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Eukaryotic Cell, February 2003, p. 62-75, Vol. 2, No. 1
1535-9778/03/$08.00+0 DOI: 10.1128/EC.2.1.62-75.2003
Copyright © 2003, American Society for Microbiology. All Rights Reserved.
W. M. Keck Dynamic Image Analysis Facility, Department of Biological Sciences, University of Iowa, Iowa City, Iowa 52242,1 Department of Biology, University of California, San Diego, La Jolla, California 920392
Received 27 August 2002/ Accepted 28 October 2002
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| RegA
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PKA, which emanates from the front of a wave. The results demonstrate that cells must suppress PKA activity in order to elongate along a substratum, suppress lateral-pseudopod formation, and crawl and chemotax efficiently. The results also implicate PKA activation in dismantling cell polarity at the peak and in the back of a natural cAMP wave. |
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FIG. 1. Model describing cell behavior in the different phases of the natural wave and the relationship of the wave to the basic motile behavior of a cell. The wave is separated into four phases, A, B, C, and D. Descriptions of the behavior of cells in each phase and the characteristics of the wave responsible for these behaviors were derived from previous studies (29, 37, 38, 40, 41, 47, 49). Vertical arrows represent regulatory pathways emanating from the different phases of the wave which target machinery involved in basic motile behavior, leading to the cell behaviors specific to each phase of the wave (29).
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Maintenance and development of strains. Cells of the parental Ax4 strain and the pkaR mutant strains DG1075, 108d2, and 108d3 were frozen in 7.5% dimethyl sulfoxide in HL-5 medium and stored at -80°C (33). For experimental purposes, cells were reconstituted every 3 weeks from stock cultures by being grown in suspension in HL-5 medium. Mutant strains were maintained in HL-5 medium supplemented with 5 µg of Blasticidin S/ml for mutant selection. For experimental purposes, mutant cells were grown for one generation in the absence of the drug. To initiate development, cells were grown to a density of 2 x 106 to 5 x 106 cells per ml, washed free of nutrients in basic salts solution (BSS; 20 mM KCl, 2.5 mM MgCl2, and 20 mM KH2PO4 [pH 6.4]), and then dispersed onto filter pads saturated with BSS as a smooth carpet at a density of 5 x 106 cells per cm2 (26). For motility experiments in buffer and in spatial and temporal gradients of cAMP (see below), cells were harvested at the ripple stage, which represents the onset of aggregation under these conditions (25). The ripple stage occurred in pkaR mutant cultures approximately 1 h earlier than in control cultures under the conditions employed.
Analysis of basic motile behavior. The methods for analyzing the basic motile behavior (Fig. 1) of cells have been described previously in detail (41, 47, 48). In brief, cells were inoculated into a Sykes-Moore chamber (Bellco Glass, Vineland, N.J.), the chamber was inverted and positioned on the stage of an upright microscope, and cell behavior was viewed through a 10x or 25x objective. The chamber was perfused with buffer at a rate that turned over the liquid volume every 15 s.
Analysis of cell motility in spatial and temporal gradients of cAMP. The methods for analyzing in two dimensions (2D) the behavioral responses of cells to spatial and temporal gradients of cAMP have been described in detail previously (36-38, 41, 47, 48). To monitor in three dimensions (3D) the behavior of individual amoebae responding to simulated temporal waves of cAMP, 350 µl of a dilute suspension of cells was inoculated into a Dvorak-Stotler chamber (Lucas-Highland Inc., Chantilly, Va.) as previously described (42). The chamber was positioned on the stage of a Zeiss ICM 405 inverted microscope equipped with differential interference contrast optics and a Planapo 63x oil immersion objective. To obtain optical sections of the cells for 3D reconstruction (11, 31, 46), the coarse-focus knob of the microscope was connected to a customized stepper motor. Sixty optical sections were automatically collected in 2 s from the z axis at 0.3-µm increments. This process was repeated at 5-s intervals. Images were recorded onto digital videotape through a cooled charge-coupled-device camera (Zeiss Inc., Thornwood, N.J.) and subsequently transferred into a Macintosh computer equipped with a Data Translation (Marlboro, Mass.) frame grabber board capable of acquiring images at 30 frames per s with Adobe Premiere software (Adobe Systems Inc., San Jose, Calif.).
Analysis of cell behavior after rapid addition of 1 µM cAMP. The methods for analyzing the response of cells to the rapid addition of 1 µM cAMP, the peak concentration in the natural wave, have previously been described in detail (42, 48).
Analysis of cell motility in natural aggregation territories. To analyze the behavior of cells in natural aggregation territories, exponentially growing cells were washed free of nutrients and suspended in BSS at a concentration of 2.4 x 106 cells per ml according to methods previously described (9). Wave propagation was analyzed by using the vector flow program of DIAS (9, 11, 31). The user selects a rectangular region of interest and the direction toward the aggregation center. When no aggregation center was apparent, an arbitrary point was selected. The behavior of each cell in the rectangle was converted into a vector, the length of which was proportional to the extent of translocation and the direction of which was the average for the cell track in the period of analysis. The vectors in the selected rectangular region were smoothed in a Tukey window to remove noise and artificial vectors. The magnitudes of the vector components parallel to the selected direction were averaged and plotted over time to form a vector flow plot. In a vector flow plot, the x axis represents time and the y axis represents the direction and extent of the displacement of cells in an aggregation territory.
Analysis of mutant cells in wild-type cell territories. To test the behavior of mutant cells in wild-type cell aggregation territories, pkaR mutant cells were stained with the vital dye DiI (Molecular Probes, Inc., Eugene, Oreg.) and mixed with unlabeled Ax4 cells (10% pkaR mutant cells and 90% Ax4 cells) and their motion during aggregation was analyzed according to methods previously described (47, 48). Cells were imaged with a laser scanning confocal microscope (NORAN, Middleton, Wis.). Transmitted light images were continuously collected through a transmitted light detector. Settings in Oz Intervision software (NORAN) were selected so that cells were exposed for 0.5 s every 20 s to laser light at an intensity of 20% and at an excitation of 568 nm and an emission of greater than 590 nm.
2D computer-assisted analysis. Cell behavior was either directly digitized or videorecorded and subsequently digitized into DIAS data files. Perimeters of cells in buffer, in spatial gradients of cAMP, in simulated temporal waves of cAMP, or in natural waves of cAMP were automatically outlined in 2D by using primarily the gray-scale threshold option of the DIAS program (27, 30, 31). Outlines were then converted to beta-spline replacement images that were used to compute motility and dynamic morphology parameters described in detail elsewhere (27, 30).
3D reconstruction and motion analysis. The reconstruction of a 3D faceted image of the cell surface and the computation of 3D parameters are described elsewhere in detail (11, 31, 46). Briefly, the perimeter of the in-focus portion of the image in each optical section was automatically outlined by 3D-DIAS software by using a pixel complexity algorithm (30, 31). The interface between the particulate cytoplasm of the main cell body and the nonparticulate cytoplasm of the pseudopodial extensions was readily identified in differential interference contrast images of optical sections. The distal nonparticulate zones of all pseudopods were manually outlined at the in-focus portions of each optical section to generate a faceted 3D reconstruction of pseudopods that were color-coded red and inserted into the faceted cell image (46). The faceted image of the cell with the color-coded pseudopods could be viewed at any angle dynamically in 3D through a Crystal Eyes 3D display station (Stereographics, San Raphael, Calif.). The 3D position of the centroid of the cell was computed by averaging the x, y, and z coordinates of all points interior to the 3D faceted cell image. 3D motility and dynamic morphology parameters have been previously described in detail (27).
Fluorescent microscopic analysis of myosin II, F-actin, and tubulin. For actin and myosin II localization, cells were fixed with 4% paraformaldehyde in 10 mM MES (morpholineethanesulfonic acid) buffer (pH 6.1) with 138 mM KCl, 3 mM MgCl2, and 2 mM EGTA to preserve the cytoskeletons. For tubulin localization, cells were fixed in Pen-Fix (Richard-Allan Scientific, Kalamazoo, Mich.). In both protocols, cells were fixed for 10 min at room temperature. Prior to immunostaining of cells for myosin II, antigen retrieval was performed by processing cells in Target retrieval solution (Dako Corp., Carpinteria, Calif.) in a steamer for 20 min at 90°C according to the manufacturer's recommendations. The polyclonal anti-myosin II antibody was a generous gift from Arturo De Lozanne (University of Texas at Austin). Tubulin immunolocalization was performed with the monoclonal antibody 12G10, obtained from the Developmental Studies Hybridoma Bank at the University of Iowa. To block nonspecific binding, cells were first treated with 10% normal goat serum in Tris-buffered saline (TBS). Cells were then incubated with rabbit anti-myosin II antibody (dilution, 1/1,000) or mouse anti-tubulin antibody (undiluted) in TBS for 45 min at 37°C. After being extensively rinsed with TBS, cells were stained with fluorescein isothiocyanate-labeled goat anti-rabbit antibody (dilution, 1/200) or goat anti-mouse antibody (Jackson ImmunoResearch, West Grove, Pa.) for 30 min at room temperature. Cells were stained for F-actin with Oregon Green-phalloidin (Molecular Probes, Inc.) according to methods previously described (42). Coverslips were mounted by using Moviol (Sigma, St. Louis, Mo.) with azide. Images were captured with a Zeiss LSM 510 laser scanning confocal microscope in the Central Microscopy Facility at the University of Iowa.
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FIG. 2. pkaR mutant cells are defective in natural aggregation. The behavior of wild-type (Ax4) (A) and pkaR mutant (108d3) (B) cells in monolayers on nonnutrient agar was analyzed. For each cell type, a representative field of cells was videorecorded for 120 min and their motion was analyzed with the 2D-DIAS vector flow program (19, 28). For each cell type, representative video images at 20, 60, and 100 min are shown. In the vector flow plots, the magnitudes of the vector components parallel to the selected direction of the aggregation center for Ax4 cells and parallel to an arbitrary direction for 108d3 cells were averaged and plotted over time. The x axis represents time, and the y axis represents the direction (+ or -) and extent of the displacement of cells. Note that while Ax4 cells form streams, pkaR mutant cells do not and that while Ax4 cells exhibit cyclic surges toward the aggregation center, pkaR mutant cells do not.
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FIG. 3. pkaR mutant cells are impaired in their response to natural cAMP waves. The behavior of individual wild-type (Ax4) and pkaR mutant (DG1075 [1075] and 108d3) cells in aggregation territories composed of 90% Ax4 cells and 10% mutant cells was analyzed. In the top of each panel, a plot of the instantaneous velocity of the representative cell under analysis is shown, and at the bottom of each panel a centroid track is presented. The instantaneous velocity plots were smoothed 10 times with Tukey windows of 10, 20, 40, 20, and 10. The arrows denote the direction toward the aggregation center assessed from the behavior of the predominant Ax4 cells. For each pair (A and B and C and D), the Ax4 cell was the closest neighbor to the analyzed pkaR mutant cell. per, average period of velocity peaks in minutes; pk, average peak velocity in micrometers per minute; tr, average trough velocity in micrometers per minute; Inst. Vel., instantaneous velocity; Agg. Center, aggregation center.
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TABLE 1. 2D-DIAS analysis of the behavior of pkaR mutant cells in buffera
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30°. While Ax4 cells translocating in buffer formed lateral pseudopods at an average frequency of 4 per 10 min, 108d3 and DG1075 cells translocating in buffer formed lateral pseudopods at approximately twice that frequency, 9 and 8 per 10 min, respectively (Table 2). Together, these 2D results demonstrate that pkaR mutant cells in buffer are rounder and slower and form lateral pseudopods more frequently than wild-type cells. |
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TABLE 2. 2D-DIAS analysis of lateral-pseudopod formation by pkaR mutant cells and control cells in buffer and in a spatial gradient of cAMPa
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TABLE 3. 2D-DIAS analysis of the behavior of pkaR mutant cells in a spatial gradient of cAMPa
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FIG. 4. Computer-generated perimeter tracks reveal that pkaR mutant cells translocate at lower velocities and turn more often than Ax4 cells in a spatial gradient of cAMP. Tracks of the three Ax4 cells (A) and the three pkaR mutant cells (B and C) with the highest chemotactic indices are shown. Cell perimeters were drawn every 4 s. 1075, DG1075.
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FIG. 5. pkaR mutant cells behave aberrantly in the front of temporal waves of cAMP. The instantaneous velocities (Inst. Vel.) of a representative Ax4 cell (A), a representative 108d3 cell (B), and a representative DG1075 (1075) cell (C) during four simulated temporal waves of cAMP generated in a perfusion chamber are plotted as a function of time. The concentration of cAMP (cAMP Conc.; top lines), estimated in dye experiments, is presented as a function of time through the four waves. Instantaneous velocity plots were smoothed 10 times with Tukey windows of 10, 20, 40, 20, and 10. Note that, unlike the Ax4 cell, pkaR mutant cells do not exhibit a velocity surge in the front of waves 2, 3, and 4.
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TABLE 4. pkaR mutant cells fail to suppress lateral-pseudopod formation in the front of simulated temporal waves of cAMP
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FIG. 6. 3D reconstructions of a representative Ax4 cell in the front (A), at the peak (B), and in the back (C) of a simulated temporal wave of cAMP generated in a perfusion chamber. Nonparticulate pseudopodial zones are demarcated in red. The cell is viewed at each time point at angles of 15 and 60° from the surface. Note that the Ax4 cell is elongate along the substratum in the front of the wave, rounds up and retracts the dominant pseudopod at the peak of the wave, and resumes pseudopod formation but in all directions and without cell elongation in the back of the wave. The behavior of this cell is representative of that of nine additional Ax4 cells reconstructed in 3D in a similar fashion.
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FIG. 7. 3D reconstructions of a representative pkaR mutant cell in the front (A), at the peak (B), and in the back (C) of a simulated temporal wave of cAMP generated in a perfusion chamber. Nonparticulate pseudopodial zones are demarcated in red. The cell is viewed at each time point at angles of 15 and 60° from the surface. Note that pkaR mutant cells remain ovoid throughout the three phases of the wave. Note also that pkaR mutant cells retract the dominant pseudopod at the peak of the wave and resume apolar pseudopod formation in the back of a wave. The behavior of this cell is representative of that of nine additional pkaR mutant cells reconstructed in 3D in a similar fashion.
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FIG. 8. pkaR mutant cells in buffer respond in an apparently normal fashion to the rapid addition of 1 µM cAMP. Centroid tracks of three representative Ax4 (A) and three representative pkaR mutant (108d3) (B) cells responding to the rapid addition of 1 µM cAMP are shown. The total track, that portion of the track before the addition of cAMP (in buffer), and that portion of the track after the addition of cAMP are shown for each representative cell. Inst. Vel., instantaneous velocity; Rnd., roundness parameter.
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FIG. 9. The organization of the cytoskeletons of pkaR mutant cells appears normal in buffer and in the front of a temporal wave of cAMP. Representative Ax4 and pkaR mutant (108d3) cells in buffer and in the front of the third in a series of four temporal waves of cAMP were stained for F-actin (A to H), myosin II (I to P), and tubulin (Q to W). a, anterior end; u, uropod. Bars, 10 µm.
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PKA is activated by intracellular cAMP, which binds to the regulatory subunit, causing it to dissociate from the catalytic subunit. The dissociated catalytic subunit represents the active form of this kinase. Therefore, it has been hypothesized that PKA activity oscillates in phase with the concentration of internal cAMP through the natural wave (13), increasing in activity in conjunction with increasing intracellular cAMP concentration and decreasing with decreasing intracellular cAMP concentration. Preliminary measurements of PKA activity in cell suspensions support this contention (6). A general model to account for the oscillation of PKA is presented in Fig. 10. When cAMP binds to cAMP surface receptor 1 (cAR1), it activates both the adenyl cyclase A (ACA) and the mitogen-activated protein kinase ERK2 (15, 20). ACA catalyzes cAMP synthesis, and ERK2 inhibits the internal phosphodiesterase RegA (7, 22, 23, 34). As the internal concentration of cAMP rises, PKA is activated, which inhibits ERK2 (4, 5). When no longer inhibited by ERK2, RegA reduces the internal level of cAMP, which in turn leads to a reduction in PKA activity. This circuit (Fig. 10) can account for the increase and decrease in the intracellular cAMP and PKA activities associated with the natural wave.
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FIG. 10. Model of the regulatory circuitry for PKA activation during normal Dictyostelium chemotaxis. When the cAMP receptor cAR1 is occupied in the increasing phase of the wave, the mitogen-activated protein kinase ERK2 and ACA are activated (4, 5, 15, 19). ERK2 inhibits the internal phosphodiesterase RegA (7, 22, 23, 34), which allows cAMP, synthesized by ACA, to accumulate. As the internal concentration of cAMP increases, so does the activity of PKA. When cAR1 occupancy decreases in the back of the wave, both ERK2 and ACA are deactivated, resulting in an increase in RegA activity, a decrease in the internal concentration of cAMP, and a decrease in PKA activity. PKA also inhibits ERK2 (4, 5), noted by a dashed line. Hence, when PKA activity increases, it begins to shut down ERK2 activity, resulting in an increase in RegA activity and a decrease in the intracellular cAMP concentration. In the pkaR mutant, PKA activity is uncoupled from this circuit and will remain constitutively high under all test conditions. R, regulatory subunit; C, catalytic subunit.
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Defects in chemotaxis. pkaR mutant cells did not respond normally to chemotactic waves in a wild-type cell aggregation territory. In particular, the mutant cells showed no directed movement toward the aggregation center and no increase in velocity in the deduced front of natural waves formed by wild-type cells that were the majority in mixed cultures. pkaR mutant cells also exhibited defects in their responses to both the spatial and temporal components of the wave (Fig. 1). The same abnormalities observed in buffer were manifested by pkaR mutant cells in both spatial and temporal gradients of cAMP. In spatial gradients of cAMP, pkaR mutant cells assessed the direction of the gradient and crawled toward the source, but they crawled at half the velocity of wild-type cells, did not suppress pseudopods to the extent that wild-type cells did, and turned more frequently. These defects lowered the efficiency of chemotaxis. Since assessment of a spatial gradient is the assumed mechanism of orientation at the onset of the front of a natural wave (phase A) (Fig. 1) (29, 47, 48), wild-type cells must also suppress PKA activity at the onset of a natural wave in order to achieve optimum orientation. This is consistent with the low level of intracellular cAMP and, hence, the low level of PKA activity expected in wild-type cells at the onset of a natural wave.
In response to the increasing temporal gradient of cAMP in the front of a natural wave (phase B), wild-type cells elongated, suppressed lateral-pseudopod formation, and translocated persistently and with increased velocity in the direction set in phase A (Fig. 1). pkaR mutant cells did not exhibit an increase in velocity, did not suppress lateral-pseudopod formation sufficiently, and did not translocate in a persistent fashion in response to the increasing temporal gradient in phase B of a simulated temporal wave of cAMP. pkaR mutant cells did, however, respond normally to the peak of the wave by suppressing lateral-pseudopod formation and retracting the dominant pseudopod(s). pkaR mutant cells also exhibited a reduction in velocity in response to a rapid increase in cAMP concentration to 1 µM, a treatment which has previously been suggested to reflect the responsiveness of a cell to the peak of a natural wave (29, 42, 47, 48). Wild-type cells also respond to the peak of a wave or to the rapid addition of 1 µM cAMP by rounding up. Since pkaR mutant cells are constitutively ovoid, they exhibited very little morphological change in response to the peak of a wave. In the back of the wave, pkaR mutant cells resumed lateral-pseudopod formation, but in all directions, just as with wild-type cells. These results suggest that although pkaR mutant cells respond abnormally to the increasing phase of a temporal wave, they respond normally to the peak and back of the wave. Since one expects the intracellular concentration of cAMP and hence the activity of PKA to cycle in a manner similar to but slightly later than that of the extracellular cAMP concentration (13), any role played by activated PKA would hence have to occur close to the peak of the natural wave and to some extent in the back of the wave. It therefore may be no coincidence that wild-type cells lose their elongate shape at the peak of a natural cAMP wave, when PKA activity should be close to maximal, and remain apolar in the back of the wave. We therefore suggest the possibility that the activation of PKA at the peak of a wave of cAMP plays a direct role in dismantling the elongate cell shape that facilitates rapid translocation along a substratum.
RegA-PKA pathway. In wild-type cells, the level of intracellular cAMP and hence the level of cAMP-stimulated PKA activity are regulated by cAR1 occupancy according to the regulatory scheme shown in Fig. 10. At the trough of the wave, when the extracellular concentration of cAMP and hence cAR1 occupancy are lowest, increased RegA (ACA) phosphodiesterase activity and ACA inactivation lead to a decrease in PKA activity, and at the peak of the wave, when the extracellular cAMP concentration is maximal, RegA phosphodiesterase inactivation and ACA activation lead to an increase in PKA activity. The deletion of regA, therefore, should result in abnormally elevated PKA activity in the trough of a natural wave, much as pkaR mutant cells should have increased levels of PKA activity in the trough. One might therefore expect regA and pkaR mutant cells to share behavioral defects. Indeed, both regA (47) and pkaR mutant cells were incapable of undergoing normal chemotaxis in monolayers, and both behaved in similar abnormal fashions in natural waves of cAMP generated by wild-type cells that were the majority in mixed cultures. In the deduced front of a natural cAMP wave, both moved in an erratic fashion, exhibiting no directional movement toward the aggregation center, like their wild-type neighbors. In addition, neither mutant was capable of suppressing lateral-pseudopod formation or turning in an increasing temporal gradient of cAMP, a necessary response in natural chemotaxis. Both mutants were still capable, however, of chemotaxing in a spatial gradient of cAMP, albeit less efficiently than wild-type cells, and both responded to the peak and back of a temporal wave of cAMP in an apparently normal fashion. We tentatively conclude that the defects shared by the two mutants stem from the abnormally high levels of PKA activity in both.
However, in contrast to pkaR mutant cells, regA mutant cells were able to extend pseudopods and elongate along a substratum when they were incubated in buffer as well as when they were in the front of a temporal wave of cAMP and showed increased velocity in response to an increasing temporal gradient of cAMP (47). regA mutant cells also differed from pkaR mutant cells in the localization of myosin II when they were analyzed in the front of a temporal wave of cAMP. While regA mutant cells exhibited less cortical staining than wild-type cells (47), pkaR mutant cells exhibited cortical staining similar to that of wild-type cells in the front of a wave. These differences in behavior and in myosin II localization may reflect differences in the levels of PKA activity attained in the two mutants under different conditions. In the pkaR mutant, PKA activity should be maximal under all conditions. In regA mutant cells, PKA activity should be low until ACA is activated by the binding of cAMP to its receptor cAR1 (Fig. 10) and might be reduced to some degree in the trough of the wave by other cytoplasmic phosphodiesterases acting on internal cAMP. PKA activity in regA mutant cells may, therefore, never attain the constitutive levels present in pkaR mutant cells.
The constitutive ovoid cell shape and propensity of pkaR mutant cells to form lateral pseudopods may be indicative of defects in cortical rigor. High PKA activity may lead to defects in the actin-myosin cytoskeleton in the cortex by affecting myosin II phosphorylation. Consistent with such a mechanism, we have recently found that cells carrying mutations that preclude phosphorylation of the myosin II regulatory light chain remain elongate through the peak and back of a temporal wave (48). These cells may be unable to respond to the increases in PKA activity associated with the peak of the wave.
Conclusions. Our results indicate that PKA activity must be inhibited through its regulatory subunit in order for cells to attain an elongate shape and extend their dominant pseudopods along a substratum in a normal fashion both in buffer and in phases A and B in the front of a chemotactic wave. The behavioral abnormalities identified in pkaR mutant cells in buffer and the absence of a velocity response in the front of a wave most likely are due to the basic defect in cell shape and the abnormal position of the dominant pseudopods. Although no major defects were observed in the general organization of F-actin, myosin II, and tubulin, our staining results were obtained with fixed cells and, therefore, do not exclude the possibility that there were defects in the dynamic cytoskeletal reorganization. Since regA mutant cells were elongate in buffer and in the front of a temporal wave while pkaR mutant cells were ovoid under both conditions, we conclude that the shared behavioral defects, namely, the incapacity to respond to natural waves of cAMP and the incapacity to suppress lateral-pseudopod formation in the front of a simulated temporal or natural wave of cAMP, are most likely unrelated to defects in cell shape but are consequences of abnormally high PKA activity in both mutants. Since wild-type cells become ovoid at the peak of simulated temporal and natural waves, we suggest that PKA activation may play a role in dismantling cell polarity during this phase of the wave through the reorganization of the actin-myosin cytoskeleton, possibly through the regulation of myosin II regulatory light-chain phosphorylation.
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