Biomedical subjects
J Dubochet
Publications and source records attributed to J Dubochet.
Interactions between actin and myosin filaments in skeletal muscle visualized in frozen-hydrated thin sections.
For the purpose of determining net interactions between actin and myosin filaments in muscle cells, perhaps the single most informative view of the myofilament lattice is its averaged axial projection. We have studied frozen-hydrated transverse thin sections with the goal of obtaining axial projections that are not subject to the limitations of conventional thin sectioning (suspect preservation of native structure) or of equatorial x-ray diffraction analysis (lack of experimental phases). In principle, good preservation of native structure may be achieved with fast freezing, followed by low-dose electron imaging of unstained vitrified cryosections. In practice, however, cryosections undergo large-scale distortions, including irreversible compression; furthermore, phase contrast imaging results in a nonlinear relationship between the projected density of the specimen and the optical density of the micrograph. To overcome these limitations, we have devised methods of image restoration and generalized correlation averaging, and applied them to cryosections of rabbit psoas fibers in both the relaxed and rigor states. Thus visualized, myosin filaments appear thicker than actin filaments by a much smaller margin than in conventional thin sections, and particularly so for rigor muscle. This may result from a significant fraction of the myosin S1-cross-bridges averaging out in projection and thus contributing only to the baseline of projected density. Entering rigor incurs a loss of density from an annulus around the myosin filament, with a compensating accumulation of density around the actin filament. This redistribution of mass represents attachment of the fraction of cross-bridges that are visible above background. Myosin filaments in the "nonoverlap" zone appear to broaden on entering rigor, suggesting that on deprivation of ATP, cross-bridges in situ move outwards even without actin in their immediate proximity.
Head structure of bacteriophages T2 and T4.
The length-to-width ratios of bacteriophage T2 and T4 heads and stereometric angles specifying the prolate icosahedral T2 capsid were evaluated on electron micrographs recorded from samples prepared by a variety of methods. The copy numbers of the major capsid protein, gp23*, of T2 and T4 phages were compared by quantitative gel electrophoresis. Taken together, the resulting values are most compatible with triangulation numbers T = 13 and Q = 21 for both T2 and T4, thus confirming the previously proposed capsid architecture of T4 revealed by indirect measurements and thereby eliminating the repeatedly reported discrepancy between T2 and T4 in favor of a common Q number of 21 corresponding to 960 copies of gp23*.
Cryo-electron microscopy of vitrified specimens.
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Length and shape variants of the bacteriophage T4 head: mutations in the scaffolding core genes 68 and 22.
The shape and size of the bacteriophage T4 head are dependent on genes that determine the scaffolding core and the shell of the prohead. Mutants of the shell proteins affect mainly the head length. Two recently identified genes (genes 67 and 68) and one already known gene (gene 22), whose products are scaffold constituents, have been investigated. Different types of mutants were shown to strongly influence the proportion of aberrantly shaped particles. By model building, these shape variants could be represented as polyhedral bodies derived from icosahedra, through outgrowths along different polyhedral axes. The normal, prolate particle is obtained by elongation along a fivefold axis. The mutations of the three core genes (genes 67, 68, and 22) affect the width mainly by lateral outgrowths of the prolate particle, although small and large isometric particles are also found. Many of the aberrant particles are multitailed, suggesting a correlation between tail attachment sites and shape.
Organization of double-stranded DNA in bacteriophages: a study by cryo-electron microscopy of vitrified samples.
In this paper it is shown that conformation and packing of double-stranded DNA within the head of bacteriophages lambda and T4 can be assessed by cryo-electron microscopy of vitrified specimens. Electron diffraction patterns show that DNA within vitrified bacteriophages has a B conformation. Electron micrographs of vitrified bacteriophages show domains within the head formed by a approximately 2.5-nm striation and arising from the DNA packing. The number of differently oriented domains seen within a vitrified bacteriophage depends upon the geometry of the DNA container: the bacteriophage capsid. The packing of DNA within bacteriophages seems then to be governed by at least two phenomena. The first is the tendency of DNA to form local alignments (nematic liquid crystals). The second is the orientation of these liquid crystals by the bacteriophage capsid. From these observations we propose a possible packaging mechanism: constrained nematic crystallization.
Cryo-electron microscopy of vitrified SV40 minichromosomes: the liquid drop model.
The structure of SV40 minichromosomes has been studied by cryo-electron microscopy of vitrified thin layers of solution. In high-salt buffer (130 mM NaCl), freshly prepared minichromosomes are condensed into globules 30 nm or more in diameter. On the micrograph, they appear to be formed by the close packing of 10 nm granules which give rise to a 10 nm reflection in the optical diffractogram. The globules can adopt many different conformations. At high concentration, they fuse into a homogeneous 'sea' of closely packed 10 nm granules. In low-salt buffer (less than 10 mM NaCl), the globules open, first into 10 nm filaments, and then into nucleosome-strings. The 'liquid drop' model is proposed to explain the condensed structure of the minichromosome in high-salt buffer: nucleosomes stack specifically on top of one another, thus forming the 10 nm filaments. 10 nm filaments in turn, tend to aggregate laterally. Optimizing both these interactions results in the condensation of 10 nm filaments or portions thereof into a structure similar to that of a liquid. Some implications of this model for the structure of cellular chromatin are discussed.
Cryo-electron microscopy of vitrified chromosomes in situ.
Chromosomes of metaphase-arrested Chinese hamster ovary (CHO) and HeLa cells were examined in situ, unfixed and unstained, by cryo-electron microscopy. In hydrated, vitrified cryo-sections, chromosomes exhibit a characteristic homogeneous, grainy texture, which, on optical diffraction, gives rise to a broad reflection corresponding to 11 nm. No superstructure or periodic order is discernible. These observations suggest that the chromosome is formed by the compact association of 11 nm filaments, or portions thereof, interacting in a manner akin to the molecules of a liquid. Some implications of the liquid model of chromosome structure are discussed.
Electron microscopy of frozen hydrated specimens: preparation and characteristics.
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Cryo-electron microscopy of vitrified insect flight muscle.
Frozen hydrated sections of vitrified unstained insect flight muscle in the rigor and relaxed states were studied by cryo-electron microscopy. High resolution images with good contrast were obtained. As judged from direct images and from the comparison of optical diffractograms with X-ray diffraction patterns obtained from glycerinated muscle fibres, the vitrified specimen is well preserved. Preparation artifacts encountered in conventional plastic sections are avoided. The preservation of the relaxed structure also seems better than in freeze-etched replicas as the 14.5 nm repeat of crossbridges on thick filaments is easily visible.
On the preparation of cryosections for immunocytochemistry.
The key preparation steps in the Tokuyasu thawed frozen section technique for immunocytochemistry, namely freezing, sectioning, thawing, and drying, were studied. A spherical tissue culture cell was used as a model system. The frozen hydrated section technique indicated that glutaraldehyde-fixed, 2.1 M sucrose-infused pellets of cells were routinely vitrified by immersion in liquid nitrogen but water was crystallized when lower sucrose concentrations (0.6-1 M) were used. Quantitative mass measurements showed that the fixed cells are freely permeable to sucrose. The frozen hydrated sections were severely compressed but cell profiles regained their circular appearance upon thawing. The average section thickness of our frozen-hydrated sections was 110 nm: this was reduced to 30-50 nm upon thawing, washing, and air-drying. This change was accompanied by severe drying artifacts. By using the methyl cellulose drying technique, this collapse upon air-drying could be significantly reduced, but not completely prevented, giving an average thickness of 70 nm.
Electron microscopy of frozen biological suspensions.
The methodology for preparing specimens in the frozen, hydrated state has been assessed using crystals and T4 bacteriophages. The methods have also been demonstrated with lambda bacteriophages, purple membrane of Halobacterium halobium and fibres of DNA. For particles dispersed in an aqueous environment, it is shown that optimum structural preservation is obtained from a thin, quench-frozen film with the bulk aqueous medium in the vitreous state. Crystallization of the bulk water may result in solute segregation and expulsion of the specimen from the film. Contrast measurements can be used to follow directly the state of hydration of a specimen during transition from the fully hydrated to the freeze-dried state and permit direct measurement of the water content of the specimen. By changing the concentration and composition of the aqueous medium the contrast of particles in a vitreous film can be controlled and any state of negative, positive or zero contrast may be obtained. At 100 K, frozen-hydrated, freeze-dried or sugar embedded crystals can withstand a three- to four-fold increase in electron exposure for the same damage when compared with similar sugar-embedded or freeze-dried samples at room temperature.
Electron microscopy of frozen hydrated sections of vitreous ice and vitrified biological samples.
The preparation and high resolution observation of frozen hydrated thin sections has been studied by transmission electron microscopy (TEM and STEM) on model systems, including pure water, protein solutions, catalase crystals, myelin sheath and various tissues. The state of the ice is determined by electron diffraction. Mass measurement in the electron microscope is used to determine section thickness and control hydration. An adequate depth of vitrified material for sectioning can be obtained from many biological suspensions or untreated tissues. Frozen hydrated sections around 100 nm thick can be produced under optimal conditions from vitreous ice or from vitrified biological samples. Sectioning, transfer and observation in the electron microscope is feasible without alteration of the sample hydration or its initial vitrification. Biological structures can be preserved and observed down to 10 nm. Under favourable working conditions, specimen compression during sectioning and electron beam damage are the factors limiting high resolution observations.
Electron microscopy of frozen-hydrated bacteria.
Amorphous, unstained, frozen-hydrated sections of bacteria provide a faithful high-resolution image of procaryotic cells. Conventional preparation artifacts due to fixation, staining, and dehydration are nonexistent. Freezing damage is avoided by using glucose as a cryoprotectant. Cutting damage on frozen material is severe, but sectioning artifacts, being always related to the cutting direction, can be systematically recognized and thus taken into consideration. Geometry and density distribution of the bacterial envelope can be resolved to about 3 nm. The following main features have been observed. In Escherichia coli the inner and outer membranes have an approximately uniform density profile. The distance between the two membranes is constant, ca. 33 nm. In Staphylococcus aureus the cell wall is ca. 40 nm wide. It is bordered on the cytoplasmic side by an asymmetric 5.5-nm-wide bilayer. The bacterial nucleoid, clearly visible with conventional preparation methods, appears in exponentially growing bacteria as an ill-defined central region with approximately the same density as the rest of the cytoplasm. It becomes more clearly visible when bacteria are in the stationary phase, plasmolysed, fixed, or stained. We confirm that "mesosomes," hitherto quite often considered to be essential organelles in all procaryotes, are artifacts. They appear in large numbers during osmium fixation.
Electron microscope observation of a fibre structure formed by non-specific binding of cAMP receptor protein to DNA.
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Low temperature electron microscopy.
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Beam damage to organic material is considerably reduced in cryo-electron microscopy.
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Self-assembly of single and closely spaced nucleosome core particles.
Self-assembly of DNA with the four core histones but in the absence of H1 generates nucleosome core particles which are spaced randomly over large distances. Closely spaced core particles, however, exhibit a preferred short linkage which is not a multiple of 10 base pairs. They bind about 140 base pairs whereas apparently shorter DNA lengths per nucleosome observed after digestion with micrococcal nuclease are the result of degradation from the ends. The DNA length of one superhelical turn in the core particle is 83 +/- 4 base pairs. Single core particles may bind more DNA than closely spaced core particles but probably less than two full turns of 168 base pairs. The internal structures of single and of native core particles are very similar as judged by their amount of DNA, sedimentation coefficient, appearance in the electron microscope, and digestion with DNase I. In addition to core particles, a particle is described which sediments at 9 S and consists of 108 base pairs of DNA bound to the histone octamer. It appears to be the smallest stable "core particle" but it is not a degradation product of the 146-base-pair core particle. Digestion of end-labeled 9 S and nucleosome core particles with DNase I shows distinct differences.