Investigation of the morphology of intermediate filaments adsorbed to different solid supports.

Morphologically, glutaraldehyde-fixed and -dried intermediate filaments (IFs) appear flexible, and with a width of 8-12 nm when observed by electron microscopy. Sometimes, the filaments are even unraveled on the carbon-coated grid and reveal a protofilamentous architecture. In this study, we have used atomic force microscopy to further investigate the morphology of IFs in a more physiological environment. First, we have imaged hydrated glutaraldehyde-fixed IFs adsorbed to a graphite support. In such conditions, human vimentin and desmin IFs appeared compact with a height of 5-8 nm and revealed either a beading repeat or a helical morphology. Second, we have analyzed the architecture of hydrated vimentin, desmin, and neurofilament IFs adsorbed to mica, graphite, and hydrophilic glass without the presence of fixative. On mica, vimentin IFs had a height of only 3-5 nm, whereas desmin IFs appeared as 8-10 nm height filaments with a helical twist. Neurofilaments were 10-12 nm in height with a pronounced 30-50 nm beading along their length. On graphite, the different IFs were either not adsorbing properly or their architecture was modified yielding, for example, broad, flattened filaments. Finally, hydrophilic glass was the surface which seemed to best preserve the architecture of the three IFs, even if, in some cases, unraveled vimentin filaments were observed on this support. These results are straightening the idea that mature IFs are dynamic polymers in vitro and that IFs can be distinguished from each others by their physicochemical properties.

Assessing the flexibility of intermediate filaments by atomic force microscopy.

Eukaryotic cells contain three cytoskeletal filament systems that exhibit very distinct assembly properties, supramolecular architectures, dynamic behaviour and mechanical properties. Microtubules and microfilaments are relatively stiff polar structures whose assembly is modulated by the state of hydrolysis of the bound nucleotide. In contrast, intermediate filaments (IFs) are more flexible apolar structures assembled from a approximately 45 nm long coiled-coil dimer as the elementary building block. The differences in flexibility that exist among the three filament systems have been described qualitatively by comparing electron micrographs of negatively stained dehydrated filaments and by directly measuring the persistence length of F-actin filaments (approximately 3-10 microm) and microtubules (approximately 1-8 mm) by various physical methods. However, quantitative data on the persistence length of IFs are still missing. Toward this goal, we have carried out atomic force microscopy (AFM) in physiological buffer to characterise the morphology of individual vimentin IFs adsorbed to different solid supports. In addition, we compared these images with those obtained by transmission electron microscopy (TEM) of negatively stained dehydrated filaments. For each support, we could accurately measure the apparent persistence length of the filaments, yielding values ranging between 0.3 microm and 1 microm. Making simple assumptions concerning the adsorption mechanism, we could estimate the persistence length of an IF in a dilute solution to be approximately 1 microm, indicating that the lower measured values reflect constraints induced by the adsorption process of the filaments on the corresponding support. Based on our knowledge of the structural organisation and mechanical properties of IFs, we reason that the lower persistence length of IFs compared to that of F-actin filaments is caused by the presence of flexible linker regions within the coiled-coil dimer and by postulating the occurrence of axial slipping between dimers within IFs.

Physical characterization of plakophilin 1 reconstituted with and without zinc.

Plakophilin 1 (PKP1) belongs to the arm-repeat protein family which is characterized by the presence of a conserved 42-amino-acid motif. Despite individual members of the family containing a similar type of structural domain, they exhibit diverse cellular functions. PKP1 is ubiquitously expressed in human tissues and, depending on the type of cell, found prominently in the karyoplasm and/or in desmosomes. In surface plasmon resonance detection experiments, we noticed that PKP1 specifically bound zinc but not calcium or magnesium. Therefore we have used circular dichroism spectroscopy, limited proteolysis, analytical ultracentrifugation, electron microscopy and dynamic light scattering to establish the physical properties of recombinant PKP1 depending on the presence or absence of zinc. The alpha helix content of PKP1 was considerably higher when reconstituted with zinc than without. By atomic absorption spectroscopy 7.3 atoms zinc were shown to be tightly associated with one molecule of wild-type PKP1. The zinc-reconstituted protein formed globular particles of 21.9 +/- 8.4 nm diameter, as measured by electron microscopy after glycerol spraying/rotary metal shadowing. In parallel, the average sedimentation coefficient (s20, w) for zinc-containing PKP1 was 41S and its diffusion coefficient, as obtained by dynamic light scattering, 1.48 x 10-7 cm2.s-1. The molecular mass of 2.44 x 106 obtained from s and D yields an average stoichiometry of 30 for the PKP1 oligomer. In contrast, PKP1, reconstituted without zinc, contained no significant amount of zinc, sedimented with 4.6S, and was present in monomeric form as determined by sedimentation equilibrium centrifugation.

Scanning force microscopy of Escherichia coli RNA polymerase.sigma54 holoenzyme complexes with DNA in buffer and in air.

Scanning force microscopy (SFM) was used to visualize complexes of Escherichia coli RNA polymerase.sigma54 (RNAP.sigma54) and a 1036 base-pair linear DNA fragment containing the glnA promoter. In order to preserve the native hydration state of the protein-DNA complexes, the samples were injected directly into the SFM fluid cell and imaged in buffer. With this protocol, an apparent bending angle of 26(+/-34) degrees was determined for the specific complexes at the promoter. The bending angle of the unspecifically bound RNAP.sigma54 showed a somewhat broader distribution of 49(+/-48) degrees, indicating the existence of conformational differences as compared to the closed complex. In about two-thirds of the closed complexes, the RNA polymerase holoenzyme was located in a lateral position with respect to the DNA and the bend of the DNA was pointing away from the protein. This conformation was consistent with the finding that for the complexes at the promoter, the apparent contour length was reduced by only about 6 nm in buffer as compared to the free DNA. From these results we conclude that in the closed complex of RNAP. sigma54, the DNA was not wrapped around the polymerase, and we present a model for the trajectory of the DNA with respect to the RNA polymerase. The images acquired in buffer were compared to samples that were washed with water and then dried before imaging. Two artefacts of the washing and drying process were detected. First, extensive washing of the sample reduced the number of the specific complexes bound at the promoter (closed complex of RNAP.sigma54) from about 70% to 30%. This is likely to be a result of sliding of the RNAP.sigma54 holoenzyme along the DNA induced by the washing process. Second, the apparent DNA shortening of the contour length of RNAP.sigma54-DNA complexes at the promoter as compared to the contour length of the free DNA was 22 nm for the dried samples as opposed to only 6 nm for the undried samples imaged in buffer. This suggests an artefact of the drying process.

Association states of the transcription activator protein NtrC from E. coli determined by analytical ultracentrifugation.

The transcription activator protein NtrC (nitrogen regulatory protein C) can catalyze the transition of E. coli RNA polymerase complexed with the sigma54 factor (RNAP.sigma54) from the closed complex (RNAP.sigma54 bound at the promoter) to the open complex (melting of the promoter DNA). This process involves phosphorylation of NtrC, assembly of a multimeric NtrC complex at the enhancer DNA sequence, interaction of this complex with promoter bound RNAP. sigma54 via DNA looping, and hydrolysis of ATP. We have used analytical ultracentrifugation to study the different NtrC association states and to derive hydrodynamic models for the conformation of the various NtrC species. The following results were obtained. (i) The unphosphorylated wild-type protein formed a dimer with a measured molecular weight of 102(+/-3) kDa, which compares to a calculated molecular weight of 54 kDa for a monomer (concentration range studied 2 to 8 microM NtrC monomer). (ii) In the unphosphorylated state one NtrC dimer was bound to one binding site as determined with DNA oligonucleotide duplexes containing one or two binding sites (concentration range studied 50 to 1000 nM NtrC dimer). (iii) The data obtained at protein concentrations that were below the concentration of binding sites indicate that binding to the DNA duplex with two binding sites occurred with essentially no cooperativity. The experiments were conducted in the absence of ATP. (iv) The phosphorylated protein formed a specific complex at the DNA duplex with the enhancer sequence (two NtrC binding sites) that consisted of four dimers (concentration range studied 100 to 1000 nM NtrC dimer). (v) The formation of this octameric complex was highly cooperative, and the data suggest that two DNA strands could bind simultaneously to this complex. (vi) From the sedimentation data a model was derived in which the NtrC dimer adopts a V shaped structure with the DNA binding domains being located at the bottom and the two receiver domains at the top of the V. In this conformation higher order NtrC complexes can be stabilized by interaction between the phosphorylated receiver domain and the central activation domain of different NtrC dimers.

Superhelix dimensions of a 1868 base pair plasmid determined by scanning force microscopy in air and in aqueous solution.

We have used scanning force microscopy (SFM) to study the conformation of a 1868 base pair plasmid (p1868) in its open circular form and at a superhelical density of sigma= -0.034. The samples were deposited on a mica surface in the presence of MgCl2. DNA images were obtained both in air and in aqueous solutions, and the dimensions of the DNA superhelix were analysed. Evaluation of the whole plasmid yielded average superhelix dimensions of 27 +/- 9 nm (outer superhelix diameter D), 107 +/- 51 nm (superhelix pitch P), and 54 +/-8 degrees (superhelix pitch angle alpha). We also analysed compact superhelical regions within the plasmid separately, and determined values of D = 9.2 +/- 3.3 nm, P = 42 +/- 13 nm and alpha= 63 +/- 20 degrees for samples scanned in air or rehydrated in water. These results indicate relatively large conformation changes between superhelical and more open regions of the plasmid. In addition to the analysis of the DNA superhelix dimensions, we have followed the deposition process of open circular p1868 to mica in real time. These experiments show that it is possible to image DNA samples by SFM without prior drying, and that the surface bound DNA molecules retain some ability to change their position on the surface.