Structure of actin filament bundles from microvilli of sea urchin eggs

The detailed substructure of actin filament bundles in microvilli of fertilized sea urchin eggs has been studied by analysing electron microscope images of negatively stained specimens. Transverse stripes which repeat about every 130 Å along the axis of a bundle, as previously observed by Burgess & Schroeder (1977), reflect the positions of cross-bridges that connect the filaments into a bundle. Analysis of optical transforms of the micrographs reveals that there are approximately 14 actin monomers between cross-overs of the two long-pitch helical strands of the actin filaments, with three cross-bridges in this interval. The structure is basically similar to that of the hexagonally packed bundles prepared in vitro from high speed supernatants of sea urchin eggs by Kane (1975) and analyzed by DeRosier et al. (1977). One clear difference, however, is that the in vivo microvillar filament bundles are supercoiled, giving rise to long axial repeats of 1500 to 2000 Å.Computationally filtered images of regions that were only slightly supercoiled reveal the relative alignment of filaments within the bundles and show that crossbridges appear to interact with four actin monomers, apparently linking two actin monomers on one strand of one filament to the nearest two monomers on a neighbouring filament. However, the cross-bridges are not spaced at equal intervals corresponding to four actin subunits, presumably because of the lack of hexagonal symmetry in the individual filaments, which have about 14 actin monomers between cross-overs. Instead, the cross-bridges are arranged quasiequivalently along the longitudinal axis of the bundles, in steps of four or five actin subunit spacings (28 Å each).     

Movement of the actin filament bundle in Mytilus sperm: a new mechanism is proposed

An actin filament bundle approximately 2-5 microns in length is present in the sperm of the blue mussel, Mytilus. In unfired sperm this bundle extends from the midpiece through a canal in the center of the nucleus to terminate on the membrane limiting the inside of the cone-shaped acrosomal vacuole. The bundle is composed of 45-65 actin filaments which are hexagonally packed and regularly cross-bridged together to form an actin paracrystal so well ordered that it has six nearly equal faces. Upon induction of the acrosomal reaction, a needle-like process is formed in a few seconds. Within this process is the actin filament bundle which appears unchanged in filament number and packing as determined by optical diffraction methods. Using fluorescein-conjugated phalloidin we were able to establish that the bundle does not change length but instead is projected anteriorly out of the midpiece and nuclear canal like an arrow. Existing mechanisms to explain this extension cannot apply. Specifically, the bundle does not increase in length (no polymerization), does not change its organization (no change in actin twist), does not change filament number (no filament sliding), and cannot move by myosin (wrong polarity). Thus we are forced to look elsewhere for a mechanism and have postulated that at least a component of this movement, or cell elongation, is the interaction of the actin filament bundle with the plasma membrane.     

Actin filaments, stereocilia, and hair cells of the bird cochlea. II. Packing of actin filaments in the stereocilia and in the cuticular plate and what happens to the organization when the stereocilia are bent

A comparison of hair cells from different parts of the cochlea reveals the same organization of actin filaments; the elements that vary are the length and number of the filaments. Thin sections of stereocilia reveal that the actin filaments are hexagonally packed and from diffraction patterns of these sections we found that the actin filaments are aligned such that the crossover points of adjacent actin filaments are in register. As a result, the cross-bridges that connect adjacent actin filaments are easily seen in longitudinal sections. The cross-bridges appear as regularly spaced bands that are perpendicular to the axis of the stereocilium. Particularly interesting is that, unlike what one might predict, when a stereocilium is bent or displaced, as might occur during stimulation by sound, the actin filaments are not compressed or stretched but slide past one another so that the bridges become tilted relative to the long axis of the actin filament bundle. In the images of bent bundles, the bands of cross- bridges are then tilted off perpendicular to the stereocilium axis. When the stereocilium is bent at its base, all cross-bridges in the stereocilium are affected. Thus, resistance to bending or displacement must be property of the number of bridges present, which in turn is a function of the number of actin filaments present and their respective lengths. Since hair cells in different parts of the cochlea have stereocilia of different, yet predictable lengths and widths, this means that the force needed to displace the stereocilia of hair cells located at different regions of the cochlea will not be the same. This suggests that fine tuning of the hair cells must be a built-in property of the stereocilia. Perhaps its physiological vulnerability may result from changes of stereociliary structure.     

Crystallographic conformers of actin in a biologically active bundle of filaments

Actin carries out many of its cellular functions through its filamentous form; thus, understanding the detailed structure of actin filaments is an essential step in achieving a mechanistic understanding of actin function. The acrosomal bundle in the Limulus sperm has been shown to be a quasi-crystalline array with an asymmetric unit composed of a filament with 14 actin-scruin pairs. The bundle in its true discharge state penetrates the jelly coat of the egg. Our previous electron crystallographic reconstruction demonstrated that the actin filament cross-linked by scruin in this acrosomal bundle state deviates significantly from a perfect F-actin helix. In that study, the tertiary structure of each of the 14 actin protomers in the asymmetric unit of the bundle filament was assumed to be constant. In the current study, an actin filament atomic model in the acrosomal bundle has been refined by combining rigid-body docking with multiple actin crystal structures from the Protein Data Bank and constrained energy minimization. Our observation demonstrates that actin protomers adopt different tertiary conformations when they form an actin filament in the bundle. The scruin and bundle packing forces appear to influence the tertiary and quaternary conformations of actin in the filament of this biologically active bundle.     

Three-dimensional structure of a single filament in the Limulus acrosomal bundle: scruin binds to homologous helix-loop-beta motifs in actin

Frozen, hydrated acrosomal bundles from Limulus sperm were imaged with a 400 kV electron cryomicroscope. Segments of this long bundle can be studied as a P1 crystal with a unit cell containing an acrosomal filament with 28 actin and 28 scruin molecules in 13 helical turns. A novel computational procedure was developed to extract single columns of superimposed acrosomal filaments from the distinctive crystallographic view. Helical reconstruction was used to generate a three-dimensional structure of this computationally isolated acrosomal filament. The scruin molecule is organized into two domains which contact two actin subunits in different strands of the same actin filament. A correlation of Holmes' actin filament model to the density in our acrosomal filament map shows that actin subdomains 1, 2, and 3 match the model density closely. However, actin subdomain 4 matches rather poorly, suggesting that interactions with scruin may have altered actin conformation. Scruin makes extensive interactions with helix-loop-beta motifs in subdomain 3 of one actin subunit and in subdomain 1 of a consecutive actin subunit along the genetic filament helix. These two actin subdomains are structurally homologous and are closely spaced along the actin filament. Our model suggests that scruin, which is derived from a tandemly duplicated gene, has evolved to bind structurally homologous but non-identical positions across two consecutive actin subunits.     

Actin filaments in the acrosomal reaction of Limulus sperm. Motion generated by alterations in the packing of the filaments

When Limulus sperm are induced to undergo the acrosomal reaction, a process, 50 mum in length, is generated in a few seconds. This process rotates as it elongates; thus the acrosomal process literally screws through the jelly of the egg. Within the process is a bundle of filaments which before induction are coiled up inside the sperm. The filament bundle exists in three stable states in the sperm. One of the states can be isolated in pure form. It is composed of only three proteins whose molecular weights (mol wt) are 43,000, 55,000, and 95,000. The 43,000 mol wt protein is actin, based on its molecular weight, net charge, morphology, G-F transformation, and heavy meromyosin (HMM) binding. The 55,000 mol wt protein is in equimolar ratio to actin and is not tubulin, binds tenaciously to actin, and inhibits HMM binding. Evidence is presented that both the 55,000 mol wt protein and the 95,000 mol wt protein (possibly alpha-actinin) are also present in Limulus muscle. Presumably these proteins function in the sperm in holding the actin filaments together. Before the acrosomal reaction, the actin filaments are twisted over one another in a supercoil; when the reaction is completed, the filaments lie parallel to each other and form an actin paracrystal. This change in their packing appears to give rise to the motion of the acrosomal process and is under the control of the 55,000 mol wt protein and the 95,000 mol wt protein.     

Actin filaments elongate from their membrane-associated ends

In limulus sperm an actin filament bundle 55 mum in length extends from the acrosomal vacuole membrane through a canal in the nucleus and then coils in a regular fashion around the base of the nucleus. The bundle expands systematically from 15 filaments near the acrosomal vacuole to 85 filaments at the basal end. Thin sections of sperm fixed during stages in spermatid maturation reveal that the filament bundle begins to assemble on dense material attached to the acrosomal vacuole membrane. In micrographs fo these early stages in maturation, short bundles are seen extending posteriorly from the dense material. The significance is that these short, developing bundles have about 85 filaments, suggesting that the 85-filament end of the bundle is assembled first. By using filament bundles isolated and incubated in vitro with G actin from muscle, we can determine the end “preferred” for addition of actin monomers during polymerization. The end that would be associated with the acrosomal vacuole membrane, a membrane destined to be continuous with the plasma membrane, is preferred about 10 times over the other, thicker end. Decoration of the newly polymerized portions of the filament bundle with subfragment 1 of myosin reveals that the arrowheads point away from the acrosomal vacuole membrane, as is true of other actin filament bundles attached to membranes. From these observations we conclude that the bundle is nucleated from the dense material associated with the acrosomal vacuole and that monomers are added to the membrane-associated end. As monomers are added at the dense material, the thick first-made end of the filament bundle is pushed down through the nucleus where, upon reaching the base of the nucleus, it coils up. Tapering is brought about by the capping of the peripheral filaments in the bundle.     

Bending stiffness of a crystalline actin bundle

The acrosomal process of the sperm of the horseshoe crab (Limulus polyphemus) is a unique crystalline actin bundle, consisting of multiple actin filaments cross-linked by the actin-bundling protein, scruin. For successful fertilization, the acrosomal bundle must penetrate through a 30 microm thick jelly coat surrounding the egg and thus it must be sufficiently stiff. Here, we present two measurements of the bending stiffness of a single crystalline bundle of actin. Results from these measurements indicate that the actin:scruin composite bundle has an average elastic modulus of 2 GPa, which is similar to that of a single actin filament, and a bending stiffness that is more than two orders of magnitude larger than that of a bundle of uncross-linked actin filaments due to stiffening by the scruin matrix.     

Modeling rigor cross-bridge patterns in muscle I. Initial studies of the rigor lattice of insect flight muscle.

We have undertaken some computer modeling studies of the cross-bridge observed by Reedy in insect flight muscle so that we investigate the geometric parameters that influence the attachment patterns of cross-bridges to actin filaments. We find that the appearance of double chevrons along an actin filament indicates that the cross-bridges are able to reach 10--14 nm axially, and about 90 degrees around the actin filament. Between three and five actin monomers are therefore available along each turn of one strand of actin helix for labeling by cross-bridges from an adjacent myosin filament. Reedy's flared X of four bridges, which appears rotated 60 degrees at successive levels on the thick filament, depends on the orientation of the actin filaments in the whole lattice as well as on the range of movement in each cross-bridge. Fairly accurate chevrons and flared X groupings can be modeled with a six-stranded myosin surface lattice. The 116-nm long repeat appears in our models as "beating" of the 14.5-nm myosin repeat and the 38.5-nm actin period. Fourier transforms of the labeled actin filaments indicate that the cross-bridges attach to each actin filament on average of 14.5 nm apart. The transform is sensitive to changes in the ease with which the cross-bridge can be distorted in different directions.     

Helical arrangement of filaments in microvillar actin bundles

Actin filament arrays in in vivo microvillar bundles of rat intestinal enterocyte were re-evaluated using electron tomography (ET). Conventional electron microscope observation of semi-thin cross sections (300nm thick) of high-pressure freeze fixed and resin embedded brush border has shown a whirling pattern in the center of the microvilli instead of hexagonally arranged dots, which strongly suggests that the bundle consists of a non-parallel array of filaments. A depth compensation method for the ET was developed to estimate the actual structure of the actin bundle. Specimen shrinkage by beam irradiation during image acquisition was estimated to be 63%, and we restored the original thickness in the reconstruction. The depth compensated tomogram displayed the individual actin filaments within the bundles and it indicated that the actin filaments do not lie exactly parallel to each other: instead, they are twisted in a clockwise coil with a pitch of ～120°/μm. Furthermore, the lattice of actin filaments was occasionally re-arranged within the bundle. As the microvillar bundle mechanically interacts with the membrane and is thought to be compressed by the membrane's faint tensile force, we removed the shrouding membrane using detergents to eliminate the mechanical interaction. The bared bundles no longer showed the whirling pattern, suggesting that the bundle had released its coiled property. These findings indicate that the bundle has not rigid but elastic properties and a dynamic transformation in its structure caused by a change in the mechanical interaction between the membrane and the bundle.     

Cross-bridge number, position, and angle in target zones of cryofixed isometrically active insect flight muscle

Electron micrographic tomograms of isometrically active insect flight muscle, freeze substituted after rapid freezing, show binding of single myosin heads at varying angles that is largely restricted to actin target zones every 38.7 nm. To quantify the parameters that govern this pattern, we measured the number and position of attached myosin heads by tracing cross-bridges through the three-dimensional tomogram from their origins on 14.5-nm-spaced shelves along the thick filament to their thin filament attachments in the target zones. The relationship between the probability of cross-bridge formation and axial offset between the shelf and target zone center was well fitted by a Gaussian distribution. One head of each myosin whose origin is close to an actin target zone forms a cross-bridge most of the time. The probability of cross-bridge formation remains high for myosin heads originating within 8 nm axially of the target zone center and is low outside 12 nm. We infer that most target zone cross-bridges are nearly perpendicular to the filaments (60% within 11 degrees ). The results suggest that in isometric contraction, most cross-bridges maintain tension near the beginning of their working stroke at angles near perpendicular to the filament axis. Moreover, in the absence of filament sliding, cross-bridges cannot change tilt angle while attached nor reach other target zones while detached, so may cycle repeatedly on and off the same actin target monomer.     

Macromolecular structure of reassembled neurofilaments as revealed by the quick-freeze deep-etch mica method: difference between NF-M and NF-H subunits in their ability to form cross-bridges.

Neurofilament (NF) structure and ability to form cross-bridges were examined by quick-freeze deep-etch mica and low-angle rotary-shadow electron microscopy in NFs purified from bovine spinal cord and reassembled in various combinations of NF subunits. When NFs were reassembled from triplet proteins, NF-L, NF-M and NF-H, they were oriented randomly and often fragmented, but their elongated filaments (12-15 nm wide) and the cross-bridges (4-5 nm wide) connecting them were similar in appearance to those of isolated bovine NFs or in vivo rat NFs. Projections extended from the wall of the core filament in almost the same pattern as the cross-bridges and were the same in width and interval (minimum interval, 20-25 nm) as the cross-bridges. Projections were more conspicuous when core filaments were separated by 60 to 80 nm or more, while cross-bridges were more conspicuous when core filaments were close to each other. Projections or cross-bridges extended bilaterally at intervals of 20 to 25 nm where core filaments expanded and formed a network between filaments which were far from one another. When NFs were reconstructed from NF-L alone, only core filaments appeared, the same width as the filaments of triplet NFs. The core filaments were occasionally in almost direct contact with each other, with no projection or cross-bridge. When NFs were reassembled from NF-M alone or NF-L + NF-M, although NF-M core filaments were shorter and slightly thinner than NF-L + NF-M core filaments, both had projections, and both had cross-bridges, but cross-bridges were less evident. Cross-bridges were almost the same in width as those of triplet NFs, but significantly shorter and much less frequent although the minimum interval was the same, and core filaments were not attached to each other. In contrast, when NFs were reconstituted from NF-H alone or NF-L + NF-H, both had conspicuous projections and cross-bridges, similar to those of triplet NFs. Thus, when NFs contained NF-H, they formed frequent cross-bridges and long projections with extensive peripheral branching. When NFs contained NF-M but no NF-H, they tended to form cross-bridges, and to form projections that were shorter and straighter and without peripheral branching. That is, there appears to be a significant difference between NF-M and NF-H in ability to form cross-bridges and thus in interaction with adjacent NFs.     

Actin from Thyone sperm assembles on only one end of an actin filament: a behavior regulated by profilin

Thyone sperm were demembranated with Triton X-100 and, after washing, extracted with 30 mM Tris at pH 8.0 and 1 mM MgCl2. After the insoluble contaminants were removed by centrifugation, the sperm extract was warmed to 22 degrees C. Actin filaments rapidly assembled and aggregated into bundles when KCl was added to the extract. When we added preformed actin filaments, i.e., the acrosomal filament bundles of Limulus sperm, to the extract, the actin monomers rapidly assembled on these filaments. What was unexpected was that assembly took place on only one end of the bundle--the end corresponding to the preferred end for monomer addition. We showed that the absence of growth on the nonpreferred end was not due to the presence of a capper because exogenously added actin readily assembled on both ends. We also analyzed the sperm extract by SDS gel electrophoresis. Two major proteins were present in a 1:1 molar ratio: actin and a 12,500-dalton protein whose apparent isoelectric point was 8.4. The 12,500-dalton protein was purified by DEAE chromatography. We concluded that it is profilin because of its size, isoelectric point, molar ratio to actin, inability to bind to DEAE, and its effect on actin assembly. When profilin was added to actin in the presence of Limulus bundles, addition of monomers on the nonpreferred end of the bundle was inhibited, even though actin by itself assembled on both ends. Using the Limulus bundles as nuclei, we determined the critical concentration for assembly off each end of the filament and estimated the Kd for the profilin-actin complex (approximately 10 microM). We present a model to explain how profilin may regulate the extension of the Thyone acrosomal process in vivo: The profilin-actin complex can add to only the preferred end of the filament bundle. Once the actin monomer is bound to the filament, the profilin is released, and is available to bind to additional actin monomers. This mechanism accounts for the rapid rate of filament elongation in the acrosomal process in vivo.     

Actin-like filaments in the acrosomal apparatus of spermatozoa of a sea urchin

The acrosomal apparatus of a sea urchin, Echinocardium cordatum, consists of an acrosomal vesicle and a post-acrosomal rod. The rod is 2.5 μm long and extends from the acrosomal vesicle to the bottom of a nuclear invagination. The rod consists of a bundle of longitudinally disposed, 60 Å thick, actin-like filaments which bind heavy meromyosin to form arrowhead complexes. The actin-like filaments may have a dual function in the fertilization process: (1) extension of the acrosomal process through the egg investments; (2) incorporation of the sperm nucleus.     

Actin filaments, stereocilia, and hair cells of the bird cochlea. IV. How the actin filaments become organized in developing stereocilia and in the cuticular plate

In 8-day-old embryos stereocilia can be identified on the hair cells of the chick cochlea; within each is a small population of actin filaments which extend from the tip of the stereocilium to the apical cytoplasm of the cell. These filaments are not ordered in a regular way, however, and tend to be found near the lateral margins of the stereocilia with large spaces between adjacent filaments. By 9 days the spaces between adjacent filaments are reduced and there are regions where the crossover points of adjacent actin helices are in register even though in cross section the actin filaments do not lie on a regular lattice. By 10-11 days the actin filaments become progressively more crossbridged together and we can recognize in longitudinal section horizontal stripes caused by the periodicity of the crossbridges. In transverse section the filaments begin to lie on a hexagonal lattice. Each stereocilium, however, contains less than 100 actin filaments. Evidence is presented that once crossbridging is maximal and the filaments hexagonally packed (Days 11-12), the stereocilia increase in width by the orderly addition of actin filaments to the lateral margins of the existing filament bundle so that by Day 16 we find up to 400 filaments all packed on a hexagonal lattice. Thus there are two stages in bundle formation. In the first a small number of filaments condense into a hexagonally packed, crosslinked bundle. In the second, the bundle increases in diameter by addition of filaments to the periphery of the bundle in a process akin to crystal growth. From observations on the elongation of filaments in the rootlets and stereocilia, we conclude that rootlets grow by addition of subunits at the nonpreferred end while stereocilia elongate by addition to the preferred end. What makes this interesting is that these two modes of addition occur at different developmental times.     

Direct electron microscopic visualization of barbed end capping and filament cutting by intestinal microvillar 95-kdalton protein (villin): a new actin assembly assay using the Limulus acrosomal process

We have re-examined the Ca(++)-dependent interaction of an intestinal microvillar 95- kdalton protein (MV-95K) and actin using the isolated acrosomal process bundles from limulus sperm. Making use of the processes as nuclei for assembling actin filaments, we quantitatively and qualitatively examined MV-95K’s effect on filament assembly and on F- actin, both in the presence and in the absence of Ca(++). The acrosomal processes are particularly advantageous for this approach because they nucleate large numbers of filaments, they are extremely stable, and their morphology can be used to determine the polarity of any nucleated filaments. When filament nucleation was initiated in the presence of MV-95K and the absence of Ca(++), there was biased filament assembly from the bundle ends. The calculated elongation rates from both the barbed and pointed filament ends were virtually indistinguishable from control preparations. In the presence of Ca(++), MV-95K completely inhibited filament assembly from the barbed filament end without affecting the initial rate of assembly from the pointed filament end. The inhibition of assembly results from MV-95K binding to and capping the barbed filament end, thereby preventing monomer addition. This indicates that, while MV-95K is a potent nucleator of actin assembly, it is also a potent inhibitor of actin filament elongation. To examine the effects of MV-95K on F-actin in the presence of Ca(++), we developed an assay where MV-95K is added to filaments previously assembled from acrosomal processes without causing filament breakage during mixing. These results clearly demonstrated that rapid filament shortening by MV-95K results through a mechanism of disrupting intrafilament monomer-monomer interactions. Finally, we show that tropomyosin-containing actin filaments are insensitive to cutting, but not to capping, by MV-95K in the presence of Ca(++).     

Crystallographic analysis of acrosomal bundle from Limulus sperm

The acrosomal process of Limulus sperm contains a bundle of filaments composed of actin and a 102 kDa protein in a 1:1 molar ratio. The structure of the bundle in true discharge was investigated by electron cryomicroscopy, X-ray scattering and crystallographic image analysis. A bundle can be characterized as a quasi-crystal with continuously varying views along the bundle axis. Each segment of the bundle is found to obey the symmetry of space group P1, with a = b = 147 A, c = 762 A, alpha = 90 degrees, beta = 90.6 degrees, gamma = 120 degrees. A unit cell contains a helical repeat of the filament with a selection rule following that of an actin filament. A 24 A projection map based on the h0l view was reconstructed after averaging 5300 unit cells from six electron images. Filaments in this projection are well separated and clearly display a 21 screw symmetry. This screw symmetry results from the helical parameters of the bundle filament and is found to be a non-crystallographic symmetry element present in the unit cell. Our structural analysis has led to the proposal that the assembly of a stable bundle with a defined maximum diameter can be controlled by the crystallographic packing of the twisted filaments.     

Cytoskeletal reorganization of human platelets after stimulation revealed by the quick-freeze deep-etch technique

We studied the cytoskeletal reorganization of saponized human platelets after stimulation by using the quick-freeze deep-etch technique, and examined the localization of myosin in thrombin-treated platelets by immunocytochemistry at the electron microscopic level. In unstimulated saponized platelets we observed cross-bridges between: adjoining microtubules, adjoining actin filaments, microtubules and actin filaments, and actin filaments and plasma membranes. After activation with 1 U/ml thrombin for 3 min, massive arrays of actin filaments with mixed polarity were found in the cytoplasm. Two types of cross-bridges between actin filaments were observed: short cross-bridges (11 +/- 2 nm), just like those observed in the resting platelets, and longer ones (22 +/- 3 nm). Actin filaments were linked with the plasma membrane via fine short filaments and sometimes ended on the membrane. Actin filaments and microtubules frequently ran close to the membrane organelles. We also found that actin filaments were associated by end-on attachments with some organelles. Decoration with subfragment 1 of myosin revealed that all the actin filaments associated end-on with the membrane pointed away in their polarity. Immunocytochemical study revealed that myosin was present in the saponin-extracted cytoskeleton after activation and that myosin was localized on the filamentous network. The results suggest that myosin forms a gel with actin filaments in activated platelets. Close associations between actin filaments and organelles in activated platelets suggests that contraction of this actomyosin gel could bring about the observed centralization of organelles.     

Polymerization of sperm actin in the presence of cytochalasin-B.

The polymerization of globular actin to fibrous actin which occurs when sperm are activated, was not inhibited by cytochalasin-B. The acrosomal filament and its component actin filaments formed in the presence of cytochalasin-B; and once formed, the actin filaments did not depolymerize when exposed to cytochalasin-B.     

Actin paracrystal in the acrosome of newt sperm

When a newt sperm-head was treated with trypsin and DNase, an arrow-like thin rod was revealed. This rod presumably corresponds to the ‘perforatorium’ described by Picheral [1, 2] in Pleurodele sperm. It consisted of one apical and one caudal part. In the apical part there appeared to be an envelope with a 530 Å structural repeat, inside which coursed a filament bundle, presumably identical with that in the caudal part. In the caudal part, a characteristic filament bundle, quite similar to the paracrystal of rabbit skeletal actin [3], was observed after extensive treatment with trypsin. The optical diffraction pattern of this bundle indicates that it has the same helical symmetry as that of rabbit skeletal actin [4] but slightly different from that of the acrosomal process of Limulus sperm [5]. The diffraction pattern frequently has a strong meridional reflection at about (27 Å)⁻¹, which is usually observed only with low intensity in the actin paracrystals. This fact suggests that the structural unit in the bundle has a shape considerably different from that of the usual G-actin.