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Department of Chemistry and Biochemistry, and the Molecular Biology Institute, University of California, Los Angeles, California
Correspondence: Address reprint requests to Dmitry S. Kudryashov, Tel.: 310-825-4585; Fax: 310-206-7286; E-mail: dkudryas{at}ucla.edu.
| ABSTRACT |
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| INTRODUCTION |
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Alternative ways of imaging actin filaments in cells involve the expression of GFP-actin fusion protein (Westphal et al., 1997
; Choidas et al., 1998
), or the use of actin with fluorescent markers (Hamaguchi and Mabuchi, 1988
; Kreis et al., 1982
; Bernstein and Bamburg, 1992
; Nwe and Shimada, 2000
; Yumura and Fukui, 1998
). The former approach was used mostly in the in vivo experiments whereas the latter approach was used in both the in vitro and in vivo studies. The small size of the fluorescent probes attached to actin (typically <1 kDa) suggests that they would impair less than GFP (Aizawa et al., 1997
; Hosein et al., 2003
) the filament structure and/or the binding of other proteins to actin. Among fluorescent dyes, derivatives of rhodamine have been particularly attractive for actin visualization due to their high quantum yield and relative resistance to photobleaching. In most cases, the rhodamine-based probes (tetramethylrhodamine maleimide or tetramethylrhodamine iodoacetomide) were attached to Cys374, the most reactive cysteine on actin. Such a rhodamine-labeled actin was helpful in imaging the in vivo actin dynamics (Sund and Axelrod, 2000
; Yumura and Fukui, 1998
; Fukui et al., 1999
), the in vitro real-time observation of Arp2/3 induced actin filaments nucleation, branching, and growth (Amann and Pollard, 2001
; Fujiwara et al., 2002a
), and the actin filaments growth and treadmilling (Fujiwara et al., 2002b
). Recently, rhodamine actin was used also to reexamine the yield-strength values of single actin filaments (Cintio et al., 2001
; Adami et al., 2002
), since previous measurements with rhodamine phalloidin-stabilized actin (Tsuda et al., 1996
) would have overestimated this value.
Despite the growing use of tetramethylrhodamine maleimide/acetamide modified actins, their polymerization properties have not been described yet. This is particularly important because tetramethylrhodamine maleimide (TMR-maleimide)-labeled actin does not polymerize by itself, without the addition of unlabeled actin (Otterbein et al., 2001
; Amann and Pollard, 2001
; present study). This property of TMR-maleimide modified actin allowed Otterbein et al. (2001)
to solve the first crystal structure of G-actin, free of any actin-binding protein. Also treatment of F-actin with TMR-iodoacetamide, although typically resulting in <50% labeling efficiency (Sund and Axelrod, 2000
; Cintio et al., 2001
), was shown to disrupt actin filaments (Cintio et al., 2001
; Adami et al., 2002
), suggesting similar properties for TMR-maleimide- and TMR-iodoacetamide-modified actins. Consequently, it may be expected that copolymerization of TMR-actin with unlabeled actin would produce some perturbation in the actin filament structure. The aim of this study was to evaluate the effect of TMR-actin on the structure and dynamics of copolymers formed from unlabeled and TMR-labeled actin.
In this work, we show that actin filaments containing a high fraction of TMR-actin are significantly shorter, less rigid, and have more bends than the control filaments. The higher fragility of the TMR-actin/unlabeled actin copolymers and the consequent filament severing produce a notably accelerated actin polymerization, most likely due to a higher concentration of free ends available for elongation. This acceleration of polymerization by TMR-actin is abolished by tropomyosin and phalloidin, apparently due to filaments stabilization against severing. Our results suggest that TMR-actin induces significant structural perturbation of the copolymers, even when used at low mole ratios to unlabeled actin.
| MATERIALS AND METHODS |
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Proteins
Myosin and actin from rabbit back muscle were prepared according to Godfrey and Harrington (1970)
and Spudich and Watt (1971)
, respectively. For light scattering measurements, actin was additionally gel-filtered through a Sephacryl S-200 high resolution matrix (Amersham Pharmacia Biotech) to eliminate traces of oligomers and actin-binding proteins (MacLean-Fletcher and Pollard, 1980
). S1 was prepared by digesting myosin filaments with
-chymotrypsin according to the procedure of Weeds and Pope (1977)
. Protein concentrations were estimated from their absorption by assuming an A (1%) at 280 nm of 7.5 cm1 for S1, and A (1%) at 290 nm in the presence of 0.5 M NaOH of 11.5 cm1 for actin. Whenever appropriate, light scattering corrections were applied. Molecular masses were assumed to be 115 and 42.3 kDa for S1 and actin monomers, respectively.
Cys-374 modification of actin with TMR-maleimide was performed according to the protocol of Otterbein et al. (2001)
, with minor modifications (Kudryashov and Reisler, 2003
). Cys-374 modification of actin with TMR-iodoacetamide was performed similarly, but because of low efficiency of this reaction pure TMR-iodocetamide actin could not be prepared. Briefly, G-actin (57 mg/ml) was incubated for 1 h in the presence of 10 mM DTT. Actin was then passed two times through PD-10 (Sephadex G-25) columns to remove DTT, and was incubated overnight with a two molar excess of TMR-iodoacetamide. The labeling was stopped with 2.0 mM DTT and the labeled actin was separated from reagent excess over a PD-10 column pre-equilibrated with G-buffer. The extent of labeling was determined by measuring actin concentration with the Bio-Rad Protein Assay (Bio-Rad laboratories; Hercules, CA), and the concentration of the incorporated TMR using its extinction coefficient at
= 543 nm (87,000 M1 cm1). ANP-crosslinked oligomers were prepared according to Hegyi et al. (1998)
.
Mg2+-G-actin was prepared by adding 0.4 mM EGTA and 0.1 mM MgCl2 to 510 µM Ca2+-G-actin and then incubating the mixture for 10 min on ice. BeFx-TMR-actin was prepared by incubating ADP-TMR-actin in the presence of 5.0 mM NaF, 0.1 mM BeCl2, and 2.0 mM MgCl2 for 4 h on ice. To prepare Mg2+-TMR-actin/unlabeled actin copolymers for light scattering and calorimetric experiments, both proteins were mixed at the desired mole ratios in the Ca2+-state, then 0.4 mM EGTA and 0.1 mM MgCl2 were added and the samples were incubated for 10 min before the addition of 100 mM KCl and/or 2.0 mM MgCl2.
Light scattering and fluorescence measurements
Light scattering measurements were performed in a PTI spectrofluorometer (Photon Technology Industries, South Brunswick, NJ) with the emission and excitation wavelengths set at 350 nm. Changes in the fluorescence of TMR-actin upon polymerization were detected at
= 580 nm after excitation at
= 544 nm.
Electrophoresis
SDS-polyacrylamide gel electrophoresis (SDS-PAGE) was performed on 10% gel slabs according to Laemmli (1970)
. Gels with TMR-actin were visualized under UV light in Alpha-Imager (Alpha Innotech, San Leandro, CA) to reveal the TMR-label, and then stained with Coomassie Blue R-250 to reveal the total protein. The stained gels were scanned using a Scan Premio ST scanner and quantified using the Sigma-Gel software (Jandel Scientific, San Rafael, CA).
Sedimentation experiments
For copolymerization experiments, TMR-actin/unlabeled actin mixtures (20 µM total actin concentration) were incubated for 1.5 h at 23°C in a buffer containing 0.2 mM CaCl2, 0.2 mM ATP, 1.0 mM DTT, and 5.0 mM HEPES (pH 7.5) (G-buffer), and supplemented with 2.0 mM MgCl2. For polymerization with filament stabilizing factors, 5.0 µM TMR-actin was incubated in the G-buffer in the presence of 2.0 mM MgCl2 and one of the following: 10 µM phalloidin, 10 µM dolastatin 11, and 5.0 µM myosin S1. After an incubation for 1.5 h at 23°C, these samples were spun down in the tabletop Beckman airfuge for 30 min at 30 psi. The supernatants and pellets were carefully separated and then denatured for SDS-PAGE analysis. The above experiments were also performed with Mg-G-actin as a starting material, and with 100 mM KCl used in addition to 2.0 mM MgCl2 for the polymerization. None of these factors change by more than 10% the results of the experiments.
Electron microscopy
For EM observation, stabilized Mg-TMR-actin (by S1, phalloidin, etc.) was diluted to 2.5 µM, whereas TMR-actin copolymers, polymerized with 2 mM MgCl2 and in the presence or absence of 100 mM KCl, were diluted to 5.0 µM, and then applied to carbon-coated grids for 60 s, washed by one drop of F-actin buffer and negatively stained with 1% (w/v) uranyl acetate. A Hitachi H-600 electron microscope was used at an accelerating voltage of 75 kV with a 50-µm objective aperture and a 200-µm condenser aperture at a nominal magnification of 30,000.
Differential scanning calorimetry
Differential scanning calorimetry (DSC) experiments were performed on a 6100 N-DSC II differential scanning calorimeter (Calorimetry Sciences, Provo, UT) with a cell volume of
0.25 ml. All experiments were performed at a scanning rate of 1°K/min under 3.0 atm of pressure. The total concentration of actin was 60 µM. The reversibility of thermal transitions was checked by a second heating of the sample immediately after cooling, after the first scan. All thermal transitions were irreversible under the conditions used in this study. Because the thermal denaturation of actin was irreversible, only simple thermodynamic parameters and terms were used for the interpretation of the results. The thermal stability of actin was described by the temperature of the maximum of thermal transition (Tm). This parameter can be obtained directly from experimental calorimetric traces after subtraction of the chemical baseline and concentration normalization and, thereby, it can be used for the description of the irreversible thermal denaturation of TMR-actin copolymers.
Analytical ultracentrifugation
1:1, 1:2, and 1:3 mixtures of unlabeled G-actin and TMR-G-actin in the Ca-bound state in G-actin buffer were converted to Mg-G-actin by supplementing the solutions with Mg/EGTA and then polymerizing actin by 2.0 mM MgCl2 for 2 h, at 23°C. Sedimentation velocity experiments were carried out at 20°C in a Beckman Optima XL-A analytical ultracentrifuge equipped with a photoelectric scanning system. Sedimentation boundaries of TMR-actin were recorded at
= 560 nm. Boundaries recorded at the beginning of the run, at 3000 rpm, provided the information on total TMR-actin concentration in the solution. Plateau regions of boundaries recorded at the top run speeds (45,000 rpm) contained information on the concentration of TMR-actin that was not incorporated into filaments. At intermediate speeds (30,000 rpm) and run times, the boundaries described all the TMR-actin species present in solution (monomers and polymers). The sedimentation coefficients distribution was determined from a g(s) plot using the Beckman Origin-based software (Version 3.01).
| RESULTS |
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To check whether TMR-labeled actin is capable of elongation, light scattering experiments were carried out in the presence of 1.0 mM MgCl2. At 1.0 mM MgCl2 the elongation rate is only 2.5 times slower, whereas the nucleation is suppressed
20-fold compared to that at 2.0 mM MgCl2 (Tobacman and Korn, 1983
), allowing for better distinction between the elongation and nucleation steps. As expected, neither control nor modified actin (5.0 µM) show any detectable polymerization by 1.0 mM MgCl2 during our observation time (Fig. 1) because of unfavorable nucleation conditions. The addition of 0.2 µM cross-linked actin oligomersas filament nucleicauses a prompt increase in the light scattering of control, unlabeled actin, but not for the TMR-modified actin (Fig. 1, AB). This result shows that unlike control actin, TMR-actin alone cannot support a stable elongation process by adding to the preformed filament nuclei.
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60s to
35s for the main fraction in the 1:1 and 3:1 mole ratios of TMR-actin/unlabeled actin copolymers, respectively; Fig. 2, BC).
According to these results, the fraction of TMR-actin in the copolymers did not exceed
50% of the sedimented actin (F-actin), even at high molar excess of TMR-actin over unlabeled actin (9:1). Therefore, it would appear that on average filaments can accommodate TMR-actin at most at an alternating basis with unlabeled actin.
Emission spectra of TMR-actinbefore and after its copolymerization with unlabeled actinshow
50% fluorescence increase upon actin polymerization. This fluorescence increase is linear with the increase in the fraction of TMR-actin incorporated in the copolymers and may be used along with light scattering for monitoring the polymerization reaction (data not shown).
Myosin S1, phalloidin, and BeFx promote the polymerization of TMR-actin
To clarify whether TMR-actin can be induced to polymerize in the absence of unlabeled actin, we investigated the polymerization of TMR-actin in the presence of myosin subfragment 1 (S1), phalloidin, dolastatin 11, and BeFx, all of which are known to stabilize the filament structure. As expected, no detectable amount of TMR-actin was found in the pellet, after actin incubation in the presence of 2.0 mM MgCl2 and high speed centrifugation (Fig. 3, Mg2+). Dolastatin 11, which has recently been shown to bind between the two long-pitch strands of actin filaments and thereby stabilize them (Oda et al., 2003
; Bai et al., 2001
), results in the pelleting of only a small percentage of total TMR-actin (Fig. 3).
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Electron microscopy of TMR-actin/unlabeled actin copolymers
Electron microscopy examination of TMR-actin/actin copolymers was carried out on samples with a known fraction of TMR-actin in the filaments (as determined by the sedimentation and SDS PAGE analysis). Filaments containing
30% TMR-labeled protein (Fig. 4, B, E, and F) are much shorter than the control filaments (Fig. 4 A). Observation of several fields revealed that most of the filaments of unlabeled actin were several micrometers long, whereas most of the TMR-actin copolymers were shorter than 0.5 µm, and <10% exceeded the length of 1.0 µm. Moreover, the structure of the copolymers is perturbed strongly, revealing a tendency of these filaments to form multiple sharp bends (Fig. 4 E). Addition of 100 mM KCl to the experimental mixture did not affect an appearance and length distribution of the copolymers (data not shown). These results reveal a significant difference in the stability and flexibility of the control F-actin and the TMR-actin copolymers. In contrast to that, the structure and length distribution of phalloidin-stabilized (Fig. 4 D), and S1-decorated (Fig. 4 C) TMR-actin filaments did not differ much from the corresponding control filaments.
Light scattering measurements of TMR-actin and unlabeled actin copolymerization
Addition of TMR-actin accelerates the overall rate of polymerization of unlabeled actin by MgCl2 (Fig. 5 A). This acceleration is detectable at a mole ratio of 1:11 of TMR-actin to unlabeled actin (0.5 µM and 5.5 µM, respectively), whereas at the 1:5 mol ratio the polymerization is completed
threefold faster than in unlabeled actin alone (Fig. 5 A). Supplementing the polymerization buffer with 100 mM KCl did not affect the polymerization acceleration by TMR-actin (Fig. 5, A and C), indicating that physiological ionic strength conditions do not significantly stabilize the copolymers. Notably, the acceleration of polymerization induced by TMR-actin was abolished (and even reversed) when either phalloidin or tropomyosin were added to stabilize actin filaments (Fig. 5 B). Thus, it appears that the faster polymerization of the copolymers stems from their instability and consequent severingas documented by electron microscopy (Fig. 4, B, E, and F)resulting in a higher concentration of free filament ends available for elongation. It has been shown before that cofilin increases the rate of actin polymerization in solution via a similar mechanism (Du and Frieden, 1998
; Blanchoin and Pollard, 1999
). Although phalloidin also accelerates the polymerization of actin, it does so not by severing filaments (which would be reflected in a characteristic sigmoidal shape of polymerization curves, as seen on Fig. 5, A and C), but rather by stabilizing filament nuclei and inhibiting monomer dissociation from filament ends.
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Thermostability of the TMR-actin/unlabeled actin copolymers
Differential scanning calorimetry (DSC) did not reveal any significant difference between the thermal transition temperatures of TMR-modified and unlabeled Ca2+-G-actins (64.6 ± 0.9 and 64.0 ± 0.7°C, respectively). The thermal transition of Mg-TMR-actin was at a lower temperature (56.6 ± 0.7°C) than that of Ca-TMR actin. The melting of unlabeled Mg-G-actin could not be measured reliably because of its tendency to oligomerize at concentrations much lower (12.5 µM; Attri et al., 1991
) than those used in the DSC (60 µM).
Filaments of unlabeled actin have a similar melting temperature irrespective of the divalent cation (Ca2+ or Mg2+) bound at the high affinity site of actin monomers (70.2 ± 0.3 and 70.3 ± 0.7°C, respectively), although Mg2+-actin shows somewhat lower enthalpy and cooperativity of heat capacity profiles. Both Ca2+ and Mg2+ copolymers of unlabeled actin and TMR-actin are destabilized, albeit unequally, with the increasing content of TMR-actin (Fig. 6 A). The destabilization of Mg2+-copolymers is significantly stronger than that of Ca2+-copolymers (Fig. 6, AB). This difference cannot be attributed to a different content of TMR-actin in the filaments (28.3 ± 2.2 and 30.7 ± 1.6% of TMR-actin in the Ca2+ and Mg2+ copolymers, respectively). Moreover, electron microscopy observation of these filaments did not reveal any significant morphological differences between them. Although heat consumption profiles for copolymer melting could not be fitted to a single Gaussian peak, they were very similar to the profiles recorded for homopolymers of unlabeled actin (Fig. 6 C), indicating their homogenous behavior in terms of thermal stability. The addition of KCl increased slightly the thermal stability of the copolymers and the cooperativity of the transition irrespective of the high affinity divalent cation bound to actin (Fig. 6 B).
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| DISCUSSION |
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TMR-actin mimics the severing effect of cofilin on F-actin
As shown in Fig. 1, TMR-actin neither nucleates new filaments nor elongates the preformed nuclei into filaments unless it is stabilized by phalloidin, myosin S1, or the presence of unlabeled actin. In the latter case, unlabeled actin and TMR-actin copolymerize with a maximum incorporation of
50% of labeled actin out of the total actin in the copolymer. This indicates that on average the unlabeled actin molecules may alternate with TMR-actin protomers, thereby decreasing the structural strain due to perturbations in the interprotomer contacts (that preclude filament existence with TMR-actin alone). The resulting TMR-copolymers are intrinsically unstable and show increased fragmentation, probably due to the accumulated structural strain (Figs. 4 and 5). In this sense, TMR-actin mimics the action of severing proteins. For cofilin, the main member of this class of proteins, filaments fragmentation has indeed been linked to the changes in lateral and longitudinal interprotomer contacts in F-actin (McGough et al., 1997
; McGough and Chiu, 1999
; Galkin et al., 2002
, 2003
; Bobkov et al., 2002
, 2004
). Also, similarly to cofilin, TMR-actin accelerates the polymerization of actin in solution (Fig. 5) by increasing the number of filament ends available for elongation.
TMR-actin accelerates the polymerization of unlabeled actin in solution
Our electron microscopy images reveal that TMR-actin shortens and impairs the structure of copolymers compared to control filaments. In principle, short copolymers (Fig. 4) could be produced if TMR-actin had increased the nucleation of actin filaments (Tait and Frieden, 1982
). However, two sets of data show that this is not the case: 1), analytical ultracentrifugation did not detect any oligomeric species in solutions of TMR-actin alone (in the presence of 2 mM MgCl2) nor in copolymer solutions; and 2), addition of TMR-actin to unlabeled actin does not accelerate, but instead delays the beginning of polymerization, indicating the inhibition of filament nucleation. After that initial period, TMR-actin speeds up the polymerization, as reflected in the sigmoidal polymerization curves (Fig. 5 A). Notably, the acceleration of polymerization at low ratios of TMR-actin/unlabeled actin is most evident when using gel-filtered actin. In the unfiltered actin, traces of oligomers and actin-binding proteins accelerate the nucleation (resulting in shorter filaments) and mask the effect of TMR-actin.
The kinetics of a similar, cofilin-dependent acceleration of actin polymerization (Du and Frieden, 1998
; Blanchoin and Pollard, 1999
) was fitted well to a scheme assuming filament fragmentation by cofilin (Du and Frieden, 1998
). The addition of tropomyosin and/or phalloidin, both of which are well known to stabilize F-actin, abolished the TMR-actin-induced acceleration of polymerization. This is consistent with filament severing being the mechanism by which TMR-actin speeds up actin polymerization. Therefore, our data strongly suggest that TMR-actin severs the copolymers, producing additional filament ends, which participate in filament elongation. These data agree well with the recent studies of Adami et al. (2002
, 2003
), who show that the yield strength of tropomyosin-stabilized filaments of unlabeled actin is
fivefold higher than that of tropomyosin-stabilized TMR-actin copolymers, which, in turn, is
threefold higher than the yield strength of TMR-actin/unlabeled actin copolymers in the absence of tropomyosin (50.5 pN, 10 pN, and 3.5 pN, respectively).
Recently, taking advantage of total internal reflection fluorescence microscopy, TMR-actin was used at a 1:9 mol ratio to unlabeled actin to image the in vitro actin filaments growth and treadmilling (Fujiwara et al., 2002b
). The analysis of length fluctuation of individual filaments led to the unexpected conclusions that the elongation and dissociation constants (k+ and k) are
40 times higher at steady state than during the elongation step (Fujiwara et al., 2002b
). To explain this difference, the assumption was made that hexamersand not monomersare the average effective size units of elongation/dissociation at the steady state treadmilling (Fujiwara et al., 2002b
). Our results point to the possibility that the suggested putative hexamers dissociation is an artifact of TMR-actin presence in the copolymers and not an intrinsic property of actin itself. Although Fujiwara et al. (2002b)
did not observe filament fragmentation at TMR-actin/unlabeled actin ratio similar to that used in this study (1:11; Fig. 5 A), the copolymers in the former case might have been stabilized through contacts with the glass surface of the coverslip. It is also possible that fragmentation could have escaped detection in that study if it occurred mainly at the pointed ends of filaments, where the contacts between subdomains 1 and 2 of two longitudinally adjacent actin protomers are strongly weakened or even disrupted (Galkin et al., 2003
). The extent of such a conformational perturbation was estimated to span
10 monomers from the pointed end (Galkin et al., 2003
), which correlates with the hexamer treadmilling unit suggested by Fujiwara et al. (2002b)
.
Factors stabilizing TMR-actin filaments
In addition to the copolymerization with unlabeled actin, TMR-actin can be stabilized in the F-actin form by myosin S1 and phalloidin, but not by dolastatin 11 (Fig. 3). Recently, dolastatin 11 was shown to strongly stabilize F-actin, similarly to phalloidin, by intercalating between the two long pitch strands of filaments (Oda et al., 2003
; Bai et al., 2001
). However, in contrast to phalloidin, which was mapped to the interface among three adjacent protomers (n1, n, and n+1; Steinmetz et al., 1998
), dolastatin 11 makes contacts with only two laterally adjacent protomers (n and n+1). The difference in dolastatin 11 and phalloidin contacts with actin appears critical to the TMR-actin polymerization. This can be explained by assuming that phalloidin stabilizes both lateral and longitudinal (inter- and intrastrand) contacts, whereas dolastatin 11 is able to stabilize mainly lateral contactswhich is not enough to allow TMR-actin assembly into filaments. Moreover, because it does not bind to actin monomers, phalloidin must stabilize otherwise unstable and transient oligomers of the TMR-actin to assist in their polymerization.
The efficient polymerization of TMR-actin in the presence of myosin S1 may reflect the restoration of normal longitudinal inter-actin contacts by S1 (Fig. 3). It has been shown that S1-induced assembly of G-actin into filaments begins with longitudinal bridging of two actin molecules by one S1 molecule, followed by their further condensation into higher oligomers and polymers (Valentin-Ranc et al., 1991
; Valentin-Ranc and Carlier, 1992
; Fievez et al., 1997
; Blanchoin et al., 1995
). Similar rates of S1-induced polymerization of unlabeled and TMR-actin (data not shown) suggest that the same mechanism of filaments assembly is involved in both cases. However, the TMR-actin filaments depend on S1 for their stability and existence, and disassemble almost immediately upon addition of ATP (and the consequent dissociation of S1), whereas the destabilization of unlabeled actin filaments is much slower. This suggests that S1 may be stabilizing weakly connected protomers in TMR-F-actin by bridging over incompatible interfaces.
Alternatively, and more generally, the polymerization of TMR-actin by phalloidin and/or S1 may be facilitated by allosteric changes in the position of the TMR-label, decreasing its inhibitory effect on actin polymerization and forcing TMR-actin into normal F-actin conformation. The destabilization and severing of actin filaments by TMR-actin, as well as the antagonistic effects of filament stabilizing factors to such action are reminiscent of the effects of cofilin on actin filaments. It will be interesting to test the possibility that the disruption of filaments by ADF/cofilin proteins and TMR-actin have a similar structural basis, perhaps related to an intrinsic mode of F-actin instability (Galkin et al., 2003
).
| ACKNOWLEDGEMENTS |
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This work was supported by grants from the United States Public Health Service (AR 22031) and the National Science Foundation (MCB 0316269).
| FOOTNOTES |
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Submitted on March 11, 2004; accepted for publication May 4, 2004.
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