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* Department of Electrical and Computer Engineering, Johns Hopkins University, Baltimore, Maryland 21218; and
Department of Cell Biology, Johns Hopkins University School of Medicine, Baltimore, Maryland 21205
Correspondence: Address reprint requests to Pablo A. Iglesias, Tel.: 410-516-6026; Fax: 410-516-5566; E-mail: pi{at}jhu.edu.
| ABSTRACT |
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| INTRODUCTION |
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During directional gradient sensing, eukaryotic cells such as Dictyostelium and neutrophils exhibit extraordinary sensitivity to external chemical gradients. By monitoring the translocation of green fluorescent protein (GFP)-tagged plekstrin homology (PH) domains, which bind to phosphatidylinositol 3,4,5-trisphosphate (PI(3,4,5)P3), as well as the enzymes that regulate PI(3,4,5)P3 production, it has been shown that signaling components are sharply localized at the leading edge when the chemoattractant concentration across the cell length can differ by as little as 5% (Parent and Devreotes, 1999
; Servant et al., 2000
; Chung et al., 2001
; Dormann et al., 2002
). This indicates that the intracellular signal transduction pathway can amplify a shallow signaling input into a much steeper internal response. Moreover, cells treated with inhibitors of actin polymerization, which removes polarization and immobilizes them, still show amplified responses, though the amplification is smaller than in polarized cells (Parent et al., 1998
; Servant et al., 2000
; Janetopoulos et al., 2004
).
Because the upstream signaling components and biochemical reactions, such as receptor occupancy, G-protein subunits, and G-protein activation, are uniformly distributed along the perimeter of a cell during directional sensing, the response must become highly localized in events between the G-protein and PI(3,4,5)P3 (Xiao et al., 1997
; Servant et al., 1999
; Jin et al., 2000
; Janetopoulos et al., 2001
; Ueda et al., 2001
). The complementary regulation of two classes of enzymes that govern the metabolism of PI(3,4,5)P3, the phosphoinositide 3-kinase (PI3K) and tensin homology protein (PTEN), likely play a role in this amplification (Funamoto et al., 2002
; Iijima and Devreotes, 2002
; Huang et al., 2003
; Janetopoulos et al., 2004
). Upon uniform cAMP stimulation, PI3K rapidly translocates from the cytosol to the plasma membrane and then dissociates with kinetics similar to those of PH-domain containing proteins. In contrast, PTEN, which is initially localized to the plasma membrane, dissociates transiently to the cytosol and returns to its original configuration within a few minutes. When a cell is exposed to a cAMP gradient, PI3K localizes to the front membrane whereas PTEN localizes to the rear sides and posterior membrane. Proper balance between the PI3Ks and PTEN is critical for local accumulation of PI(3,4,5)P3 as well as further signaling events that lead to pseudopodia production (Funamoto et al., 2002
; Iijima and Devreotes, 2002
). The receptor regulation of these enzyme movements occurs in both polarized and unpolarized cells, though they are not as dynamic in polarized cells (Janetopoulos et al., 2004
).
Recent experimental quantification of the external chemoattractant gradient and the internal localized response provides a means for designing and validating mathematical models (Janetopoulos et al., 2004
). Direct measurements of the gradient of the fluorescent Cy3-cAMP, and a readout of the binding of PH-GFP, PI3K-GFP, and PTEN-GFP to the cell membrane, have shed light on the amount of amplification between stimulus and response during gradient sensing. These experiments provide a means for quantitatively testing the predictive nature of a number of gradient sensing models. We propose a model that accounts for the observed transient localization of PI3K and PTEN during persistent homogeneous chemoattractant stimulation. The complementary regulation of PI3K and PTEN explains the observed amplification of membrane lipid PI(3,4,5)P3 in immobilized cells in a chemotactic gradient. Using this model, we duplicate the observed response of several mutants. Moreover, we predict the cellular response to several complex combinations of temporal and spatial stimuli.
| MATERIALS AND METHODS |
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The first LEGI mechanism generates PI3K binding sites on the membrane as described in Huang et al. (2003)
. The molecule responsible for fast excitation (EPI3K) is confined to the membrane, whereas the slower inhibitory molecule (IPI3K) is allowed to diffuse freely in the cytoplasm. This mechanism results in a transient increase of PI3K binding sites in response to uniform stimulus, and an accumulation of PI3K binding sites on the side of the cell facing the chemoattractant gradient. Images of fluorescently tagged PI3K distribution show that the PI3K gradient at the leading edge is slightly sharper than the external cAMP gradient (Funamoto et al., 2002
; Janetopoulos et al., 2004
). To account for this, we assume that the reaction dynamics governing the activation of the PI3K binding sites follows Michaelis-Menten kinetics with a Hill coefficient of 2. This limited positive cooperativity is used in our model to generate the initial amplification observed in PI3K binding (see supplementary material).
PTEN binding sites are controlled by a second LEGI mechanism using separate excitation (EPTEN) and inhibition (IPTEN) molecules (Fig. 1 A). In this case, however, the response regulator destroys active binding sites. This results in a transient depletion of membrane binding sites for PTEN under uniform stimulation and a localization of binding sites for PTEN at the posterior membrane under graded inputs. Our earlier findings (Janetopoulos et al., 2004
) indicate that PTEN and cAMP concentrations are inversely correlated, and thus we have assigned a linear inhibition of PTEN binding sites.
Our model structure assumes no cross talk between the two channels of binding/activation of PI3K and PTEN. Biochemically, it has been shown that PI3K activation is independent of PTEN (Huang et al., 2003
). The regulation of PTEN binding is also independent of PI3K and PI(3,4,5)P3 levels (Iijima et al., 2004
).
Specifications and conditions of the model
| RESULTS |
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20% of basal membrane-bound PTEN remains. After 80 s, 90% of this PTEN returns to the membrane. For both enzymes, the membrane localization mirrors closely the existence of binding sites on the membrane, owing to the high KD and fast off-rate chosen for these binding events. The complementary behavior of membrane binding mirrors the transient localization of PI3K-GFP and PTEN-GFP observed experimentally in response to uniform cAMP (Funamoto et al., 2002
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Spatial regulation
A cell's ability to detect static spatial gradients can be observed experimentally by exposing Dictyostelium cells treated with latrunculin, an inhibitor of actin polymerization, to a micropipette containing cAMP (Parent and Devreotes, 1999
). Recent quantitative analysis of a series of these micropipette-assay experiments has made it possible to validate our model (Fig. 3 A and Janetopoulos et al., 2004
). Spatial sensing is simulated by placing a circular cell of diameter 14 µm at the center of a 26 x 26 µm environment where a source with 1 µM cAMP is introduced in one corner. The cAMP diffuses away from the source and creates a concentration gradient around the cell perimeter (Fig. 3 B). A representative simulation result of membrane-associated PTEN, PI3K, and PI(3,4,5)P3 illustrates that, at steady state, PI3K and PI(3,4,5)P3 accumulate at the front, whereas PTEN localizes at the rear in response to the cAMP gradient (Fig. 3, CE). To compare the gradient of different components along the cell periphery, intensities of PTEN, PI3K, and PI(3,4,5)P3, normalized to their maximum values, are plotted in polar coordinates and compared with experimentally obtained fluorescent levels (Fig. 3 F). In this simulation, the shallow external cAMP gradient gives rise to a slightly amplified membrane-bound PI3K gradient. Membrane-bound PTEN, on the other hand, is inversely distributed on the membrane, away from the micropipette. This complementary regulation elicits a sharp PI(3,4,5)P3 gradient. Qualitatively, the model demonstrates the membrane distribution of PTEN, PI3K, and PI(3,4,5)P3 observed in previous experiments (Funamoto et al., 2002
; Iijima and Devreotes, 2002
; Huang et al., 2003
).
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To determine how the shape and size of the cAMP gradient affects the PI(3,4,5)P3 concentration profile, we simulated various situations in which either the position or the cAMP concentration of the micropipette is varied (Fig. 4 A), and monitor PI(3,4,5)P3 distribution along the membrane (Fig. 4 B). These simulations show that the shape of the PI(3,4,5)P3 response is affected both by the shape of the cAMP gradient as well as its midpoint concentration. Thus, two gradients having the same shape can elicit vastly different responses. For example, the cells in b and c have cAMP profiles with approximately the same shape and absolute gradient (the difference in concentrations between the maximum and minimum in Fig. 4 A). However, the cell in c has a higher response (Fig. 4 B) because the mean (global) level of chemoattractant is higher. Similarly, the cell in a has a large absolute cAMP gradient but the PI(3,4,5)P3 response is relatively muted because the mean level of cAMP is also very high. In the LEGI mechanism, the response depends on the ratio of excitation over inhibition (see supplementary material), which mirror local and global receptor occupancies, respectively. Thus, when the data from these simulations is plotted in terms of relative concentrations, all four cases yield essentially the same curve (Fig. 4 C). It is known that the overall chemotactic response depends on the relative gradient steepness (Zigmond, 1977
; Fisher et al., 1989
). The simulation results suggest that this feature is mediated by PI(3,4,5)P3, and agree with our recent experimental results (Janetopoulos et al., 2004
).
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| DISCUSSION |
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The model exhibits several important features of the chemotactic, spatial sensing response that we have demonstrated recently (Janetopoulos et al., 2004
) and that are missing in other models proposed to explain gradient sensing (Meinhardt, 1999
; Narang et al., 2001
; Postma and Van Haastert, 2001
; Rappel et al., 2002
). Our model shows that the spatial distribution of the response is affected by the chemoattractant gradient, so that steeper gradients elicit more localized responses than shallower gradients. Similarly, the midpoint cAMP concentration affects the degree of localization since the response depends on the relative gradient (Janetopoulos et al., 2004
). Both these features are direct consequences of the LEGI mechanisms. In contrast, several other models predict a steady-state response that is invariant with respect to the mean value and relative gradient of the chemoattractant concentration profile (Meinhardt, 1999
; Narang et al., 2001
), whereas others cannot account for the cell's ability to sense gradients of increasing midpoint concentration (Postma and Van Haastert, 2001
). Our model also shows that the rear of a cell in a gradient remains responsive to further stimulation, be it spatial or temporal. These features agree with our recent experimental findings on latrunculin-treated cells (Janetopoulos et al., 2004
). Other proposed models suggest that the rear of the cell becomes inhibited and so would not be able to sense further stimuli (Rappel et al., 2002
). The simulation shown in Fig. 6 also explains the observed behavior in a recent experiment (Janetopoulos et al., 2004
), and in doing so, provides support for the existence of a receptor-mediated, slower inhibitory process. The extinguishing of the PI(3,4,5)P3 response at the front of the cell after the removal of the uniform cAMP stimulus is a result of the slower decrease in the concentration of the inhibitor, relative to that of the excitation process, in response to a decrease in receptor occupancy.
The adaptation achieved through the LEGI mechanism is not affected by model parameter values and hence is a robust process. However, it is also known that the external gradient is not amplified with a single LEGI regulator (Iglesias and Levchenko, 2002
; Levchenko and Iglesias, 2002
). To introduce high amplification, a positive feedback mechanism can be added downstream of the standard LEGI mechanism. The resulting model inherits robust adaptation from the LEGI regulator, but the amplification performance is very sensitive to parameter values. Other methods of achieving amplification that are not sensitive to parameter variations have been considered (Meinhardt, 1999
; Narang et al., 2001
; Postma and Van Haastert, 2001
). However, because of the hysteretic nature of their response, these models cannot account for the response seen in unpolarized Dictyostelium to rapidly changing sources (Iglesias and Levchenko, 2002
; Devreotes and Janetopoulos, 2003
). In contrast, the model presented in this article, through the dual spatial sensing mechanisms, exhibits robust adaptation as well as redundant amplification. From a biological standpoint, this mechanism offers considerable advantages as it allows a cell to sense gradients, and hence chemotaxthough perhaps with reduced efficiencyeven if the function of one of the two regulators is missing or impaired, as has been experimentally observed (Funamoto et al., 2002
; Iijima and Devreotes, 2002
).
In our model, we assume cooperative activation of PI3K with a Hill coefficient of 2 and linear inhibition for PTEN, both of which are activated by receptor occupancy. These model parameters were chosen so that the concentration of PI3K is proportional to the square, and the concentration of PTEN is inversely proportional to the first power of normalized cAMP concentration, respectively, to agree with our experimental data (Iijima et al., 2004
; Janetopoulos et al., 2004
). The need for cooperativity in PI3K binding suggests that additional regulatory elements exist. The resulting concentration of PI(3,4,5)P3 is proportional to the cubic power of normalized cAMP concentration, also in agreement with our experimental data observed in nonpolarized cells (see supplemental material).
The effect of varying cell geometry on the model was tested by importing various images of polarized cells into the Virtual Cell environment and simulating the cellular response. The simulations predicted that polarized cells exhibit slightly greater gradient amplification than the spherical cells (data not shown). Since no biochemical data were changed in the model, these results show that the streamlined cell morphology associated with moving cells can enhance the spatial heterogeneity of the PI(3,4,5)P3 distribution. However, when we compare the simulation to experimental data (Janetopoulos et al., 2004
), we find that not all the experimentally observed amplification is achieved by the model. The experimental and virtual setups differ in several aspects. In vivo, neither the shape of the moving cell nor the observed chemotactic gradients is constant; this influences the observed response. In contrast, in our simulation, the polarized cell is assumed immobile in a static chemoattractant gradient. These differences between model and experiment do not arise in the spherical, static cells where a strong match between theory and experiment is observed. Nevertheless, our simulations suggest that there are additional amplification steps in the regulatory pathway of polarized cells. A positive feedback loop involving actin polymerization has been suggested (Weiner et al., 2002
). This loop would have no effect on the immobilized cells, and might help to account for the missing amplification in the polarized cells. A positive feedback loop involving mild hysteretic effect may also explain some cell's ability to remain polarized even in the absence of external gradients (Devreotes and Janetopoulos, 2003
).
Our simulations predict cellular responses to stimuli that are not easily implemented experimentally. For example, our model makes a very strong prediction as to the behavior expected when a fraction of the cell membrane is exposed to saturating concentrations of cAMP, but the rest of the cell is unstimulated. The cell experiences no chemoattractant gradient, only a steplike change in concentration. The predicted response suggests that a chemoattractant gradient is not necessary for a static spatial response. The inhibitory molecules acting in each LEGI mechanism diffuse away from the region of the cell membrane where they are activated, allowing a cellular response to develop (Fig. 7 E). Because the inhibitor is created by receptor occupancy, as the fraction of the cell stimulated is decreased, the total number of inhibitor molecules created is smaller. Moreover, since they diffuse around the whole cell membrane, the concentration at any one point along the membrane decreases. This explains the increase in the local response seen in Fig. 7. To our knowledge, this experiment has not been performed, but could be attempted using a clamp or microfluidic device (Dertinger et al., 2001
) to stimulate only a fraction of the cell. Experimental determination of the cellular response would help greatly in our understanding of the chemotactic behavior of cells. Were the behavior predicted here to be observed, this experiment would provide further evidence for the existence of a receptor-mediated global inhibitor.
Although our simulations provide cellular responses that mirror most of the observed response of directional sensing Dictyostelium cells, there are several features that are not accounted for.
First, as stated at the outset, our model does not explain the other processes involved in gradient sensing, polarization, and movement. Polarization is known to have an effect on the accumulation of PI(3,4,5)P3, as it leads to greater amplification and the desensitization of the cell's rear (Jin et al., 2000
; Janetopoulos et al., 2004
). Although our model can accurately explain gradient sensing in latrunculin-treated cells, aspects of other models may be needed to account for the observed differences in the responses between treated and untreated cells.
Second, chemoattractant stimulation elicits a localized, second phase of PI(3,4,5)P3 accumulation on the membrane (Chen et al., 2003
; Postma et al., 2003
). The mechanics that underlie the two phases are unknown and are not taken into account in these models.
Thirdly, specific biochemical entities have not been assigned to the excitation (EPI3K, EPTEN) or inhibition (IPI3K, IPTEN) processes. All four of these processes must be mediated by receptor occupancy. The two excitation processes must mirror receptor occupancy so they could be expected to be bound near the G-protein. In contrast, the inhibitory processes should be diffusible to provide a global signal. These properties allow us to speculate on possible candidates. For PTEN, it is known that a putative N-terminal PI(4,5)P2 binding motif is necessary for binding to the membrane (Iijima et al., 2004
). Thus, the excitation process for PTEN (EPTEN) may represent a receptor-mediated decrease in the binding affinity of the PI(4,5)P2 binding motif. A conformational change in PTEN, possibly phosphorylation (Vazquez et al., 2001
; Das et al., 2003
), could also affect this binding affinity. If this change takes place while PTEN is in the cytosol, this would represent a global signal and thus serve as the inhibitor in the PTEN LEGI mechanism. For the PI3K LEGI mechanism, several candidates exist for the excitation and inhibition processes. It is known that PI3K activation depends on Gß
, and that the PI3Ks contain Ras binding motifs. Moreover, an N-terminal fragment of PI3K is sufficient for binding to the membrane. Molecules that may be involved as inhibitors in the LEGI mechanisms include the G-protein
-subunit, G
9, which is believed to play a role in adaptation (Brzostowski et al., 2002
) and RCK1 (Sun and Firtel, 2003
) (see Manahan et al., 2004
).
Finally, recent experiments suggest that Dictyostelium cells do not adapt perfectly when stimulated uniformly (Postma et al., 2003
; Postma et al., 2004b
). Although our simulation parameters have been chosen to adapt perfectly or nearly perfectly, our model of dual regulation through complementary LEGI mechanisms does not require this perfect adaptation. If we allow the parameter values to change (as described in the supplementary material), perfect adaptation can be lost. However, spatial sensing is still possible, though at a reduced efficiency.
| SUPPLEMENTARY MATERIAL |
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| ACKNOWLEDGEMENTS |
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Submitted on June 9, 2004; accepted for publication September 22, 2004.
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