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* Department of Mechanical Engineering and Materials Science, Duke University, Durham, North Carolina 27708-0300 USA; and
Department of Mechanical Engineering, United Arab Emirates University, Al Ain, United Arab Emirates
Correspondence: Address reprint requests to Doncho V. Zhelev, Dept. of Mechanical Engineering and Materials Science, Duke University, Durham, NC 27708-0300. Tel.: 919-660-5335; Fax: 919-660-8963; E-mail: dvzh{at}duke.edu.
| ABSTRACT |
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| INTRODUCTION |
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(SDF-1
) secreted by stromal cells (Juarez and Bendall, 2004
Neutrophil chemotaxis is closely regulated by a group of receptors loosely divided into two main groups called nonclassical and classical chemotactic receptors (Katanaev, 2001
). The nonclassical receptors induce chemotaxis but do not induce degranulation and superoxide production. These include the tumor necrosis factor receptors (CD120a and CD120b), the platelet derived growth factor receptor, and the receptor for transforming growth factor ß (Katanaev, 2001
). The classical chemotactic receptors are G-protein coupled receptors (GPCRs) and are capable of inducing all immune functions of the neutrophil including chemotaxis, degranulation, and superoxide production. These receptors are divided into five groups named after their most common ligands, namely, the receptors for the N-formylated peptides, the receptor for the platelet activated factor (PAF), the chemokine receptors (CXCR1, CXCR2, and CXCR4), the complement anaphylotoxin receptors, and the leukotriene receptors (BLT1 and BLT2) (Tarlowe et al., 2003
; Katanaev, 2001
). It has been shown recently that the classical chemotactic receptors (called here also GPCRs) activate distinct pathways of intracellular signaling, which induce differential superoxide production and/or integrin activation (Nick et al., 1997
; Berger et al., 2002
). It has been shown also that GPCRs are intimately involved in the regulation of F-actin polymerization in the lamella region during chemotaxis, which is critical for cell crawling (Pollard et al., 2000
; Katanaev, 2001
). Different chemotactic receptors have different capacity to induce directional crawling (hierarchical chemotactic response), which is seen by the ability of these receptors to induce a stepwise crawling of neutrophils in complex chemoattractant gradients (Foxman et al., 1999
; Heit et al., 2002
). However, it is not known whether this differential intracellular signaling also induces F-actin polymerization in the lamella region with different rates.
The evidence for the differential intracellular signaling by GPCRs is derived mostly from studies of secretion or secretion-related responses (Berger et al., 2002
; Haribabu et al., 2000
), whereas the signaling of secretion and chemotaxis are known to follow distinct pathways of activation (Haribabu et al., 1999
). Most importantly, chemotactic responses such as pseudopod extension were not desensitized after multiple exposures to chemoattractant (Alteraifi and Zhelev, 1997
) in contrast to secretion responses (Haribabu et al., 2000
). These differences suggest that, at least for pseudopod extension, the signaling of F-actin polymerization by different GPCRs may be limited to a degree of utilization of the recently identified phosphoinositide-3 kinase (PI3K)-dependent and -independent pathways of pseudopod growth (Chodniewicz and Zhelev, 2003a
).
Here we model the distribution of chemoattractant in the micropipet assay for pseudopod extension (Zhelev et al., 1996
) to define similar conditions for stimulating pseudopod growth with different chemoattractants. Then we use representative chemoattractants for the five classical chemotactic receptors and study the dependence of the rate of pseudopod extension on chemoattractant concentration. The used chemoattractants include N-formyl-methionyl-leucyl-phenylalanine (fMLP) for the N-formyl peptide receptors, PAF for PAFR, leukotriene B4 (LTB4) for BLT1 and BLT2, C5a for complement anaphylotoxin receptors, and interleukin-8 (IL-8) for CXCR1 and CXCR2. To evaluate the utilization of the PI3K-dependent and -independent pathways of F-actin polymerization by different GPCRs we measured the decrease of the rate of pseudopod extension in the presence of wortmannin (WTM), which is a specific inhibitor of the activity of the PI3Ks of class I (Davies et al., 2000
; Thelen et al., 1994
; Wymann et al., 1996
; Stoyanova et al., 1997
). We also study the effect of blocking RhoA and ROCK activity on oscillatory pseudopod formation, which is observed during the stimulation of pseudopod growth in suspended cells.
| MATERIALS AND METHODS |
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Cell preparation
Human neutrophils were freshly isolated from whole blood obtained by venipuncture from consenting, healthy adult volunteers (mean age 29 ± 8.5 years) into vacutainers anticoagulated with K2EDTA. The neutrophils were isolated by a one-step density gradient centrifugation on Polymorphoprep (Nycomed, Oslo, Norway), at 500 x g for 35 min at 23°C. The neutrophil fraction was washed once with Ca2+/Mg2+-containing Hanks' Balanced Salt Solution (HBSS), (Sigma Chemical, St. Louis, MO) and resuspended in an autologous plasma/HBSS solution (1:3, v/v). The cells were added to the manipulation chamber filled with an autologous plasma/HBSS solution (1:3, v/v). Microscopic evaluation of isolated cells indicated that 95% of the cells were neutrophils. The trypan blue dye exclusion test showed that >98% of the cells were viable. Approval for these studies was obtained from the Institutional Review Board at Duke University.
Micromanipulation
The experimental temperature controlled chamber was 2 mm thick. The bottom half of the chamber was covered with a cover glass strip and was open at both sides to allow for micromanipulation. The micropipets used to manipulate the cells were made from capillary glass tubing (A-M systems, Everett, WA) pulled with a vertical pipet puller (David Kopf Instruments, model 730, Tujunga, CA). The tip of the pipets was cut using a microforge. The micropipets were mounted on the microscope stage and inserted coaxially into the experimental chamber. They were connected to a manometer system, which allowed control of the pipet-chamber pressure difference. The temperature of the experimental chamber was controlled by flow of thermostated water and was measured with a thermocouple.
In the experiments of pseudopod extension, a single, passive neutrophil with smooth membrane surface and uniform optical density was chosen. The cell was held in a supporting pipet with a 5-µm internal diameter. Another pipet with an internal diameter of 1 µm was filled with a chemotactic solution of fMLP, PAF, LTB4, C5a, IL-8 (Sigma), or their equimolar mixture and positioned 1 µm from the cell surface. The used chemoattractants and inhibitors were initially diluted in either HBSS, or ethanol (with a maximal final concentration of 0.8%), or dimethyl sulfoxide (with a maximal final concentration of 0.2%). The following inhibitors were used: wortmannin (at 1-µM concentration and incubation for 15 min at 23°C; Sigma), Clostridium botulinium C3 exoenzyme (C3; 20-µg/ml concentration and incubation for 3 h at 23°C), and Y-27632 (10-µM concentration and incubation for 30 min at 23°C; Biomol, Plymouth Meeting, PA). The incubation of the cells with either ethanol or dimethyl sulfoxide at the above concentrations had no measurable effect on the rates of pseudopod extension (data not shown).
Chemoattractant containing solution was blown over the cell, which initiated the extension of a single pseudopod. Pseudopod extension was observed using an inverted Nikon (Tokyo, Japan) microscope equipped with a 60x oil immersion objective. The microscope images were recorded using a charge-coupled device (CCD) camera (Cohu, San Diego, CA). A real-time counter and the chamber temperature were multiplexed onto the recorded images using a multiplexer (Vista Electronics, La Mesa, CA). The recorded images were analyzed with Metamorph Imaging software (Universal Imaging, Downingtown, PA), and the rate of pseudopod extension was calculated from the measured pseudopod lengths and time lapses. Approximately 90% of the neutrophils tested produced pseudopods. The nonresponding fraction of the cells was not reported in the averages of the rates of pseudopod extension.
Modeling the chemoattractant distribution
Pseudopod formation was stimulated using the assay shown in Fig. 3. Our previous use of this assay showed that the rate of pseudopod extension was dependent on the concentration of chemoattractant in the delivery pipet (Zhelev et al., 1996
); however, the chemoattractant concentration at the leading edge of the extending pseudopod and the distribution of chemoattractant in the vicinity of the cell were not known. We used FIDAP to model the distribution of chemoattractant in the vicinity of the activated cell and to evaluate the concentration of chemoattractant at the leading pseudopod edge. In the micropipet assay, the chemoattractant was delivered using a small pipet as shown in Fig. 3, and the distribution of chemoattractant was dependent on both convection and diffusion. Two basic cell shapes were considered: a), a spherical shape representing the neutrophil before the start of pseudopod growth and b), a spherical shape with a single projection representing the neutrophil with a single pseudopod. The cell membrane was considered impermeable for chemoattractant.
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![]() | (1) |
![]() | (2) |
and P were the dimensionless velocity
and pressure respectively. Re was the Reynolds number defined as
where
was the fluid density, U was the characteristic velocity, Rp was the characteristic length, and µ was the fluid viscosity.
The chemoattractant released from the delivery pipet was also subject to diffusion, which was characterized by the diffusion equation,
![]() | (3) |
was the Peclet number, and DAB was the diffusion coefficient. The dimensionless boundary conditions at the pipet orifice, cell surface, symmetry line, and the far stream were as follows (Fig. 1).
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At the cell surface:
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At the symmetry line:
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At the far stream:
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The parameters used in the model were determined as follows. The velocity of the fluid flow in the pipet was measured by tracking 0.2-µm latex beads or small liposomes made of the debris of red cell membranes (Zhelev and Needham, 1993
). The calculated maximal fluid velocity at the center of the pipet for all experiments was on the order of 5 µm/s. The experimental solution for most experiments was made of 75% HBSS and 25% plasma. The viscosity of this solution was 1.17 cp, and its density was similar to the density of water (1 g/cm3). The diffusion coefficient was inversely related to the molecular size by the Stokes-Einstein equation. The molecular mass of the used chemoattractant ranged from 0.3 to 0.4 kDa for LTB4 and fMLP and from 8 to 11 kDa for IL-8 and C5a, respectively. The diffusion coefficient of N-formyl-norleucyl-leucyl-phenylalanine (FNLLP), which was similar to fMLP, was on the order of 105 cm2/s (Stickle et al., 1984
), and the diffusion coefficient of IL-8, which was the largest of the used chemoattractants, was on the order of 2.5 x 106 cm2/s (Moghe et al., 1995
). The chemoattractant distribution was calculated for diffusion coefficients from 105 to 106 cm2/s (only the data for the diffusion coefficient equal to 106 cm2/s are shown).
The FI-GEN module of FIDAP was used for mesh generation. The interior elements were four nodded quadrilaterals, whereas the boundary elements were two nodded linear elements. We used 1100 and 10,000 element mashes to test the dependence of the numerical solution on mesh density. The difference of the solutions for the two mesh densities did not exceed 2%. The shown numerical solutions were for meshes with 1100 elements. The validity of the solutions was tested by introducing a residual vector error (0.001) and by testing for convergence. The transient solution reached convergence in less than 10 iterations. We also tested the validity of the solution by changing the domain size. The solutions for the domains extending from 50 to 100 µm from the cell surface were almost identical.
The modeling of the convective transport showed that even for low Reynolds numbers such as Reynolds numbers on the order of 5 x 105, the streamlines of the liquid leaving the delivery pipet were strongly dependent on the cell shape (not shown). This suggested that at the regime of dominant convective mass transport (Peclet numbers larger than 1) the chemoattractant distribution around the cell would change with the change of the cell shape. To avoid experimental conditions, where chemoattractant distribution was dependent on cell shape, we worked in a regime of diffusion-limited mass transport by choosing low rates of chemoattractant delivery. The maximal rate of flow of chemoattractant from the delivery pipet in our experiments was on the order of 5 µm/s. The size of the neutrophil along the pseudopod axis in the presence of a maximally extended pseudopod was on the order of 15 µm, and the smallest diffusion coefficient for the chemoattractants used was 2 x 106 cm2/s. For these values of the experimental parameters, the Peclet number was 0.4, which provided for diffusion-limited delivery of chemoattractant. The distribution of chemoattractant around the cell in these experimental conditions reached steady state within several seconds (data not shown). This was much smaller than the delay time for pseudopod extension measured experimentally (Fig. 3). The chemoattractant concentration at the leading edge of the pseudopod was strongly dependent on the distance between the cell and the delivery pipet, although it was independent of cell shape (Fig. 2). This provided conditions for steady-state stimulation of pseudopod extension at a constant concentration of chemoattractant at the leading edge of the extending pseudopod as long as the distance between the cell and the delivery pipet remained constant. The calculated chemoattractant concentration at the leading edge of the pseudopod decreased almost exponentially with the increase of the distance between the cell and the delivery pipet (not shown). For a distance between the cell and the delivery pipet equal to 1 µm, this decrease was 30%, which was the distance between the cell and the delivery pipet in our experiments. The diffusion-limited delivery of chemoattractant to the cell's surroundings was characterized by the generation of a steep chemoattractant gradient, where the chemoattractant concentration at the rare(back) of the cell was more than one order of magnitude smaller than the chemoattractant concentration at the leading edge (Fig. 2 C).
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| EXPERIMENTAL RESULTS |
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10 s after activation (Niggli and Keller, 1997
After the beginning of pseudopod growth, the pseudopod length increased at almost constant rate for a period of 3040 s (Fig. 3 B). This allowed the pseudopod to reach its maximal length. After reaching a maximal length, the pseudopod retracted and then increased its length and retracted it in an oscillatory fashion as long as the chemoattractant was delivered to the tip of the pseudopod. Fig. 1 C shows the change of pseudopod length verses time for a pseudopod stimulated with 107 M fMLP delivered with a pipet 1 µm from the cell surface for a time interval of 700 s. It is seen from the figure that for 700 s the pseudopod extended and retracted its length 12 times, although in two occasions the retraction of the pseudopod was almost complete. This oscillatory pseudopod formation was most probably actively regulated. To determine the pathway regulating the oscillatory pseudopod extension, we blocked the activity of the signaling molecules from the PI3K-dependent and -independent pathways of pseudopod extension that we have identified earlier (Chodniewicz and Zhelev, 2003a
). Interestingly, the blocking of either RhoA activity with C3 or the activation of its downstream effector kinase ROCK with Y-27632 abolished pseudopod retraction, which resulted in an initial pseudopod extension and maintaining of the extended pseudopod at its maximal length for the duration of chemoattractant delivery. The blocking of RhoA activity did not arrest F-actin polymerization after reaching the maximal pseudopod length, which was detected from the continuous reshaping of the pseudopod leading edge after the maximal pseudopod length was reached.
The steep chemoattractant gradient created by the micropipet assay provided an opportunity for testing the predictions of the current models for cytoskeleton F-actin polymerization in the lamella region. The paradigm for F-actin polymerization in the lamella region postulates the assembly of a group of molecules, including WASp or WAVE, Arp2/3, the small GTPases Rac and Cdc42, and phosphatidylinositol (4,5)-bisphosphate (PtdIns(3,4)P2) and phosphatidylinositol (3,4,5)-triphosphate (PtdIns(3,4,5)P3), into molecular complexes that govern F-actin polymerization in the interior of the plasma membrane (Pollard and Borisy, 2003
; Ridley et al., 2003
). This mechanism of F-actin polymerization restricts the newly polymerized F-actin to the vicinity of the plasma membrane. The creation of a steep chemoattractant gradient by the micropipet assay, which allowed the activation of GPCRs only in a small area on the plasma membrane was expected to induce F-actin polymerization in a localized region of the activated cell. Therefore, the increase of the pseudopod length was expected to be the dominant shape change. Indeed, the contour analysis of the change of the cell shape during pseudopod extension showed that the increase of the pseudopod length was much larger than any other shape change (Fig. 3 D). The shape of the pseudopod region was independent of the used chemoattractant (Fig. 3 E), which confirmed the hypothesis that the micropipet assay induced cytoskeleton F-actin polymerization only in a localized region of the cell and allowed us to use the rate of pseudopod extension as a measure for the rate of the process controlling F-actin polymerization in the pseudopod region. The rate of pseudopod extension was determined from the measured pseudopod length verses time as shown in Fig. 3 B.
Dependence of the rate of pseudopod extension on chemoattractant concentration
The rates of pseudopod extension induced by the ligands of the five classical chemotactic receptors considered here were similar for the range of concentrations from 1010 to 106 M (Fig. 4). All measured rates reached saturation at 107 M chemoattractant. It is not known how different chemoattractants contribute to the signaling of F-actin polymerization in the lamella region; however, the observed similar rates of pseudopod extension for the different chemoattractants provided the opportunity to test whether the action of the different GPCRs is synergistic and whether there was a common rate-liming process for pseudopod extension.
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Effect of wortmannin on the rate of pseudopod extension
Wortmannin blocks PI3K activity and allows the determining of the degree of utilization of the PI3K-dependent signaling during pseudopod extension. The incubation of the cells with 1 µM wortmannin, which was the saturating concentration of this inhibitor for pseudopod extension (Chodniewicz and Zhelev, 2003a
), decreased the rate of pseudopod extension induced with IL-8 by 55% and the rate of pseudopod extension induced by all other used chemoattractants from 72% to 80% (Fig. 5). This showed that except for the chemokine receptors, the F-actin polymerization signaled by the classical chemotactic receptors was strongly dependent on PI3K activation, which suggested that the rate-limiting process of the PI3K-dependent signaling of F-actin polymerization may be the rate-limiting process of pseudopod extension.
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| DISCUSSION |
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The existence of a rate-limiting process for pseudopod extension suggests that pseudopod extension is limited by the enzymatic reactions involved in the pathways of F-actin polymerization. The strong dependence of F-actin polymerization induced with fMLP, LTB4, PAF, and C5a on PI3K activity suggests that this pathway could provide the rate-limiting process for pseudopod extension. Our earlier finding that the PI3K pathway is represented by a cascade of enzymes including protein kinase C (PKC) and Akt/protein kinase B (PKB) (Chodniewicz and Zhelev, 2003a
) suggests that pseudopod extension may be limited by the slowest enzymatic reaction in the pathway. We have studied this possibility in more detail and have found that, indeed, the rate of pseudopod extension was limited by the enzymatic activity of its signaling reactions (Chodniewicz et al., 2004
).
The discovery of the oscillatory pseudopod extension is intriguing. Crawling neutrophils change their direction of movement by either following the change of the direction of the chemoattractant gradient or by repolarizing in the new gradient (Zigmond et al., 1981
). Most of the cells (60%) follow the change of the stimulus direction; however, a significant fraction of the cells (30%) repolarize in the direction of the newly established gradient (Zigmond et al., 1981
). The studying of the mechanism of establishing cell polarity using HL-60 cells differentiated into neutrophil-like cells showed that RhoA and ROCK play pivotal roles in signaling of polarity (Xu et al., 2003
). In view of this finding, and our finding that the oscillatory pseudopod formation was abolished after blocking RhoA or ROCK activity, we propose that the role of the oscillatory pseudopod formation is to provide means for the crawling cell to change its direction of crawling via repolarization in a newly established gradient.
| ACKNOWLEDGEMENTS |
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| FOOTNOTES |
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Submitted on October 31, 2003; accepted for publication March 29, 2004.
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