Dark-field Light Microscopy Research Articles

Surface-Induced Polymerization of Actin

Living cells contain a very large amount of membrane surface area, which potentially influences the direction, the kinetics, and the localization of biochemical reactions. This paper quantitatively evaluates the possibility that a lipid monolayer can adsorb actin from a nonpolymerizing solution, induce its polymerization, and form a 2D network of individual actin filaments, in conditions that forbid bulk polymerization. G- and F-actin solutions were studied beneath saturated Langmuir monolayers containing phosphatidylcholine (PC, neutral) and stearylamine (SA, a positively charged surfactant) at PC:SA = 3:1 molar ratio. Ellipsometry, tensiometry, shear elastic measurements, electron microscopy, and dark-field light microscopy were used to characterize the adsorption kinetics and the interfacial polymerization of actin. In all cases studied, actin follows a monoexponential reaction-limited adsorption with similar time constants (∼10 3 s). At a longer time scale the shear elasticity of the monomeric actin adsorbate increases only in the presence of lipids, to a 2D shear elastic modulus of μ ≈ 30 mN/m, indicating the formation of a structure coupled to the monolayer. Electron microscopy shows the formation of a 2D network of actin filaments at the PC:SA surface, and several arguments strongly suggest that this network is indeed causing the observed elasticity. Adsorption of F-actin to PC:SA leads more quickly to a silghtly more rigid interface with a modulus of μ ≈ 50 mN/m.

Self-Diffusion in Concentrated Colloid Suspensions Studied by Digital Video Microscopy of Core−Shell Tracer Particles

Optical video microscopy and digital image processing have been used to study the self-diffusion of colloidal particles with a hard-sphere potential. The colloid particles consist of cross-linked polymers and are dispersed in a good solvent to avoid aggregation. To investigate single particle motion in highly concentrated dispersions, a host−tracer system, consisting of two different kinds of polymer particles, has been designed: the host particles are made of poly-t-butylacrylate (with ethanedioldiacrylate as cross-linker) and have the same refractive index as the employed solvent, 4-fluorotoluene. The tracer particles have a core−shell structure with a polystyrene core (cross-linked with m-diisopropenylbenzene) and a shell consisting of cross-linked poly-t-butylacrylate to match surface properties and interaction potential to those of the “invisible” particles. The motion of the strongly scattering core−shell particles (“tracer” particles) was observed by dark-field light microscopy. From the obtained ...

Calcium-dependent bidirectional power stroke of the dynein arms in sea urchin sperm axonemes.

Active sliding between doublet microtubules of sea urchin sperm axonemes that were demembranated with Triton X-100 in the presence or absence of calcium was induced with ATP and elastase at various concentrations of Ca2+ to examine the effects of Ca2+ on the direction of the power stroke of the dynein arms. Dark-field light microscopy of microtubule sliding revealed that the sliding from the axonemes demembranated with Triton and millimolar calcium and disintegrated with ATP and elastase showed various patterns of sliding disintegration, including loops of doublet microtubules formed near the head or the basal body. These loops were often thicker than the remaining axonemal bundle. In contrast, only thinner loops were found from the axonemes demembranated with Triton in the absence of calcium and disintegrated with ATP and elastase at high Ca2+ concentrations. Electron microscopic examination of the direction of microtubule sliding showed that the doublet microtubules in the axonemes demembranated in the presence of millimolar calcium moved toward the base of the axonemes by the dynein arms on the adjacent doublet microtubule as well as by their own dynein arms. Doublet microtubules in the axonemes demembranated in the absence of calcium moved toward the base of the axonemes only by their own dynein arms. Similar observations have been obtained from the axonemes from which the outer dynein arms were selectively extracted. From these observations, we can conclude that the dynein arms generate force in both directions and this feature of the dynein arms arises from at least the inner dynein arms.

Aspects of the mechanics of lobed liposomes.

Hotani has studied, by means of dark-field light microscopy, morphological transformations which unilamellar liposomes undergo when their interior volume decreases steadily with time as a consequence of osmosis. In a previous paper, we made a theoretical study of the initial buckling of an originally spherical vesicle into the observed oblate spheroidal shape; and we argued that some in-plane shear elastic stiffness is required-in addition to the well-known flexural stiffness of the lipid bilayer-in order to explain the observed phenomena. In the present paper, we consider a later stage in the chain of morphological transitions observed by Hotani, when a series of cudgel-shaped lobes have sprung out of a previously axisymmetric, biconcave-shaped vesicle. Specifically, we compare the observed shapes of such lobes with half of a series of "peanut"-shaped vesicles that are an equilibrium conformation of an initially spherical liposome under reduced internal volume. We find that the shapes do not match well. On the other hand, the observed lobe forms do match satisfactorily portions of "undulating tube" shapes which evolve from a hypothetical cylindrical vesicle, according to some simple calculations. In view of this agreement, we are led to propose that the formation of cudgel-shaped lobes requires some sliding of one lipid monolayer over another. This conflicts, of course, with the Love-Kirchhoff hypothesis which is normally invoked at the outset of analyses of lipid vesicles by means of classical thin-shell theory; but it is in accord with previous suggestions in the context of more obviously severe distortion of the lipid bilayer.

Spiroplasma syrphidicola sp. nov., from a syrphid fly (Diptera: Syrphidae).

Spiroplasma sp. strain EA-1(T) (T = type strain) (subgroup VIII-1), which was isolated from the syrphid fly Eristalis arbustorum, was serologically distinct from other spiroplasma species, groups, and subgroups, The cells of this strain, as revealed by dark-field light microscopy, were short, helical, and motile. An electron microscopic examination revealed wall-less cells delimited by a single membrane. The unusually short cells passed through 220-nm filter pores with no reduction in titer. The organisms grew well in SM-1, M1D, and SP-4 liquid media. Growth also occurred in conventional horse serum medium and 1% serum fraction medium. Strain EA-1(T) grew at temperatures between 10 and 41 degrees C, and optimum growth occurred at 32 degrees C. The doubling time at the optimal temperature was 1.0 h. The strain catabolized glucose and hydrolyzed arginine but did not hydrolyze urea. The guanine-plus-cytosine content of the DNA was 30 +/- 1 mol%. The genome size was about 1,230 kbp. Strain Ea-1 (= ATCC 33826), which represents subgroup VIII-1, is designated the type strain of a new species, Spiroplasma syrphidicola.

Chapter 30 Reactivation of Chlamydomonas Cell Models

Unicellular biflagellate alga Chlamydomonas has been used to study how changes in the surrounding medium can alter axonemal motility. This chapter describes a procedure for the preparation of these models, with particular reference to their use in examining the effects of free calcium concentration on axonemal motility. The basic technique is applicable not only to the study of calcium effects, but to the effect of any soluble substance that acts on a detergent-stable component of the axoneme. Similar Chlamydomonas cell models have been useful for investigating the functional rebinding of purified dynein to outer-doublet microtubules. In this approach, the cell's plasma membrane is disrupted by the addition of a nonionic detergent, leaving the cell wall, axonemes, and most internal cell components apparently intact. These resulting cell models are then reactivated by dilution into a reactivation buffer containing ATP. Through the addition of ethylene glycol bis(β-aminoethyl ether)- N,N’ -tetraacetic acid (EGTA) and CaCl 2 , to the reactivation buffer, the amount of free Ca 2+ during reactivation can be carefully regulated. Dark-field light microscopic observation of reactivated cell models allows the integrity of the axonemes, as well as changes in swimming behavior, to be monitored. In studies comparing cell models reactivated at 10 -7 and 10 -9 M Ca 2+ , it has been established that the cell's two axonemes are differentially sensitive to calcium. The chapter describes the solutions and the procedure for the experiment. Cell models are very fragile and easily damaged. Dark-field light microscopy allows the condition of the axonemes to be assessed during the assay. Broken axonemes and axonemes in which the microtubules have splayed apart at the distal end are common forms of damage. Additionally, cell models may be observed in which one axoneme is completely inactivated because of extrusion of the central pair microtubules, which appear coiled at the distal end of the axoneme.

Self-assembly into fibrils of collagen II by enzymic cleavage of recombinant procollagen II. Lag period, critical concentration, and morphology of fibrils differ from collagen I

A recently developed recombinant system for synthesis of human procollagen II by stably transfected host cells was used to prepare adequate amounts of protein to study the self-assembly of collagen II into fibrils. The procollagen II was cleaved to pCcollagen II by procollagen N-proteinase (EC 3.4.24.14), the pCcollagen II was chromatographically purified, and the pCcollagen II was then used as a substrate to generate collagen II fibrils by cleavage with procollagen C-proteinase. The kinetics for assembly of collagen II fibrils were similar to those observed previously for the self-assembly of collagen I in that a distinct lag phase was observed followed by a sigmoidal propagation phase. However, under the same experimental conditions, the lag time for assembly of collagen II fibrils was 5-6-fold longer, and the propagation rate for collagen II fibrils was about 30-fold lower than for collagen I fibrils. The relatively long lag time for the assembly of collagen II into fibrils made it possible to demonstrate that most of the conversion of pCcollagen II to collagen II occurred in the solution phase. The critical concentration at 37 degrees C for collagen II was about 50-fold greater than the critical concentration for collagen I. The Gibbs free energy change for the assembly of collagen II into fibrils was -40 kJ/mol, a value that was about 14 kJ/mol less than the free energy change for collagen I and about the same as the free energy change for the homotrimer of collagen I. Dark-field light microscopy and negative-staining electron microscopy demonstrated that the collagen II fibrils were thin and formed network-like structures. The results demonstrated, therefore, that the structural information of the monomer is sufficient to explain the characteristically small diameters and arcade-like geometry of collagen II fibrils found in cartilage and other tissues.

Self-assembly of collagen I from a proband homozygous for a mutation that substituted serine for glycine at position 661 in the alpha 2(I) chain. Possible relationship between the effects of mutations on critical concentration and the severity of the phenotype

Procollagen I was isolated from cultured skin fibroblasts from a proband who was homozygous for a mutation in the COL1A2 gene that substituted a serine codon for a glycine codon at position 661 of the alpha 2(I) chain. The procollagen I was cleaved to pCcollagen I by procollagen N-proteinase and the pCcollagen I was used as a substrate for assay of self-assembly of collagen I into fibrils. The mutated pCcollagen I was cleaved to collagen I by procollagen C-proteinase at the same rate as control pCcollagen I. However, self-assembly of the mutated collagen I had a lag period that was 15-fold greater than the lag period observed with normal collagen I under the same conditions. Also, self-assembly of the mutated collagen I had a propagation rate of about one-fourth of the propagation rate of normal collagen I. In addition, the critical concentration for fibril assembly was slightly increased. Rotary shadowing electron microscopy of the mutated procollagen I did not reveal any increased flexibility of the triple helix as was seen previously with two mutated procollagens I in which there were substitutions of cysteine for glycine residues in the alpha 1(I) chain (Vogel, B. E., Doelz, R., Kadler, K. E., Hojima, Y., Engel, J., and Prockop, D. J. (1988) J. Biol. Chem. 263, 19249-19255; Lightfoot, S. J., Holmes, D. F., Brass, A., Grant, M. E., Byers, P. H., and Kadler, K. E. (1992) J. Biol. Chem. 267, 25521-25528). However, morphometric analysis by dark-field light microscopy and electron microscopy showed that the fibrils formed from the mutated collagen I appeared thicker in diameter than the fibrils formed from the normal collagen I. Comparison of the results with similar data on four mutated procollagens previously studied raised the possibility that mutations which markedly increase the critical concentration of fibril assembly produce more severe phenotypes than mutations which change other parameters of fibril assembly.

Three-Dimensional Laser-Scanning Confocal Microscopy of In Situ Hybridization in the Skin

In situ hybridization is an important tool in molecular and developmental biology to detect specific nucleic acid sequences (either mRNA or DNA) within cells. This technique is especially applicable to tissue sections since it provides information about the spatial distribution of DNA or mRNA sequences. However, previous studies utilizing in situ hybridization in the skin were hampered by a high degree of nonspecific background, which has made interpretation of the results difficult. In this paper, we demonstrate how refinements in in situ hybridization techniques, combined with laser-scanning confocal microscopy, significantly reduce nonspecific background and produce improved resolution of in situ hybridization in skin specimens. The sensitive detection method of laser-scanning confocal microscopy allows three-dimensional localization of S35 radioactive-labeled riboprobes within the emulsion of specimens, which is not possible with conventional bright or dark field light microscopy.

Functional studies of Alzheimer's disease tau protein

In vitro assays were used to monitor and compare the kinetic behavior of bovine tubulin polymerization enhanced by tau proteins isolated from Alzheimer's disease (AD) and nondemented (ND) age-matched control brains. Tau from AD cases induced slower polymerization and a steady state turbidity value approximately 50% of that stimulated by tau from control cases. Tau from the most severe AD case was least effective at promoting polymerization. Dark-field light microscopy of the control samples revealed abundant microtubule formation and many microtubule bundles. Microtubule assembly was observed in AD samples as well, but bundling was not obvious. These results were confirmed by negative-stain electron microscopy. Morphological analysis showed that AD tau-induced microtubules were longer than control microtubules. Furthermore, our initial results suggest that the reduction of AD tau activity is correlated with neurofibrillary pathology in AD brains. Earlier reports indicated that AD tau is modified by phosphorylation (Grundke-Iqbal et al., 1986; Wood et al., 1986; Iqbal et al., 1989; Brion et al., 1991a,b; Lee et al., 1991). Our results support the hypothesis that tau modification compromises its function by altering its ability to nucleate and bundle microtubules.

Neurofilaments move apart freely when released from the circumferential constraint of the axonal plasma membrane.

Squid giant axons were used to obtain axonal cytoskeletons that had been separated from the confines of their plasma membranes. To remove the plasma membrane, axoplasm was extruded from the giant axon directly into an artificial axoplasm solution (AAS). This procedure produces a smooth axoplasmic cylinder in which neurofilaments (NFs) are the most prevalent cytological elements. The NFs scatter light strongly and thus dark-field light microscopy can be used to quantify the volume occupied by these polymers. Measurements of the widths of the dark-field images of the axoplasmic cylinders showed that the cross-sectional area of the NF population increased by 60-110% (n = 8) between 1-100 min after plasma membrane removal, and then continued to increase more slowly for many hours. After 1,000 min, the cross-sectional area was 75-160% (n = 8) larger than at 1 min. These light microscopic measurements of axoplasm suggest that the NF population disperses to occupy a continuously increasing volume after removal of the plasma membrane and immersion in AAS. This inference was confirmed by quantitative ultrastructural studies of NFs in axoplasmic cross-sections, which demonstrated that the spacing between the NFs increased between 1-1,000 min after plasma membrane removal. Comparison of the NF density distribution after 1,000 min with a theoretical distribution calculated using the Poisson theorem indicated that the NFs dispersed randomly. These studies on NFs in isolated axoplasm suggest that ordinary thermal forces of Brownian motion are sufficient to move axonal NFs apart independently and thereby to disperse them. We propose that, in the intact axon, the dispersive movements of the NFs spread the NF cytoskeleton radially and expansively to fill out the cylindrical space contained by the axonal plasma membrane and its surrounding connective tissue elements.

Morphological changes in liposomes caused by polymerization of encapsulated actin and spontaneous formation of actin bundles.

Spherical giant liposomes that had encapsulated skeletal-muscle G-actin were made by swelling a dried lipid mixture of dimyristoyl phosphatidylcholine/cardiolipin, 1:1 (wt/wt), in a solution of G-actin/CaCl2 at 0 degree C. Polymerization of the encapsulated G-actin into actin filaments was achieved by raising the temperature to 30 degrees C. We observed the subsequent shape changes of the liposomes by dark-field and differential interference-contrast light microscopy. After approximately 40 min, which was required for completion of actin polymerization, two shapes of liposome were evident: dumbbell and disk. Elongation of the dumbbell-shaped liposomes was concomitant with actin polymerization. Polarization microscopy showed that actin filaments formed thick bundles in the liposomes and that these filaments lay contiguous to the periphery of the liposome. Localization of actin filaments in the liposomes was confirmed by observation of rhodamine phalloidin-conjugated actin filaments by fluorescence microscopy. Both dumbbell- and disk-shaped liposomes were rigid and kept their shapes as far as actin filaments were stabilized. In contrast, liposomes containing bovine serum albumin were fragile, and their shapes continually fluctuated from Brownian motion, indicating that the actin bundles served as mechanical support for the liposome shapes.

Turbid alkali feldspars from the Isle of Skye, northwest Scotland

Partially turbid alkali feldspars from hydrothermally altered Tertiary granites on the Isle of Skye (the Red Hills granites) were studied using light microscopy, scanning and transmission electron microscopies, and energy-dispersive X-ray spectroscopy. Limpid cores and turbid rims of individual crystals were compared to determine the causes of the turbidity. The limpid cores were cryptoperthitic, with lamellar widths of 0.1–0.3 μm. In contrast, the turbid rims contained K-rich and Narich areas coarsened to >0.5 μm. Turbid regions contained abundant inclusions, whereas limpid regions did not. Two generations of turbidity were recognized. Feldspars from the Beinn an Dubhaich granite, a granite with near-normal values for 18O/16O possessed limpid cores surrounded by turbid rims that cast a reddish-brown hue in transmitted light. When viewed in darkfield light microscopy, the regions with the reddish-brown turbidity were blue. This is consistent with the hypothesis that the cloudy appearance of these turbid regions arises from the scattering of light by micrometerto submicrometer-sized inhomogeneities in refractive index caused by fluid-filled cavities. Feldspars from the Loch Ainort granite, a granite with low values for 18O/16O possessed limpid and reddish-brown-turbid cores surrounded by turbid rims that cast a blackish hue in transmitted light. Ion thinning of the turbid areas produced an abundance of small holes (≤1–2 μm) apparently the remains of fluid inclusions. Transmission electron microscopy revealed that some holes from regions of reddish-brown turbidity contained non-feldspar material, including halite and metal-rich phases of various compositions. In contrast, blackish turbid regions contained cavities filled with alteration products, such as kaolinite. Hence, the feldspars from granites on the Isle of Skye apparently record interactions with at least two fluids: a saline fluid (possibly a late-stage magmatic fluid) and a meteoric fluid.

Dynamic features of microtubules as visualized by dark-field microscopy

We have reviewed recent progress in the dynamic features of microtubules in vitro as visualized by dark-field light microscopy using high intensity illumination. Observations of individual microtubules in real-time have made it possible to analyze the unique characteristics of microtubules exactly. The following three topics have been discussed: (1) treadmilling, i.e., the simultaneous assembly of tubulin at one end and disassembly at the other end on a single microtubule at a steady state. (2) Dynamic instability, i.e., the very unusual phenomenon in which two populations of microtubules coexist: those in one population elongating while those in the other shortening in the absence of MAPs. Both ends of the microtubules exist either in the growing or the shortening phase, and alternate between the two phases in a stochastic manner. (3) Morphogenesis of liposomes by microtubule growth. Tubulin is encapsulated into model membrane vesicles, liposomes. Polymerization of the encapsulated tubulin causes a change in shape of the spherical liposomes to form bipolar or multipolar vesicles, suggesting that microtubules have an active function in the morphogenesis of membranous organelles and cells.

Same-section correlative light and electron microscopy

Epoxy embedded biological material, sectioned for conventional, intermediate or high-voltage electron microscopy (EM), can be visualized within the section with good contrast and detail by phase-contrast or dark-field light microscopy (LM). The contrast of such material is not substantially influenced by the type of embedding resin or section support substrate. It is, however, influenced by the type of fixation (glutaraldehyde with and without osmium postfixation), by heavy metal (uranyl and lead) staining, and by the section thickness. The ability to examine the specimen with the LM, within a section cut for EM, allows each section to be rapidly screened for content prior to examination in the EM. We have found this approach to be particularly useful for studies requiring the ultrastructural examination of a selected area or structure which is large enough to be visualized with the LM but which comprises only a small volume of the embedded material (e.g., centrosomes and nuclei within oocytes; specific regions of large protists.)Same section LM-EM can also be extended to sections cut from cells stained prior to embedding for the immunofluorescent localization of antigens using fluorescein, rhodamine or Texas red-conjugated antibodies. Under these conditions the sections show high resolution patterns of antigen-specific fluorescence against a background void of autoflouorescence. The fidelity in the correlation between the distribution of immunofluorescently labeled antigens and the ultrastructure in the same section can be extended to structures as small as a single microtubule or just a few actin filaments . This approach of same section correlative fluorescence microscopy (FLM) and EM can eliminate the need, in many instances, to employ more complex procedures such as immunoferritin or immunogold for labeling antigens for ultrastructural detection.

Imaging sub-micron objects with light microscopy: Visualization of the T-4 bacteriophage

While light microscopy has been used to image sub-micron objects, numerous problems with diffraction-limitations often preclude extraction of useful information. Using conventional dark-field and phase contrast light microscopy coupled with image processing, we have studied the following objects: (a) polystyrene beads (88nm, 264nm, and 557mn); (b) frustules of the diatom, Pleurosigma angulatum, and the T-4 bacteriophage attached to its host, E. coli or free in the medium. Equivalent images of the same areas of polystyrene beads and T-4 bacteriophages were produced using transmission electron microscopy.For light microscopy, we used a Zeiss universal microscope. For phase contrast observations a 100X Neofluar objective (N.A.=1.3) was applied. With dark-field, a 100X planachromat objective (N.A.=1.25) in combination with an ultra-condenser (N.A.=1.25) was employed. An intermediate magnifier (Optivar) was available to conveniently give magnification settings of 1.25, 1.6, and 2.0. The image was projected onto the back focal plane of a film or television camera with a Carl Zeiss Jena 18X Compens ocular.

Occurrence of Corn Stunt Spiroplasma at Different Elevations in Mexico

A survey of Spiroplasma kunkelii, or corn stunt spiroplasma (CSS), was conducted in Mexico from October 1985 to March 1988 using phase contrast or dark field light microscopy (DFM) and enzyme-linked immunosorbent assay (ELISA). Three types of symptoms were observed: consistently stunted plants whose leaves had well-defined broad chlorotic streaking and that were usually observed at 60-940 m above sea level, plants that were not always stunted but whose leaf margins showed red to purple streaks, and plants that usually were not stunted but whose leaves showed either a diffuse yellow or a chlorotic stripe condition with or without red margins. (…)

Isolation of a sodium dodecyl sulfate-insoluble transglutaminase substrate from liver plasma membranes.

Rat liver plasma membranes contain transglutaminase activity and a large molecular weight protein complex which serves as a substrate for this enzyme. When plasma membranes were solubilized in sodium dodecyl sulfate and disulfide-reducing agents the transglutaminase substrate was recovered in the detergent-insoluble fraction. The insolubility of the complex suggested that it might be further studied by adsorbing membranes onto glass slides, then extracting with the detergent and reducing agent. After extraction, dark field light microscopy revealed numerous flattened sheets which varied in size from 4 to 12 micrometers. To confirm that these structures were the large molecular weight transglutaminase substrate, the plasma membranes were solubilized in sodium dodecyl sulfate and dithiothreitol and sedimented through a sucrose gradient containing the agent. The large molecular weight substrate was the only material found at the 1.11/1.23 g/cm3 interface. Microscopic examination showed the same structures previously observed on the glass slides. We conclude that the large molecular weight transglutaminase substrate is a sodium dodecyl sulfate-insoluble, morphologically distinct, protein complex. Due to its considerable size, nondissociable nature, and association with the lateral membrane, the sodium dodecyl sulfate-insoluble transglutaminase substrate may serve as a type of skeleton or scaffolding for this plasma membrane domain.

Isolated cytoskeletons of human blood platelets: dark-field imaging of coiled and uncoiled microtubules

Detergent extraction of human blood platelets pre-treated with Taxol to stabilize microtubules allows isolation of marginal band (MB) cytoskeletons. We studied MB cytoskeleton structure using dark-field light microscopy and negative stain electron microscopy (EM). Dark-field illumination clearly demonstrated the “hoop” shape of MB cytoskeletons in unfixed suspension where the microtubule coils had a mean diameter of 2.87 μm (± 0.18 μm, SD). Microtubules were uncoiled by brief exposure to trypsin (2 mg/μg protein) or by NaCl (154–600 mM) but not by DNase I, which removed ∼40% of total actin, but had no effect on dark-field images of microtubule coils. As microtubules uncoiled, a single fiber emerged from the hoop and gradually lengthened as the brightness of the hoop diminished; these fibers correspond to the single microtubules seen by EM. Polypeptides of coiled and uncoiled MB cytoskeletons were analyzed by SDS-PAGE. When microtubules became uncoiled, no changes in the major components (α- and β-tubulin, IEF-51K, or actin) were found. However, a number (> 10) of minor polypeptides, each <5% of total cytoskeletal protein and with an Mr ranging from 80,000⪰ 260,000, were decreased in “uncoiled” MB cytoskeletons. These results implicate one or more of these minor polypeptides in maintenance of hoop integrity. Dark-field light microscopy thus provides an approach toward investigating the mechanisms(s) involved in maintaining the microtubule coil of the platelet marginal band.

Dynamics of microtubules visualized by darkfield microscopy: treadmilling and dynamic instability.

Individual microtubules undergoing treadmilling in vitro were visualized by darkfield light microscopy, and the relationship between treadmilling and dynamic instability was studied as a function of microtubule-associated proteins (MAPs). In order to demonstrate treadmilling directly by real-time observation, we constructed three-block microtubules, the center-block of which was decorated with Tetrahymena dynein. The decorated block can easily be distinguished from undecorated blocks in the darkfield microscope because the decorated one appears much thicker. At steady-state conditions, the length of an undecorated block at one end increased and that at another end decreased, while the decorated center-block did not change in its length. The results from these direct observations show that calf brain 3X-microtubules exhibit a treadmilling flux of 0.9 micron/h. Using a similar microscopy technique, we previously demonstrated that phosphocellulose PC-microtubules existed in either the growing or the shortening phase and alternated quite frequently at steady-state conditions (dynamic instability). How does treadmilling relate to dynamic instability? An image recording of individual 3X-microtubules containing MAPs revealed that the microtubules undergo treadmilling and do not exhibit any dynamic instability. This evidence shows that MAPs suppress the dynamic instability of microtubules. That is, treadmilling can take place in the steady state only after microtubules have been stabilized by MAPs.