Planar wire-array Z-pinch implosion dynamics and X-ray scaling at multiple-MA drive currents for a compact multisource hohlraum configuration.

An indirect drive configuration is proposed wherein multiple compact Z-pinch x-ray sources surround a secondary hohlraum. Planar compact wire arrays allow reduced primary hohlraum surface area compared to cylindrical loads. Implosions of planar arrays are studied at up to 15 TW x-ray power on Saturn with radiated yields exceeding the calculated kinetic energy, suggesting other heating paths. X-ray power and yield scaling studied from 1-6 MA motivates viewfactor modeling of four 6-MA planar arrays producing 90 eV radiation temperature in a secondary hohlraum.

Characteristics and scaling of tungsten-wire-array z -pinch implosion dynamics at 20 MA.

We present observations for 20-MA wire-array z pinches of an extended wire ablation period of 57%+/-3% of the stagnation time of the array and non-thin-shell implosion trajectories. These experiments were performed with 20-mm-diam wire arrays used for the double- z -pinch inertial confinement fusion experiments [M. E. Cuneo, Phys. Rev. Lett. 88, 215004 (2002)] on the Z accelerator [R. B. Spielman, Phys. Plasmas 5, 2105 (1998)]. This array has the smallest wire-wire gaps typically used at 20 MA (209 microm ). The extended ablation period for this array indicates that two-dimensional (r-z) thin-shell implosion models that implicitly assume wire ablation and wire-to-wire merger into a shell on a rapid time scale compared to wire acceleration are fundamentally incorrect or incomplete for high-wire-number, massive (>2 mg/cm) , single, tungsten wire arrays. In contrast to earlier work where the wire array accelerated from its initial position at approximately 80% of the stagnation time, our results show that very late acceleration is not a universal aspect of wire array implosions. We also varied the ablation period between 46%+/-2% and 71%+/-3% of the stagnation time, for the first time, by scaling the array diameter between 40 mm (at a wire-wire gap of 524 mum ) and 12 mm (at a wire-wire gap of 209 microm ), at a constant stagnation time of 100+/-6 ns . The deviation of the wire-array trajectory from that of a thin shell scales inversely with the ablation rate per unit mass: f(m) proportional[dm(ablate)/dt]/m(array). The convergence ratio of the effective position of the current at peak x-ray power is approximately 3.6+/-0.6:1 , much less than the > or = 10:1 typically inferred from x-ray pinhole camera measurements of the brightest emitting regions on axis, at peak x-ray power. The trailing mass at the array edge early in the implosion appears to produce wings on the pinch mass profile at stagnation that reduces the rate of compression of the pinch. The observation of precursor pinch formation, trailing mass, and trailing current indicates that all the mass and current do not assemble simultaneously on axis. Precursor and trailing implosions appear to impact the efficiency of the conversion of current (driver energy) to x rays. An instability with the character of an m = 0 sausage grows rapidly on axis at stagnation, during the rise time of pinch power. Just after peak power, a mild m = 1 kink instability of the pinch occurs which is correlated with the higher compression ratio of the pinch after peak power and the decrease of the power pulse. Understanding these three-dimensional, discrete-wire implosion characteristics is critical in order to efficiently scale wire arrays to higher currents and powers for fusion applications.

Movement disorders after status epilepticus and other brain injuries.

A retrospective medical record review was conducted of 173 consecutive children hospitalized for acquired brain injuries on a specialized pediatric rehabilitation service. The chart review identified children who developed movement disorders with acquired brain injuries: 8 with status epilepticus, 2 with trauma, and 1 with anoxia. Movement disorders were observed more frequently following status epilepticus (8 of 12) than following other causes of acquired brain injury (3 of 161; P = .0001). Four additional children had severe neurologic deficits following status epilepticus but did not develop movement disorders. The 11 patients who developed movement disorders had choreiform movements predominantly. Even though status epilepticus is a clinical phenomenon resulting from a variety of etiologies, the features of movement disorders in these children were strikingly similar. The pathophysiology of this complication is unknown.

Electron microscopy of human factor V and factor VIII: correlation of morphology with domain structure and localization of factor V activation fragments.

Clotting factor V and factor VIII are each represented by the domain structure A1-A2-B-A3-C1-C2 and share 40% sequence homology in the A and C domains. Rotary-shadowed samples of human factor V and factor VIII were examined in the electron microscope. Single-chain factor V molecules exhibited a globular "head" domain 12-14 nm in diameter. In addition, up to 25% of these molecules showed a rod-like "tail" of up to 50 nm. Glycerol-gradient centrifugation of factor V treated with thrombin partially resolved the factor Va heterodimer from a larger activation peptide of 150 kDa, as determined by gel electrophoresis. Electron microscopy of factor Va revealed globular molecules with several smaller appendicular structures but lacking the tails seen in factor V. Images of the 150-kDa activation peptide showed rod-like structures, similar in width to the tail of intact factor V and approximately 34 nm long. Rotary shadowing was also used to visualize factor VIII that had been fractionated into heterodimers containing heavy chains of distinct sizes. Each factor VIII preparation showed a globular structure approximately 14 nm in diameter, but the associated tails were observed much more frequently with factor VIII heterodimers containing the higher-molecular-weight heavy chains. These results, in conjunction with results of studies using other biophysical techniques, suggest a model in which the A and C domains of each cofactor constitute a globular head and the connecting B domain is contained in a two-stranded tail that is released by thrombin cleavage.

Substructure of human von Willebrand factor. Proteolysis by V8 and characterization of two functional domains.

The effects of Staphylococcus aureus V8 protease (V8) on the multimeric structure of human von Willebrand factor (vWF) were studied to test and expand our model for the substructure of vWF. Electron microscopy of V8 digests of vWF revealed that the multimers were cleaved where the flexible rod (R) domains join the large elongated globular (G) domains. The resulting two major fragments, which were purified by affinity and hydrophobic interaction chromatography and by glycerol-gradient ultracentrifugation, are disulfide-linked homodimers of these domains (i.e. RR and GG) and are morphologically identical to the alternating RR and GG domains of intact vWF. The glycoprotein fragment GG (6.5 X 35 nm) has mass 343 kDa by sedimentation equilibrium and the amino-terminal sequence of intact plasma vWF. It contains the binding site for heparin within 300 residues of its amino terminus and a separate site for the platelet GPIb receptor responsible for platelet agglutination in the presence of ristocetin. With approximately 18% alpha-helix and approximately 15% beta-pleated sheet, fragment GG accounts for most of the ordered secondary structure present in whole vWF. The two thin flexible rod domains (1.8-2.0 X 30-34 nm) of fragment RR are joined at a small central nodule (approximately 5 nm diameter) and also have a small nodule at each free end. Fragment RR contains an extraordinarily high cystine content, lower than average amounts of other hydrophobic residues, and essentially no alpha-helix, as judged by circular dichroism. The amino-terminal sequence and amino acid composition of fragment RR corresponded to that of the COOH-terminal 685 residues of the intact vWF subunit (Titani, K., Kumar, S., Takio, K., Ericsson, L. H., Wade, R. D., Ashida, K., Walsh, K. A., Chopek, M. W., Sadler, J. E., and Fujikawa, K. (1986) Biochemistry 25, 3171-3184). This sequence analysis gives a mass of 180 kDa for glycosylated fragment RR, somewhat higher than the 130 kDa we obtained by sedimentation equilibrium. Our sequence analysis of a 110-kDa plasmic vWF peptide also permitted identification of a major plasmin cleavage site 705 residues from the COOH terminus and a half-cystine residue (1360) involved in maintaining the multimeric structure of plasmin-degraded vWF.(ABSTRACT TRUNCATED AT 400 WORDS)

Substructure of human von Willebrand factor.

Using electron microscopy, we have visualized the substructure of human von Willebrand factor (vWf) purified by two different approaches. vWf multimers, which appear as flexible strands varying in length up to 2 micron, consist of dimeric units (protomers) polymerized linearly in an end-to-end fashion through disulfide bonds. Examination of small multimers (e.g., one-mers, two-mers, and three-mers) suggests that each protomer consists of two large globular end domains (22 X 6.5 nm) connected to a small central node (6.4 X 3.4 nm) by two flexible rod domains each approximately 34 nm long and approximately 2 nm in diameter. The protomer is 120 nm in length when fully extended. These same structural features are seen both in vWf molecules that were rapidly purified from fresh plasma by a new two-step procedure and in those purified from lyophilized intermediate-purity Factor VIII/vWf concentrates. The 240,000-mol wt subunit observed by gel electrophoresis upon complete reduction of vWf apparently contains both a rod domain and a globular domain and corresponds to one half of the protomer. Two subunits are disulfide-linked, probably near their carboxyl termini, to form the protomer; disulfide bonds in the amino-terminal globular ends link promoters to form vWf multimers. The vWf multimer strands have at least two morphologically distinct types of ends, which may result from proteolytic cleavage in the globular domains after formation of large linear polymers. In addition to releasing fragments that were similar in size and shape to the repeating protomeric unit, plasmic degradation of either preparation of vWf reduced the size of multimers, but had no detectable effect on the substructure of internal protomers.

Electron microscopy and image processing applied to the study of protein structure and protein-protein interactions.

We review the application of electron microscopy and image processing at the molecular level to an ever increasing range of biological specimens. Although recent advances have been due in part to development of more sophisticated instrumentation and/or processing algorithms, widespread application of the well-known techniques of image enhancement and structure reconstruction has depended on new strategies of in vitro crystallization and polymerization, some of which are outlined here. We also discuss the use of stoichiometric labeling and/or "cocrystallization" in identifying the different subunits in multisubunit complexes and in studying protein-protein interactions.

Tubular arrays of the actin-DNase I complex induced by gadolinium.

We describe the preparation and structural analysis of ordered tubular arrays of the actin-DNase I complex. These structures consist of helically stacked rings; each ring is 73 A thick, has a 240 A outer and a 120 A inner diameter, and has 7-fold rotational symmetry. The actin-DNase I complex forms tubes under conditions in which actin alone aggregates into crystalline sheets-i.e., in the presence of the trivalent cation gadolinium. Moreover, upon addition of an equimolar amount of DNase I, crystalline actin sheets are slowly converted to tubes. The rings making the tubes contain a radial dyad axis that may be identical to the dyad axis of the unit cell of the crystalline actin sheet. Evidence is presented for this identification, which in turn allows tentative assignment of actin- and DNase I-containing regions in three-dimensional reconstructions of the rings. The structural analysis presented here may be useful in aligning available three-dimensional molecular models of actin determined from crystals of the actin-DNase I complex and from crystalline actin sheets with each other and ultimately within the biologically important actin filament.

Towards an alignment of the actin molecule within the actin filament.

Electron micrographs of negatively stained actin filament paracrystals and single-layered filament rafts showing different interfilament spacings have been studied and three-dimensional reconstructions have been computed from them. Lateral ordering of the filaments in rafts was lost when interfilament spacings exceeded 8.5 nm, suggesting this distance as an upper limit for the filament diameter. Further, all reconstructions showed the same structural features at the 3 nm resolution level, except that the filaments from ordered single-layered rafts appeared 10-20% wider than those from multi-layered paracrystals. A comparison between electron microscopical and X-ray filament data, and synthetic filaments generated using different tentative molecular models and/or orientations for actin did not allow a single best model to be selected.

The fibrillar substructure of keratin filaments unraveled.

We show that intermediate-sized filaments reconstituted from human epidermal keratins appear unraveled in the presence of phosphate ions. In such unraveling filaments, up to four "4.5-nm protofibrils" can be distinguished, which are helically twisted around each other in a right-handed sense. Lowering the pH of phosphate-containing preparations causes the unraveling filaments to further dissociate into "2-nm protofilaments." In addition, we find that reconstitution of keratin extracts in the presence of small amounts of trypsin yields paracrystalline arrays of 4.5-nm protofibrils with a prominent 5.4-nm axial repeat. Limited proteolysis of intact filaments immobilized on an electron microscope grid also unveils the presence of 4.5-nm protofibrils within the filament with the same 5.4-nm axial repeat. These results, together with other published data, are consistent with a 10-nm filament model based on three distinct levels of helical organization: (a) the 2-nm protofilament, consisting of multi-chain extended alpha-helical segments coiled around each other; (b) the 4.5-nm protofibril, being a multi-stranded helix of protofilaments; and (c) the 10-nm filament, being a four-stranded helix of protofibrils.

Structure of the actin molecule determined from electron micrographs of crystalline actin sheets with a tentative alignment of the molecule in the actin filament.

Electron microscopy and image processing of negatively stained crystalline sheets induced from Acanthamoeba actin have been used to yield a three-dimensional reconstruction of the actin molecule, including data to a maximum resolution of 15 A. This model shows actin to be an asymmetric, wedge-shaped molecule. A three-dimensional reconstruction of an averaged, polar actin filament from negatively stained polylysine-induced actin filament paracrystals has also been computed. We show two possible ways in which the wedge-shaped actin molecule from the sheets can be placed into such a filament reconstruction. In both, the major intermolecular contacts are formed on complementary surfaces of the actin subunit and follow the left-handed genetic helix of the filament, a feature also found in the filament reconstruction.

A consistent picture of the actin filament related to the orientation of the actin molecule.

We show that freeze-dried actin filaments which have been rotary shadowed with a light coat of platinum appear very similar in morphology and width to negatively-stained filaments. The addition of a thicker coat of platinum to such preparations gives the actin filaments a different morphology and width, which are similar to those of the rotary-shadowed, quick-frozen filaments described by Heuser and Kirschner (J. Cell Biol. 1980, 86:212-234). The consistent view of the actin filament presented here, particularly its 7-8-nm width, can be interpreted in terms of the overall orientation of the actin subunit in the actin filament.

Preparation of single molecules and supramolecular complexes for high-resolution metal shadowing.

We have compared the appearance and preservation of molecular and supramolecular structures in preparations that were dried in vacuo at room temperature or freeze-dried. Fibrinogen and brain spectrin molecules appear similar in both types of preparation provided that drying at room temperature is performed in the presence of glycerol, which results in an even and reproducible distribution of such molecules (Shotton et al., 1979, J. Mol. Biol. 131, 303-329; Fowler and Erickson, 1979, J. Mol. Biol. 134, 241-249). In the case of crystalline actin sheets, actin filaments, and keratin filaments, freeze-drying preserves structural details that are often completely lost during drying at room temperature, whether or not glycerol is used. On the other hand, keratin filaments prepared by drying in the presence of glycerol display a beaded axial repeat that is probably due to "glycerol decoration." We conclude that although freeze-drying has no clear advantage over glycerol spraying/vacuum-drying in the case of single extended molecules, it may provide insight into the multiple effects of glycerol in specimen preparation. In the case of supramolecular assemblies such as filaments or crystalline sheets, freeze-drying preserves significantly more substructure and surface detail. The loss of such detail during drying at room temperature, probably through collapse phenomena such as distortion and flattening, cannot be prevented by glycerol.

Actin and myosin function in acanthamoeba.

We have studied the functions of contractile proteins in Acanthamoeba by a combination of structural, biochemical and physiological approaches. We used electron microscopy and image processing to determine the three-dimensional structure of actin and the orientation of the molecule in the actin filament. We measured the rate constants for actin filament elongation and re-evaluated the effect of MgCl2 on the filament nucleation process. In Acanthamoeba actin polymerization is regulated, at least in part, by profilin, which binds to actin monomers, and by capping protein, which both nucleates polymerization and blocks monomer addition at the 'barbed' end of the filament. To test for physiological functions of myosin-II, we produced a monoclonal antibody that inhibits the actin-activated ATPase. When microinjected into living cells, this active-site-specific antibody inhibits amoeboid locomotion. We expect that similar experiments can be used to test for the physiological functions of the other components of the Acanthamoeba contractile system.

Brain spectrin, a membrane-associated protein related in structure and function to erythrocyte spectrin.

An immunoreactive analogue of erythrocyte spectrin has been purified from brain membranes. This protein co-sediments with and cross-links actin filaments, associates with spectrin-binding sites on erythrocyte membranes, and has been visualized by rotary shadowing as an extended, flexible rod. The brain spectrin comprises 3% of the total membrane protein, and may have a major role in mediating linkage of actin to membranes.

Polymorphism of actin paracrystals induced by polylysine.

We describe a method for the induction of different polymorphic forms of actin filament paracrystals. This polymorphism is probably based on differences in the stagger and/or polarity of adjacent filaments in single-layered paracrystals and by superposition of different layers in multilayered paracrystals. The helical parameters defining the filament geometry are indistinguishable for the different polymorphic forms observed and for the four different actins used. Analysis of these paracrystals, some of which are ordered to better than 2.5 nm, should provide a reference structure suitable for alignment and orientation within the actin filament of high resolution models of the actin monomer obtained from crystal data.