min). In addition, the fraction of dead cells did not significantly change with time of stretch, which indicates that the released surfactant was a result of a cellular secretion rather than due to cell injury or death.
We modeled the secretion of surfactant from AEII cells to explain two key aspects of the experimental results: 1) during and immediately after stretch, cells secreted less surfactant than unstretched cells; and 2) cells stretched for 15 min secreted significantly more surfactant than unstretched cells after ∼45 min of rest. The former indicates that stretching suppressed surfactant secretion, while the latter implies that the system retained a memory of the stretch. The subsequent increase in secretion suggests that stretch indeed induces an enhancement of surfactant secretion, but the delay implies that the rate of secretion is in fact decreased.
In general, the release of surfactant from the cell would involve a sequence of steps, such as packaging the surfactant into LBs, transport of the LBs to the cell membrane, fusion of the LBs to the membrane to form a fusion pore, and opening of the fusion pore to release the surfactant (9). Each step in such a sequence would be dependent on the predecessors, and the dynamics of the process would depend on the dynamics of each individual step, as well as the stretch-induced changes of each step. However, this process is simplified if one of these steps is much slower than the others, where the slow step or bottleneck becomes the dominant step of the dynamics. In this case, all other processes are virtually instantaneous, and the overall dynamics of surfactant release can then be well approximated by the dynamics of the bottleneck step, regardless of the location of the bottleneck in the sequence. Moreover, the stretch response of the bottleneck becomes the only relevant determinant to the stretch response of surfactant release. Thus we restrict our modeling to a single equivalent “surface” compartment, which represents the slowest process in the surfactant secretory dynamics.
To better understand this bottleneck phenomenon, we examine a simple linear secretion process. Figure 7A shows a simple linear model described by the equations (13a) (13b) where the rate k and input flow ϕ could depend on the stretch. We assume that, during stretch, 0 ≤ t ≤ T, k → k*, and ϕ → Φ. Notice that, in the absence of stretch, t > T, k → k0, and ϕ → ϕ0. First, we note that, if the input flow ϕ is independent of stretch, that is Φ = ϕ0, the mass of secreted surfactant, mOut, would converge to that for the unstretched case after sufficient time has elapsed after the stretch. Thus the long-term amount of released surfactant cannot increase beyond that during the spontaneous release, if stretch only affects the rate constant k.
To mimic the experimental result, where mOut increases at a slower rate during stretch, we can assume that k decreases during stretch, k* < k0. At the same time, since mOut increases beyond the unstretched case after sufficient time, ϕ must increase with stretch, Φ > ϕ0. A salient property of a bottleneck is the formation of a reservoir of mass mS upstream the bottleneck, which can be controlled by k. During stretch, mS increases as a result of increased inflow Φ, as well as decreased outflow k mS. Once the stretch stops, this excess mass in the reservoir is released, and mOut increases. Figure 7B shows the dynamics of surfactant release from this simple linear model. We note that, using this model, we could match the unstretched case (solid curve), as well as the 15-min and 60-min time points when T = 15 min. However, the model is unable to match the 30-min time point for T = 15 min, as well as all the independent points for T = 30 min and 60 min. To estimate the quality of the fits, we calculated the root-mean-squared relative error for the linear model, as well as our jamming model for all data points and their corresponding model fits. The root-mean-squared relative error for the linear model was 40%, while that of the jamming model was 17%. The reason for this is that a single rate constant, k0, governs the release of surfactant from the reservoir. This rate is independent of the reservoir mass mS. We conclude that the dynamics of the secretion of surfactant is a fundamentally nonlinear process with memory.
The inability of the above general linear model to account for these dynamic features leads us to invoke a jamming model inspired by observed phenomena in the dynamics of vehicular traffic, escape panic, and related systems (7, 8, 18, 19). Simply, we hypothesized that stretch induces an increased current of surfactant from the interior of the cell to the exterior. However, this transport is mediated by a surface layer in the cell, which has a finite capacity due to the limited number of fusion pores. When the amount of surfactant in the surface layer approaches this capacity, there will be interference among LBs carrying the surfactant, and this interference causes a decrease in the amount of secreted surfactant per unit time and hence effectively creating a jam. When stretch stops, the jam takes an extended time to clear, and subsequently the amount of secreted surfactant increases. This process, therefore, also produces memory of the system.
We also note that, for small increases in the input flow, Φ < Φ*, the jamming model behaves like the simple linear model and no jamming occurs. However, once Φ > Φ*, the surface mass mS eventually exceeds the threshold mP, and the system enters a jammed phase, and the relation between outflow Q and mS reverses such that increased mS leads to decreased outflow. Once the stretch stops, the system remains in the jammed phase while mS > mP. The characteristic time T2 − T to recover from the jam after stretch ceases is proportional to the length of time T − T1 spent in the jammed phase during stretch, unlike the constant recovery time for the simple linear process. Thus this model is able to capture the salient features of the dynamics of surfactant secretion by AEII cells, including its temporary inhibition and the subsequent enhancement due to cyclic stretch (Fig. 2).
The model also provides several testable predictions. In the jammed state, the mass mS should increase, which could be directly observed following different stretch patterns. Although stretching for longer than 15 min does not show enhanced secretion within 1 h, our model suggests that such an increase should be observable at even longer times, unless other intracellular processes break down the activated but jammed LBs.
While the simplicity of the model allows analytic solutions, it is also accompanied by several limitations. First, we modeled the cell population by the dynamics of a single representative cell. This mean field approach neglects the difference in the response of individual cells, as well as their known interaction (9). We thus numerically explored the effect of heterogeneous cell sizes and the effect of nonuniform stretch. In both cases, the time course of surfactant secretion remains qualitatively similar, although the secretion process starts somewhat earlier and ends later after the cessation of stretch. This is due to the fact that larger cells or cells experiencing smaller stretches are less jammed than smaller cells or cells experiencing larger stretches. Cells that are less jammed can clear their excess surfactant quicker than cells that are more jammed. It is also worth noting that the effects of heterogeneous cell size and heterogeneous cell stretch on secretion dynamics are similar (Fig. 6), and hence it is unlikely that they could be experimentally resolved by simply observing bulk secretion.
In addition, we do not account for the uptake of the secreted surfactant, assuming that its low extracellular concentration (<10%) has a negligible effect on the dynamics. This is reasonable given that, in the present study, as well as in our recent experimental study, we found little effect of stretch on surfactant uptake, as shown in Table 2 (3). Our model also does not explicitly account for the physical or chemical interaction among LBs, but such interference is implicitly taken into account as a jamming process. It is known that various chemical substances stimulate surfactant secretion (23). While the effect of stretch was incorporated into ϕ(t) by increasing it from ϕ0 to Φ, we can also think of the change in ϕ(t) as a result of chemical stimulation. Therefore, it is possible that jamming would occur during chemical stimulation. Indeed, in neuronal cells, synaptic endocytosis was shown to be severely impaired after strong stimulation (13), which was interpreted as traffic jams at synapses (26). In AEII cells, a similar mechanism may take place. Visual inspection of Fig. 1A in the study by Frick et al. (14) reveals clusters of stimulated LBs just under the cell membrane after stimulation with ATP. Additionally, cell-cell interactions, either mechanical or through signaling that can modify the secretion, is not considered in the model. However, it is thought that type I epithelial cell signaling plays an important role in the secretory response of AEII in vivo (20). Finally, the biophysical and biochemical properties of the underlying substrate may also influence secretion (4). Thus the applicability of our results may be limited to the pure AEII cell culture, and this issue warrants further experimental verification.
The piecewise-linear fundamental diagram with a single peak (Fig. 3) describes the average jamming behavior of LBs and does not specify the mechanism that leads to jamming. Fusion pores, through which the surfactant is released from the LBs, are dynamic, rate-limiting structures (16), and hence their ability to stay open could be hampered by the presence of large queues of LBs. Regulated surfactant secretion through fusion pores requires specific membrane-bound target SNARE (soluble N-ethylmaleimide-sensitive factor attachment protein receptors) proteins called SNAP-23 and syntaxin-2 (1). Recently, it was shown that syntaxin molecules in the plasma membrane naturally self-organize into clusters due to a weak attractive interaction between the molecules, but the size of the clusters is limited by crowding-induced repulsion (24). We speculate that this mechanism organizes the available syntaxin in the membrane into a finite-number docking sites, allowing jamming to occur when secretion is strongly stimulated. Stretch could directly influence these docking protein clusters together with the fusion pore opening dynamics. Stretching is known to affect the openings of calcium channels that are required for secretion (27). At high concentrations, LBs could also form large aggregates, which would take a longer time to empty through the fusion pores. Thus, although jamming provides a simple unified mechanism to explain the delayed enhancement of secretion in response to stretch, alternate models involving more specific time-dependent responses of the various subsystems of the secretory pathway could also lead to similar results.
Despite the above limitations, our model captures the key features of the dynamics of surfactant secretion observed under the current experimental conditions. The proposed mechanism of jamming highlights the importance of dynamics in cellular secretory response to applied stretch. In several diseases, such as respiratory distress syndrome in premature infants (25), where the surfactant pool is not sufficient to maintain a physiologically appropriate low level of surface tension in the alveoli, it is often desirable to quickly replenish the surfactant pool, which has either been depleted or rendered ineffective (17). Additional experiments mapping the effects of both timing and amplitude of stretch could make it possible to tune stretch patterns for avoiding the jammed state and hence maximizing surfactant release. It is possible that jamming is avoided during variable stretch patterns that have been reported to increase surfactant release (3). Finally, jamming could also be relevant to the dynamics of stimulated secretion by other means, as well as by other cells in vivo, such as cells in the vascular or endocrine systems.
This study was supported by National Heart, Lung, and Blood Institute (HL-098976).
No conflicts of interest, financial or otherwise, are declared by the author(s).
Author contributions: A.M., S.P.A., E.B.-S., and B.S. conception and design of research; A.M., S.P.A., and H.P. analyzed data; A.M., E.B.-S., and B.S. interpreted results of experiments; A.M. prepared figures; A.M. drafted manuscript; A.M., E.B.-S., and B.S. edited and revised manuscript; A.M., S.P.A., E.B.-S., H.P., and B.S. approved final version of manuscript; S.P.A., E.B.-S., and B.S. performed experiments.
- Copyright © 2012 the American Physiological Society