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First published online February 8, 2008; 10.1104/pp.107.113035 Plant Physiology 146:1611-1621 (2008) © 2008 American Society of Plant Biologists OPEN ACCESS ARTICLE
Pollen Tube Growth Oscillations and Intracellular Calcium Levels Are Reversibly Modulated by Actin Polymerization1,[OA]Departamento de Biología Molecular de Plantas Instituto de Biotecnología, Universidad Nacional Autónoma de México, Cuernavaca, Morelos 62271, Mexico (L.C.); Department of Neuroscience, Tufts School of Medicine, Boston, Massachusetts 02111 (A.L.-W.); and Department of Biology and the Plant Biology Graduate Program, University of Massachusetts, Amherst, Massachusetts 01003 (J.G.K., P.K.H.)
Prevention of actin polymerization with low concentrations of latrunculin B (Lat-B; 2 nM) exerts a profound inhibitory effect on pollen tube growth. Using flow-through chambers, we show that growth retardation starts after 10 min treatment with 2 nM Lat-B, and by 15 to 20 min reaches a basal rate of 0.1 to 0.2 µm/s, during which the pollen tube exhibits relatively few oscillations. If treated for 30 min, complete stoppage of growth can occur. Studies on the intracellular Ca2+ concentration indicate that the tip-focused gradient declines in parallel with the inhibition of growth. Tubes exhibiting nonoscillating growth display a similarly reduced and nonoscillating Ca2+ gradient. Studies on the pH gradient indicate that Lat-B eliminates the acidic domain at the extreme apex, and causes the alkaline band to move more closely to the tip. Removing Lat-B and returning the cells to control medium reverses these effects. Phalloidin staining of F-actin reveals that 2 nM Lat-B degrades the cortical fringe; it also disorganizes the microfilaments in the shank causing the longitudinally oriented elements to be disposed in swirls. Cytoplasmic streaming continues under these conditions, however the clear zone is obliterated with all organelles moving into and through the extreme apex of the tube. We suggest that actin polymerization promotes pollen tube growth through extension of the cortical actin fringe, which serves as a track to target cell wall vesicles to preferred exocytotic sites on the plasma membrane.
Actin plays a central role in the control of pollen tube growth (Hepler et al., 2001
Together with these physiological data have been recent structural observations that help us appreciate where and how actin is involved in apical growth. Recent studies from Lovy-Wheeler et al. (2005)
Attempts to monitor the activity of apical actin have met with considerable difficulty; nevertheless two reports have addressed this issue in pollen tubes exhibiting oscillatory growth. Fu et al. (2001)
If actin polymerization and activity are growth-initiating processes, what then regulates actin? Some obvious candidates include actin binding proteins (e.g. profilin, gelsolin/villin, and actin depolymerizing factor [ADF]), perhaps especially in response to certain regulatory ions (e.g. Ca2+ and H+). Briefly we note that all these components are well represented in the apex of growing pollen tubes (Hepler et al., 2001 With these questions in mind we have revisited the role of actin polymerization in the control of pollen tube growth. Herein we examine the effect of low concentrations of Lat-B on pollen tube growth, and also on intracellular Ca2+ and pH. Lat-B (2 nM) has a profound but selective effect on the actin cytoskeleton; it destroys the cortical actin fringe but retains arrays, albeit disorganized, of microfilaments in the shank of the tube. Using a flow through culture chamber, where changes in growth rate and ions can be followed with great care, we find that 2 nM Lat-B markedly slows cell elongation, leading to a situation in which basal growth occurs, but oscillatory growth is eliminated. Under these circumstances the tip-focused Ca2+ gradient declines and the alkaline band moves closer to the apex. These results enhance our understanding of the role of actin polymerization in pollen tube growth.
Actin Polymerization Is Necessary for Oscillatory Pollen Tube Growth When 2 nM Lat-B is administered to pollen tubes exhibiting oscillatory growth, there is no apparent effect for the first 5 min (Fig. 1A ). However, during the next 10 to 15 min the overall growth rate starts to decline; the oscillations become erratic with a marked diminution in excursions from the midpoint to high growth rates. During the next 20 min the growth rate declines further with the pollen tube exhibiting mainly a basal rate of growth with a few brief excursions to the formerly midlevel rate of growth (Fig. 1, A and B). This condition of basal, nonoscillating growth can be sustained for 10 min; if the pollen tube is retained in 2 nM Lat-B, cell extension will eventually stop completely after 30 min (Fig. 1B). Of particular note, these effects are completely reversible when the pollen tube is returned to normal, control conditions. Following removal of Lat-B, the tubes require a few minutes (approximately 5 min) to reinitiate growth (Fig. 1B). At first there are fluctuations between nongrowth and a basal rate, but after 10 min, the tube typically exhibits a basal, nonoscillating rate of growth. After 20 min, oscillations to higher values of growth become evident and within 30 min the tube exhibits normal oscillatory growth, which is equivalent to that seen prior to Lat-B treatment (Fig. 1B). A summary shown in Figure 1C emphasizes the reversibility of the Lat-B effect, where the expressions of normal growth, slow growth, and a return to normal growth are visually juxtaposed.
Lat-B Profoundly Affects the Cortical Actin Fringe
To monitor the effect of Lat-B on the structure of the actin cytoskeleton, we have fixed pollen tubes according to the room temperature protocol developed recently by Lovy-Wheeler et al. (2005)
Lat-B (2 nM) Causes a Decline in the Tip-Focused Ca2+ Gradient Treatment of pollen tubes with 2 nM Lat-B, which degrades the cortical fringe and slows growth, also profoundly affects the tip-focused Ca2+ gradient (Fig. 3 ). In close agreement with the growth data, 5-min treatment causes only a slight lowering of the Ca2+ gradient (Fig. 3B), whereas by 15 min it is much more pronounced (Fig. 3C). Whenever pollen tubes exhibit basal growth, there is always an accompanying gradient even though it may only be 500 nM at the high point. However, if pollen tube growth is completely inhibited, then the Ca2+ gradient declines to basal values of 100 to 200 nM, which are expressed throughout the length of the tube (Fig. 3D). As with the growth data, even when the Ca2+ gradient is totally eliminated, it can recover when the pollen tube is returned to control culture medium (Fig. 3E).
The detailed relationship between Ca2+ and growth oscillations in pollen tubes treated with Lat-B is shown in Figure 4 . Under control conditions Ca2+ and growth oscillate with the same period, but not exactly with the same phase. As previously shown by Messerli et al. (2000)
Lat-B (2 nM) Causes the Alkaline Band to Move Apically Repetitive measurements of the intracellular pH at 5-s intervals in cells loaded with 2'7'-bis-(2carboxyethyl)-5-(and-6)-carboxyfluorescein (BCECF)-dextran indicate that treatment with 2 nM Lat-B causes the acidic domain at the tip to disappear and the alkaline band to move closely to the extreme apex (Fig. 5 ). Unfortunately it has not been possible to conduct a reversal of this effect because the tubes rapidly burst after the removal of Lat-B, while in the presence of BCECF. The bursting of the recovering tubes appears to be peculiar to the presence of BCECF-dextran, because we do not observe this phenomenon in tubes recovering in the presence of fura-2-dextran (see Fig. 3).
Lat-B Increases the Level of G-Actin
Lat-B achieves its effect by binding to G-actin and preventing it from undergoing assembly into microfilaments (Spector et al., 1989
Imaging DNase fluorescence in control cells reveals a relatively high level of G-actin in the apical domain (Fig. 6A
), as shown previously (Cárdenas et al., 2005
A further result that has emerged from this analysis is that the level of G-actin in the apex of control pollen tubes oscillates during growth (Fig. 7). When the data are subjected to cross-correlation analysis, we find that the increase in G-actin follows the increase in growth rate by 91.3° (±2.3° SE, n = 3). A comparable analysis of the troughs reveals that they are nearly as strongly correlated with growth rate as are the peaks. But more importantly they are advanced over growth by an approximately equal interval of 84° (±2.8° SE, n = 3). A low level of G-actin, which we interpret as an increase in F-actin polymerization, thus anticipates the increase in growth rate.
The results presented expand our understanding of the role of actin polymerization in pollen tube growth. Although it has been known that Lat-B retards pollen tube growth, the use of flow-through chambers herein, reveals important details about the inhibitory process. In brief we find that Lat-B at 2 nM routinely requires 15 min or more before irregular growth oscillations are observed. Thereafter we reliably observe a decline in growth to a basal level (20–30 min), and finally after an additional 10 min to a nongrowing state. The results also show that the inhibitory effects of Lat-B on growth are closely coupled to a similar decline in the apical Ca2+ gradient. Thus oscillations in both growth and Ca2+ decline in parallel, and both reach nonoscillating states, which can persist for some minutes. Finally, when growth stops completely, the Ca2+ gradient disappears, and a basal level of the ion is observed throughout the length of the tube. Despite the severity of these effects, they are completely reversible when the tubes are returned to control culture conditions.
The cortical actin fringe, which is rapidly destroyed by Lat-B, emerges as a structure that plays a central role both in establishing cell/cytoplasmic polarity and in controlling rapid, oscillatory growth. In addition to the growth and Ca2+ effects noted above, Lat-B also produces an increase in G-actin, leads to a loss in the apical clear zone, and causes the alkaline band to move closely to the extreme apex of the cell. This last mentioned observation is particularly interesting because it suggests that there is a connection between the apical actin fringe, and the H+-ATPase, which produces the alkaline band. It seems likely that the fringe controls the spatial location of the plasma membrane associated H+-ATPase, and by extension the location of the alkaline band as well as the pattern of extracellular proton currents, which seem pivotal in the regulation of pollen tube growth (Feijó et al., 1999
By what mechanism could the apical actin fringe promote oscillatory pollen tube growth? Pollen tube elongation, as in other plant cells, is assumed to be dependent on a balance between turgor pressure and a yielding of the cell wall (Cosgrove, 1993
It is also possible that actin polymerization contributes directly to the driving force. There is a rich pool of G-actin in the apex of pollen tubes (Fig. 6; Cárdenas et al., 2005
The results showing that inhibition of actin polymerization with Lat-B causes the Ca2+ to decline stand at marked contrast with those of Wang et al. (2004)
The studies with fluorescently tagged DNase indicate that Lat-B, as predicted, causes the G-actin pool to increase. A further observation reveals that this pool oscillates in control cells, with the increase in G-actin following, and the decrease in G-actin preceding the increase in growth rate. These results support the view that F-actin undergoes repetitive cycles of polymerization/depolymerization. Specifically F-actin appears to depolymerize following the peak in growth rate, and repolymerize in anticipation of the increase in growth rate. These conclusions are consistent with those showing that both the formation of F-actin (Fu et al., 2001
Whereas actin depolymerization does not appear to regulate Ca2+, changes in the ion may exert a profound effect on actin organization. It has been known for over 20 years that elevated Ca2+ causes fragmentation of F-actin in lily pollen tubes (Kohno and Shimmen, 1987
Additional players involved in Ca2+ and actin interaction include the phosphoinositides (
Based on these lines of information we suggest the following scenario to explain the interactive roles of Ca2+ and actin in the apex during oscillatory pollen tube growth (Fig. 8
). When growth accelerates, there is an increase in Ca2+ that follows the increase in growth rate. The ion influx might be controlled by the opening of SACs (Fig. 8; Dutta and Robinson, 2004
However, as pollen tube growth slows, there will be a reversal of the processes that retard growth (Fig. 8). Thus as growth declines during the oscillatory cycle, the SACs (Fig. 8) close, preventing Ca2+ entry; in addition the [Ca2+] is reduced through sequestration by the ER, mitochondria, and the vacuole (Sze et al., 2006 In conclusion, we have shown that preventing actin polymerization exerts a profound inhibitory effect on pollen tube growth. Lat-B at 2 nM markedly slows and even completely inhibits elongation. The underlying changes include a degradation of the apical actin fringe, a loss in cytoplasmic zonation, a diminution of the Ca2+ gradient, and a forward motion of the alkaline band. In considering the mechanism by which actin polymerization controls growth we favor the idea that the apical actin fringe targets vesicles to select regions in the apex, where exocytosis occurs. Through the targeted addition of material to the cell wall, loosening occurs that allows turgor-driven expansion. Our observations also suggest a close interaction between intracellular Ca2+ and the cytoskeleton in the pollen tube apex, wherein the ion, operating through different actin binding proteins, regulates the structure and activity of F-actin.
Cell Culture Lilium formosanum plants were first grown from seed in growth chambers for approximately 9 months to develop vigorous bulbs. The plants were then given a cold induction (approximately 5° C) for 6 weeks, which promotes flowering, and transferred to the greenhouse. Fresh pollen grains, harvested from flowering plants, were hydrated, germinated, and grown in pollen growth medium (PGM), which contained 15 mM MES, 1.6 mM H3BO3, 1 mM KCl, 0.1 mM CaCl2, 7% Suc, and pH 5.5. After 30 min of germination and elongation on a rotary device at 25°C, the pollen tubes were allowed to settle for 5 min, and then 35 µL were mixed on a coverslip with an equal volume of 1.4% low melting point agarose (Type VII; Sigma-Aldrich) dissolved in PGM. After mixing, and wicking away the excess fluid, the preparation was chilled briefly (15 s) to gel the agarose. The pollen tubes were then allowed to recover for 15 min before examination with the microscope. To maximize the conditions and achieve optimal pollen tube growth, we set up a continuous perfusion system consisting of a peristaltic pump (Bio-Rad Laboratories), which can perfuse the PGM medium at a flow rate of 250 µL/s. This system also allowed us to administer the PGM with or without drugs, under conditions where there was minimal disturbance of pollen tube growth due to medium replacement. Those pollen tubes showing good growth rates and oscillations, and normal morphology were selected for further studies.
Pollen tubes were pressure injected with different probes as follows: fura-2-dextran (10 kD; 500 µM) for intracellular Ca2+, BECEF-dextran (70 kD; 0.1 mg/mL) for pH, and DNaseI Oregon green (1.61 µM) for G-actin visualization. For microinjection the probes were centrifuged for 2 min at 7,000 rpm to remove nondissolved particles. Injection needles were pulled in a vertical pipette puller (model 700D; David Kopf Instruments) from borosilicate glass capillaries (World Precision Instruments). Using very thin-diameter plastic tubing attached to a micropipette, a small volume of injectate (0.5 µL) was introduced into the injection needle. The remaining volume of the needle was topped with distilled water. Following insertion of the needle into the pollen tube, approximately 100 µm from the tip, the desired probe was pressure injected into the pollen tube.
Pollen tube images were acquired using a CCD camera (Quantix Cool Snap HQ; Roper Scientific) attached to a Nikon TE300 inverted microscope (Nikon Instruments) with a 40x/1.3 numerical aperture oil immersion objective lens. All the equipment was operated with MetaMorph/MetaFluor software (Molecular Devices). Microinjected cells were excited using a xenon illumination source (DG-4; Sutter Instruments) that contains a 175-W ozone-free xenon lamp (330–700 nm) and a galvanometer for fast switching between excitation wavelengths. A filter wheel system (Lambda 10-2; Sutter Instruments), mounted immediately before the CCD camera, was used to control the position of emission filters for fluorescence ratio imaging, and a polarizing filter for Nomarski DIC imaging. The setup allowed fast (<1 s) acquisition of the ratio pair and the corresponding DIC image. The tracking function in MetaMorph was used to process the DIC images and calculate growth rate, amplitude, and frequency of the oscillations. For Ca2+ determinations, fura-2 dextran loaded cells were excited at 340 and 380 nm, with excitation collected at 510 nm. Image pairs were also matched with a corresponding DIC image to show the status of the pollen tube. The two fluorescence images were ratioed to provide a quantitative map of the Ca2+ levels throughout the pollen tube. Ca2+ calibration was performed using buffer kit number two (Molecular Probes) and the kilodaltons calculated from the dissociation constant calculator Web site from Molecular Probes (http://www.probes.com).
For pH imaging, pollen tubes loaded with BCECF-dextran were excited at 440 and 495 nm, with emission at 535 nm. Although the amount of dye injected could not be tightly controlled, we attempted to work at levels below 1 µM, because it has been shown that higher concentrations dissipate local pH gradients (Feijó et al., 1999
For G-actin imaging, DNaseI Oregon green was injected together with tetramethyl-rhodamine-dextran (70 kD), a reference marker. Because DNase can inhibit pollen tube growth by modulating actin polymerization, we therefore kept its final concentration between 0.15 and 0.2 µM, which is approximately 10-fold below that needed to cause half-maximal inhibition of elongation (1.9 µM; Vidali et al., 2001
Pollen tubes were cultured 1 to 2 h, treated with 2 nM Lat-B for 4 min, and then were simultaneously fixed and permeabilized with a buffer composed of 100 mM PIPES (or 100 mM 3-{[2-hydroxy-1,1-bis(hydroxymethyl)ethyl]amino}-1-propanesulfonic acid [TAPS]), 5 mM MgSO4, 0.5 mM CaCl2, 0.05% Triton X-100, 5 mM ethylene glycol bis[sulfosuccinimidylsuccinate], 1.5% formaldehyde, and 0.05% glutaraldehyde at pH 9 for 0.5 to 1 h. The growth medium was completely removed before adding the fixative. The cells were rinsed free of fixative and then incubated in the same buffer as outlined above but at pH 7 and also containing 6.6 µM (10 µL/mL) Alexa 543-phalloidin (Molecular Probes) and 10 mM EGTA. Imaging, which began approximately 1 h after staining, was performed on a Zeiss LSM510 Meta confocal microscope using the HeNe 543-nm laser excitation, and a long-pass 568-nm emission filter.
We thank our colleagues for many helpful discussions throughout the course of this investigation. Received November 9, 2007; accepted February 4, 2008; published February 8, 2008.
1 This work was supported by the National Science Foundation (grant nos. MCB–0077599 and MCB–0516852 to P.K.H.). This work was also supported by grants from Dirección General de Asuntos del Personal Académico de la Universidad Nacional Autónoma de México (grant nos. IN228903 and IN206507 to L.C.). The author responsible for distribution of materials integral to the findings presented in this article in accordance with the policy described in the Instructions for Authors (www.plantphysiol.org) is: Luis Cárdenas (luisc{at}ibt.unam.mx).
[OA] Open Access articles can be viewed online without a subscription. www.plantphysiol.org/cgi/doi/10.1104/pp.107.113035 * Corresponding author; e-mail luisc{at}ibt.unam.mx.
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