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Actin filaments in different parts of a cell interact with specific actin binding proteins (ABPs) and perform different functions in a spatially regulated manner. However, the mechanisms of those spatially-defined interactions have not been fully elucidated. If the structures of actin filaments differ in different parts of a cell, as suggested by previous in vitro structural studies, ABPs may distinguish these structural differences and interact with specific actin filaments in the cell. To test this hypothesis, we followed the translocation of the actin binding domain of filamin (ABDFLN) fused with photoswitchable fluorescent protein (mKikGR) in polarized Dictyostelium cells. When ABDFLN-mKikGR was photoswitched in the middle of a polarized cell, photoswitched ABDFLN-mKikGR rapidly translocated to the rear of the cell, even though actin filaments were abundant in the front. The speed of translocation (>3 μm/s) was much faster than that of the retrograde flow of cortical actin filaments. Rapid translocation of ABDFLN-mKikGR to the rear occurred normally in cells lacking GAPA, the only protein, other than actin, known to bind ABDFLN. We suggest that ABDFLN recognizes a certain feature of actin filaments in the rear of the cell and selectively binds to them, contributing to the posterior localization of filamin.
Actin is a ubiquitous cytoskeletal protein that plays important roles in various cellular activities such as cell migration, cell division and intracellular transport in eukaryotic cells [1–4]. Each of the multiple functions of actin is dependent on interactions with specific actin binding proteins (ABPs). Interaction with the Arp2/3 complex, for example, produces a dendric meshwork of actin filaments in sheet-like pseudopods called lamellipods at the front of migrating cells, and polymerization of actin filaments in this dendric meshwork extends the lamellipods forward. The length of lamellipods is controlled by cofilin, which severs and depolymerizes actin filaments at the back of lamellipods. Additionally, actin filaments form a cortical network underlying the cell membrane, and interact with focal adhesions through linker proteins. Myosin II filaments produce a contractile force at the rear of the cell by pulling the network of actin filaments [5,6]. An advance of the leading lamellipods and contraction of the rear cooperatively drives movement of an amoeboid cell. Thus, actin filaments interact with various ABPs and perform different functions in a spatially regulated manner in a cell. It is generally believed that the spatially-defined interactions between actin filaments and ABPs are controlled by local biochemical regulation of each ABP, but there are a number of cases in which such simple biochemical explanations are unknown or insufficient.
Notably, the cortical actin network continuously moves toward the rear of a polarized cell during cell migration, in part driven by contraction of actin and myosin in the rear [7–10]. Recent measurements in the cellular slime mold Dictyostelium discoideum demonstrated that the speed of this rearward cortical flow, or retrograde flow, is similar to that of the forward movement of polarized cells , such that the cortical actin meshwork is stationary relative to the substrate during movement. Nonetheless, there is a rapid turnover of cortical actin filaments within seconds, and it is not that the same group of actin filaments remain stationary to the substrate .
Dictyostelium filamin, an orthologue of human filamin, is a dimeric ABP with actin cross-linking activity. The meshwork of actin filaments cross-linked by filamin is important for cell migration, chemotaxis and mechanosensing [11–14]. Each filamin polypeptide has an actin binding domain (ABD) consisting of two calponin homology (CH) domains at the N-terminus, a rod domain, and a dimerization domain at the C-terminus [15,16]. ABDFLN interacts with actin filaments with high affinity allowing ABDFLN to be fused with green fluorescent protein (GFP) to visualize actin filaments in vivo [6,17,18]. In polarized cells, filamin is localized in the posterior region [14,19,20]. Moreover, filamin tends to localize at stretched actin filaments in vivo . It is possible that this property contributes to the control of force transmission and rigidity sensing by filamin [11,12,21]. However, it is not known how filamin distinguishes and interacts with specific actin filaments in a cell.
Each actin protomer in a filament assumes one of the multiple structures depending on its nucleotide state, applied mechanical stress and/or interactions with ABP [22–32]. Binding of cofilin induces a cooperative structural change of actin protomers in filaments that involves supertwisting of the helix. This cooperative structural change enhances the affinity of affected actin protomers for cofilin, resulting in cooperative binding of cofilin [26,28,30]. Conversely, stretching actin filaments inhibits their interaction with cofilin but enhances their interaction with myosin II [5,28,33,34]. Additionally, there is some evidence that certain ABPs, including cortexilin [35,36], fimbrin [24,37], and drebrin [29,38], selectively interact with actin filaments of a specific structure. Along this line, we recently showed that binding of the motor domain of myosin II in the presence of ATP induces a conformational change in actin filaments to reduce the affinity for cofilin, while the supertwisted actin filaments induced by cofilin binding has a lower affinity for the myosin motor domain . Thus, the structure of actin protomers in filaments is potentially an important factor for selective binding of ABPs.
Here, we hypothesized that ABDFLN accumulates in the rear of polarized cells by recognizing a certain structural feature of specific actin filaments in the rear of cells. To test this hypothesis, we followed the translocation of ABDFLN using a photoswitchable fluorescent protein, monomeric kikume green-red (mKikGR), in polarized Dictyostelium cells . Use of ABD, pioneered by Washington and Knecht , eliminates the possible contribution of dimeric filamin molecules by recognizing the orthogonal arrangement of actin filaments [2,15,16,21], and may reduce the contribution of biochemical regulation in actin binding because Dictyostelium ABDFLN is not known to be influenced by phosphorylation or by other biochemical regulations. Photo-switching of mKikGR from green to red fluorescence by local irradiation with purple light allows observation of translocation of ABDFLN from the irradiated area to other places. We found that the majority of red ABDFLN-mKikGR molecules generated in the middle of an elongated cell translocated to the cell rear at a much faster speed than the retrograde flow of cortical actin filaments, even though actin filaments were equally or more abundant in the front of cells. The result suggests that ABDFLN recognizes a certain feature of actin filaments in the cell rear, and selectively binds to those filaments.
pTX/ABD-fluorescent protein: Coding sequences of ABDs of filamin and α-actinin of Dictyostelium discoideum were subcloned into a modified pTX-GFP vector , from which sequences coding 8×His, GFP and myc had been removed. Then, the coding sequence of GFP (from pTX-GFP) or mKikGR (from CoralHue® phmKikGR1-MCLinker, Molecular and Biological Laboratories) preceded by a linker (GSGGGGS) was inserted downstream of the ABD sequence of pTX/ABD.
pBIG GFP-GAPA: The coding sequence of Dictyostelium gapA was inserted downstream of GFP in pBIG GFP .
Wild-type D. discoideum AX2 cells and GAPA null cells  were cultured in HL5 medium supplemented with penicillin and streptomycin , and transfected by electro-poration with the pTX/ABD-fluorescent protein, pDdBsr/mCherry-Lifeact and/or pBIG GFP-GAPA as described previously . Transfectants were selected by 20 μg/mL G418 and/or 6 μg/mL blasticidin S in HL-5 medium at 22°C.
Cells expressing ABD-fluorescent proteins and/or mCherry-Lifeact were settled on glass-bottomed dishes (Matsunami, 35 mm dish, hole size: 27 mm, uncoated). To obtain polarized cells, the cells were then starved in 10 mM K+-Na+-phosphate buffer (pH 6.4) until chemotaxis started (~11–12 h at 22°C or ~14–16 h at 11°C). To obtain images of flattened cells, the polarized cells were overlaid with a thin agarose sheet, as described previously . The flattened and polarized cells were observed with a confocal microscope (Zeiss, LSM700) equipped with a 100× objective lens (Zeiss, Plan-Neofluar 100×/1.30 Oil Iris). LED lasers (488 nm: 10 mW, 555 nm: 10 mW) were used for scanning the cells, and images were acquired with ZEN imaging software (Zeiss). The duration for a single frame acquisition was 4~5 s, depending on the size of scanned area. The pinhole size was 1 AU (airy unit) (1 AU = 74.20 μm for the 488 nm laser, 79.74 μm for the 555 nm laser). To prevent photo-bleaching and affecting cell motility, the excitation laser power was set at minimum value (0.5%).
Cells expressing both ABD-GFP and mCherry-Lifeact were irradiated with the 488 nm and 555 nm laser light simultaneously, and those expressing ABD-mKikGR were sequentially irradiated with the 488 nm and 555 nm laser light. The resultant green fluorescence from GFP or mKikGR and red fluorescence from mCherry or mKikGR were separated by a variable secondary dichroic beam splitter (Carl Zeiss) and emission filters, and also a differential interference contrast (DIC) image was simultaneously acquired with each frame. For photoswitching of mKikGR, square areas were scanned four times repeatedly by 405 nm LED laser light (5 mW, 100% laser power). Fluorescence intensities along the cell cortex were analyzed with ZEN and ZEN lite imaging software (Zeiss), as follows. For each cell image, a 1 μm wide band was drawn manually along the cell periphery in the DIC image, such that the cell periphery ran along the center of the band. This band is shown as a thick white line in each cell image. Then the intensities of red and green fluorescence were measured along the length of the band. Each cell type in this report was analyzed in 4–5 independent experiments, and more than 3 cells were observed in each experiment. Rapidly migrating and well-separated polarized cells were selected for observation.
There was weak but non-negligible fluorescence in the red channel from ABDFLN-mKikGR-expressing cells not irradiated with 405 nm laser light. It was thus necessary to subtract this red fluorescence from the image of irradiated cells, in order to extract red fluorescence intensity that was derived from photoswitching by irradiation. For this purpose, a correction coefficient was obtained for each cell from a plotted graph of the green and red fluorescence intensities at the same points along the cell cortex before irradiation with 405 nm light (Supplementary Fig. S1). This coefficient and the fluorescence intensity in the green channel at each pixel were used to estimate fluorescence intensity in the red channel that derived from ABD-mKikGR that was not photoswitched by irradiation. This value was subtracted from the fluorescence intensity in the red channel at that pixel.
Polarized cells prepared as above were permeabilized and fixed by changing the K+-Na+-phosphate buffer (pH 6.4) to PF buffer (10 mM Pipes-KOH pH 6.8, 3 mM MgCl2, 1 mM EGTA, 1 mM DTT, 0.05% Triton X-100, 0.1% glutaraldehyde, 1% formaldehyde) and incubated for 5 min at 22°C, followed by incubation in 10 mM Tris-HCl pH 7.0, 3 mM MgCl2, 1 mM EGTA, and 1 mM DTT for 5 min. Then, they were stained for 1 h in PBS containing 3 nM rhodamine-phalloidin (Invitrogen), rinsed in PBS containing 10 mM DTT, and observed with an LSM 700 microscope.
Localization of ABDFLN fused with GFP at the C terminus (ABDFLN-GFP) via a Gly-based linker (GSGGGGS) was observed in polarized Dictyostelium cells with a confocal fluorescence microscope (Fig. 1A and Supplementary Fig. S2). Actin filaments were visualized by expression of lifeact  fused with mCherry at the N terminus (mCherry-lifeact). To compare the localization of ABDFLN with that of actin filaments more quantitatively, the fluorescence intensities of the images of Figure 1A were measured along the cell cortex (Fig. 1B). Although ABDFLN-GFP colocalized with actin filaments, it localized more intensely in the rear of the cell (Fig. 1B: at ~0 μm) than in the front (Fig. 1B: at ~−20 and ~20 μm). This is indicated by the magenta color of the cell front in the merged image (Fig. 1A), as well as by the ratio of GFP fluorescence intensity to that of mCherry (Fig. 1E: purple line, and Supplementary Fig. S3A), and is consistent with the previous study by Washington and Knecht .
Next, the localization of α-actinin ABD (ABDACTN) was observed (Fig. 1, C and D and Supplementary Fig. S2) to compare with the localization of ABDFLN-GFP, because ABDACTN consists of two CH domains and is homologous to ABDFLN. A previous report showed that accumulation of GFP-ABDACTN in actin-rich structures is weaker than that of GFP-ABDFLN, and discernable localization in actin-rich structures was observed only when the ABDACTN is in oligomers such as dimers and tetramers . In this study, monomeric ABDACTN-GFP showed almost the same distribution as actin filaments along the cortex (Fig. 1, C and D and orange line in E), although the localization signal along the cortex was not very strong relative to that of cytosol (Supplementary Fig. S3, D and H). GFP alone was only diffusely distributed in the cytoplasm (Fig. 1F). These results suggest that ABDFLN shows strong preference for rear actin filaments, but this is not a general property of ABDs consisting of two CH domains.
To investigate the mechanism by which ABDFLN localizes at the rear of a cell, we next followed the translocation of ABDFLN real time by observing ABDFLN-mKikGR in polarized cells with a confocal microscope (Fig. 2, A and B and Supplementary Fig. S4). A pair of green and red fluorescence images was obtained by scanning with 488 nm laser light followed by 555 nm laser light. The green fluorescent ABD FLN-mKikGR, which is the native state of this fluorescent protein in the absence of photoswitching by irradiation with 405 nm light, showed stronger accumulation in the rear of a cell than ABDFLN-GFP (Fig. 2A; at −4.9 s). Additionally, weak red fluorescence was also detected in the rear even without photoswitching (Fig. 2B; at −4.9 s). This is presumably due to very strong accumulation of ABDFLN-mKikGR in the cell rear. Red fluorescence might derive from native mKikGR that is weakly excited by 555 nm light and bled through the red emission filter. Alternatively, a small, background fraction of mKikGR was in the red fluorescent state due to ambient light or by spontaneous conversion.
To locally photoswitch ABDFLN-mKikGR in a polarized cell, the area bound by the yellow square in Figure 2A and B was scanned by 405 nm laser light for ~0.4 s. The red fluorescent ABDFLN-mKikGR generated near the center of the polarized cell spread in the area slightly posterior to the irradiated area and more intensely at the rear of the cell (Fig. 2, A and B). Fluorescence intensity along the cell cortex was measured to reveal the movement of ABDFLN during this process (Fig. 2, C and D). In addition, the intensity profile of the observed red fluorescence of ABDFLN-mKikGR was corrected by subtracting the red fluorescence that was unrelated to irradiation with 405 nm light (see Materials and Methods). Since neighboring cells in the same microscopic field not irradiated with the 405 nm laser light did not show an increase in red fluorescence, the 488 or 555 nm laser light did not contribute to the generation of red fluorescent ABD FLN-mKikGR (Supplementary Fig. S5). Therefore, this procedure extracted the red fluorescence of ABDFLN-mKikGR generated by 405 nm laser light irradiation in the boxed area (Fig. 2D).
Accumulation of red fluorescent ABDFLN-mKikGR in the rear of the cell was evident in the first image, which was scanned between 0.9 and 5.5 s after the irradiation. More specifically, the red fluorescence image of the rear end of this cell was scanned at 3.9 s after the start of the irradiation. The irradiated site was ~12 μm away from the rear end of the cell, implying that the red fluorescent ABDFLN-mKikGR moved at a velocity faster than 3.1 μm/s. This velocity is ~9 times faster than the retrograde flow of cortical actin filaments in polarized Dictyostelium cells reported previously (0.34±0.15 μm/s) . Ruchira et al. (2004) demonstrated that a diffusion coefficient (D) of GFP in a polarized Dictyostelium cell was 32±6 μm2/s . Diffusion time (Tdif), calculated by an equation (Tdif ≈ x2/2D) was 2.3 s for 12 μm of diffusion distance x. This value is slightly shorter the interval between the irradiation and the acquisition of the first image (3.9 s), suggesting that the red fluorescent ABDFLN-mKikGR mainly moved by diffusion, and specifically interacted with and was trapped by actin filaments in the rear of the cell.
In addition, there were two minor peaks of red fluorescence along both sides of the cell near the irradiation site (white arrowhead at −13.5 μm and black arrowhead at 10.5 μm from the rear end at 0.9 s after irradiation). The cell cortex around −13.5 μm was close to the irradiated area, but was not directly irradiated. Presumably cortical actin filaments in this area trapped a small fraction of red ABDFLN-mKikGR generated close by. These minor peaks in polarized cells moved back to the rear relative to the cells at 0.30±0.19 μm/s (mean±S.D., n=7). These velocities are at the same level as the migration velocity of the cells (0.18±0.11 μm/s: measured at the rear end of four cells), and equivalent to the retrograde flow estimated in a previous study (0.34±0.15 μm/s) . This coincidence suggests that the red fluorescent ABDFLN-mKikGR that was bound to the lateral cortical actin filaments was transported to the rear by the retrograde flow of cortical actin filaments. Apparently, total amounts of red fluorescence of ABDFLN-mKikGR increased gradually over the time course of 15 s after the irradiation (Fig 2, Supplementary Figs. S4 and S5). This is presumably because fractions of newly generated red ABDFLN-mKikGR was initially in the cytoplasm or bound to the dorsal or ventral cortex outside the thin confocal plane, and these fractions gradually became detectable as it bound to the side cortices or transported to the rear end, which was in the confocal plane.
We next followed the translocation of ABDACTN using the same method as above. Green fluorescent ABDACTN-mKikGR showed stronger localization along the cortex and in the lamellipodia, and weaker distribution in the cytoplasm, than ABDACTN-GFP (Fig. 3A and Supplementary Fig. S6). Red fluorescent ABDACTN-mKikGR was undetectably low before irradiation with 405 nm light (Fig. 3B). This is presumably because the local concentration of ABDACTN-mKikGR never reached the levels of ABDFLN-mKikGR at the rear of a cell, and consequently, the red fluorescence of ABDACTN-mKikGR rarely exceeded the background. After irradiation with 405 nm light near the center of the cell, red fluorescent ABDACTN-mKikGR spread along the length of the cell, with slight enrichment along the cortex (Fig. 3, B and C). The red fluorescence was somewhat stronger in the central region at 1.2 s after irradiation, but was nearly uniform along the cell length at 10.4 s. The localization of green and red fluorescence of ABDACTN-mKikGRs were eventually similar at ~33.4 s after irradiation (Fig. 3D). This localization is in sharp contrast to that of ABDFLN-mKikGR, which was rapidly and specifically translocated to the rear of the cell.
In polarized cells expressing ABDFLN-GFP, actin filaments were abundant in the lamellipodia, localized along the entire cortex, and enriched in the front and rear (Fig. 1E). However, because ABDFLN-mKikGR showed much stronger posterior accumulation (Fig. 2A) than ABDFLN-GFP (Fig. 1A: top), it was possible that the expression of ABDFLN-mKikGR drove the accumulation of actin filaments at the rear, and ABDFLN-mKikGR simply co-localized with these actin filaments. To rule out this possibility, localization of actin filaments was observed in cells expressing ABDs-mKikGR using two methods. First, mCherry-lifeact was co-expressed with ABDFLN-mKikGR, and was observed simultaneously with the green fluorescence of ABDFLN-mKikGR. As shown in Figure 4A, ABDFLN-mKikGR was exclusively localized in the rear of the cell, while actin filaments were localized not only in the rear, but also in lamellipodia at the front. Second, polarized cells expressing ABDFLN-mKikGR were fixed with glutaraldehyde and formaldehyde, and their actin filaments were stained with rhodamine-phalloidin (Fig. 4B). The staining patterns were largely consistent with live-cell imaging of ABDFLN-mKikGR and mCherry-lifeact, except that cytoplasmic staining with rhodamine-phalloidin was very weak.
Localization of actin filaments in cells expressing ABDACTN-mKikGR was also observed using the same two methods (Fig. 4, C and D). The localization of actin filaments was similar to that in cells expressing ABDFLN-mKikGR or in cells expressing ABDFLN-GFP or ABDACTN-GFP. These results suggest that the expression of ABD-mKikGR does not noticeably influence the localization of actin filaments, and it was clear that ABDFLN preferentially localizes at the rear of polarized cells even though actin filaments are abundant, not only in the rear of cells, but also in lamellipodia at the front of cells.
Although ABDFLN is a relatively small domain (240 amino acids) with a high affinity for actin filaments, some other protein that is localized at the rear of polarized cells may also bind to ABDFLN and mediate its posterior localization. GAPA, an IQGAP-related protein of D. discoideum, is the only other protein that has been shown or suggested to bind to ABDFLN . We thus observed the localization of GFP-GAPA in polarized wild type cells, and that of ABDFLN in polarized GAPA-null cells (Fig. 5 and Supplementary Fig. S7). GFP-GAPA localized at the lamellipodia and weakly along the cortex in polarized cells, and posterior enrichment of GFP-GAPA was rarely observed (Fig. 5, A and B). Moreover, ABDFLN-mKikGR localized at the rear of polarized GAPA-null cells. When ABDFLN-mKikGR in the middle of a polarized GAPA-null cell was photoswitched by irradiation with the 405 nm laser, red fluorescent ABDFLN-mKikGR was rapidly and specifically localized at the rear of the cell (Fig. 5, C–F), as occurred in wild type cells (Fig. 2). These results demonstrate that GAPA hardly influences the localization of ABDFLN in polarized cells.
In this study, we revealed two separate mechanisms with distinct velocities for the translocation of ABDFLN from the cytosol to the rear of a polarized cell. Even though actin filaments were abundant in the front of a cell, the majority of red fluorescent ABDFLN-mKikGR newly generated in the middle of an elongated cell moved very rapidly to the rear, but not to the front. The speed of this translocation was ~9 times faster than the retrograde flow of cortical actin filaments. In contrast, the speed of the translocation was similar to that of diffusion of GFP, and therefore, we concluded that this translocation depends on diffusion, rather than on active transport. ABDACTN, which is homologous to ABDFLN, showed the same distribution as actin filaments, strongly supporting the argument against the possibility that some other ABD that competes with ABDFLN for actin binding inhibits ABD FLN from localizing at the front of the cell. It is also evident that the physical size of ABDFLN-GFP or ABDFLN-mKikGR should not hinder its penetration into the actin meshwork at the front of the cell. Taken together, it is suggested that ABDFLN diffusing in the cytoplasm recognized some feature( s) of actin filaments in the rear of the cell and interacted specifically with these filaments (diffusion and specific capture mechanism, Fig. 6A). It is beyond the scope of this study to elucidate the molecular mechanism of the specific binding between ABDFLN and the posterior actin filaments. However, we and others have proposed that certain ABDs can distinguish actin filaments with different conformations. This hypothesis is based on recent discoveries that actin filaments are inherently polymorphic [32,50], and that external stimuli, including interactions with certain ABPs and mechanical tension, further expands the repertoire of conformational variations [22,23,26,27,30,51–54]. Naturally, actin filaments with different conformations would have different affinities for each ABD. Indeed, stretched actin filaments have a lower affinity for cofilin in vivo and in vitro, and a higher affinity for the motor domain of myosin II in vivo [5,28,34]. Furthermore, certain ABPs also localize in regions where the structure of actin filaments is changed in vivo. For example, when a cell is aspirated locally by a microcapillary, myosin II and filamin accumulate at the aspirated site where actin filaments are tensed and bent [5,13,33,34,55]. In a polarized cell, myosin II and filamin mainly colocalize with posterior actin filaments. Those posterior actin filaments should be stretched by a pulling force exerted by myosin II filaments, unlike those in the front that should be compressed and bent by a pushing force for migration. We thus propose that ABDFLN can recognize the stretched conformation of actin filaments, and specifically binds to them. Irrespective of these proposals, our findings strongly suggest that filamin can distinguish some feature of actin filaments in the rear of a cell, and this contributes to the specific localization of filamin in cells.
In the second mechanism, which is relatively minor based on the red fluorescence intensity of ABDFLN-mKikGR, ABD FLN that strongly interacts with actin filaments in the lateral cortex is carried to the rear of the cell by a retrograde flow of the cortical actin filaments (Fig. 6B). Ratios of fluorescence intensities between the cytosol and cortex (Supplementary Fig. S3) suggest that association of ABDFLN with cortical actin filaments is stronger than that of ABDACTN, and this may be one reason why ABDACTN does not accumulate in the rear, as weakly interacting ABDACTN cannot be stably carried to the rear by this cortical flow. It should be noted, however, that ABDFLN is not stably carried to the rear by binding to one actin filament, because the turnover of cortical actin filaments is very rapid during retrograde flow. For instance, based on a FRAP experiment using GFP-ABDFLN as the fluorescent probe, Yumura et al. (2013) reported that the recovery half-time was only 0.62±0.12 s . This is much shorter than the time required to carry ABDFLN-mKikGR from the middle to the rear of a polarized cell at a rate of 0.34±0.15 μm/s. Furthermore, in the presence of jasplakinolide, a membrane-permeable actin-stabilizer, the half-time of fluorescence recovery was 1.82±0.39 s, which represents the off-rate of GFP-ABDFLN from cortical actin filaments. This is three times slower than the recovery rate in the absence of jasplakinolide, implying that cortical actin filaments turn over before bound GFP-ABDFLN dissociates . Lemieux et al. (2014) have shown that artificially dimeric ABDFLN localizes to the rear of a cell, although monomeric ABDFLN does not appreciably localize there . GFP tends to form a dimer weakly and it is believed that certain linker sequences between GFP and the fusion partner enhance dimerization [20,56,57]. mKikGR is reportedly a monomeric fluorescent protein while the parent KikGR forms tetramers . Therefore, if mKikGR retains a weak tendency to form oligomers, ABDFLN-mKikGR in this study (Fig. 2) might be assembled to oligomers by the influence of the fused proteins and/or the linker peptide. Since the oligomerized ABDFLN can remain tethered to the cortical actin meshwork more stably than the monomeric ABDFLN even when actin filaments turnover rapidly, oligomeric ABDFLN may be transported to the rear of a cell by the retrograde flow of cortical actin filaments more efficiently than monomeric ABDFLN. The ABDFLN-GFP in this study (Fig. 1) might not be significantly assembled to an oligomer and is thus primarily translocated to the rear of the cells by diffusion and a specific capture mechanism. This is because our linker peptide is not hydrophobic and the posterior localization of ABDFLN-GFP was weaker than that of ABDFLN-mKikGR. This cortical actin flow mechanism is presumably physiologically relevant, however, since the parent molecules, filamin and α-actinin, are naturally dimers.
It is possible that these two mechanisms contribute to the localization of various other ABPs in vivo. In particular, if actin filaments at different sites in a cell have unique structural features caused by biochemical modulation, nucleotide state, ABP binding, tension, twisting or bending, the diffusion and specific capture mechanism can be applied to ABP localization at various sites in a cell. Since differential localization of multiple ABPs to specific actin filaments in cells leads to functional differentiation of actin filaments, it is important to elucidate the mechanisms by which ABPs recognize structural features of actin filaments.
It is not well understood how different actin filaments interact with different actin binding proteins (ABPs) in a spatially regulated manner. Here, we demonstrate that the actin binding domain of filamin (ABDFLN) in the middle of elongated, polarized Dictyostelium cells rapidly and specifically binds to posterior actin filaments. The speed of translocation was much faster than the retrograde flow of actin cortex, suggesting that ABDFLN diffusing in the cytoplasm was captured by posterior actin filaments. We suggest that this specific interaction depends on structural polymorphism of actin filaments, and a similar mechanism may contribute to intracellular localization of other ABPs.
This work was supported in part by a Grant-in-Aid from the Ministry of Education, Culture, Sports, Science and Technology No. 24117008 to TU.
Conflicts of Interest
All the authors declare that they have no conflict of interest.
K. S. and T. U. conceived and planned the experiments. K. S., A. N. and T. U. performed the experiments. K. S. analyzed the data. K. S., A. N., H. A. and T. U. contributed reagents and materials. K. S., H. A. and T. U. wrote the manuscript. All the authors reviewed the result and agreed the final manuscript.