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Biomedical subjects

J Langowski

Publications and source records attributed to J Langowski.

At least 19 recordsLinked to original sources

DNA damaging capability of hematoporphyrin towards DNAs of various accessibilities.

In this work we wanted to verify that photoactivation of DNA-non-binding porphyrin derivative hematoporphyrin IX (Hp) is able to induce damages in DNAs of various accessibilities such as B-conformation and superhelical isolated DNA, nucleoprotein complex and intracellular DNAs. It was found that photodynamic reaction of Hp results significant changes in thermal stability of isolated T7 DNA and induces single strand breaks in supercoiled Bluescript plasmid isolated from Escherichia coli cells. As optical melting measurements revealed, the irradiation of photosensitized T7 nucleoprotein complex leads to a destabilization of the protein capsid. The photodynamic reaction affected both the protein structure and DNA-protein interaction, however, the parameters corresponding to the DNA denaturation are not influenced. The accumulation of Hp in HeLa cells was followed by laser scanning confocal microscopy. The picture received is typical for lipophilic dyes. When Hp loaded cells were irradiated, a reduction of viability could be observed in a concentration and a light dose dependent manner; 12microM porphyrin induced almost complete cell killing after 30min irradiation. After similar treatment, alkaline agarose gel electrophoresis of isolated nuclear DNA did not show the presence of single strand breaks. The alkaline comet assay also failed to demonstrate any DNA damage in HeLa cells. We also considered the possibility of the generation of damages in intracellular SV40 DNA. According to the electropherograms there was no difference between the patterns of DNAs from treated and control samples.

DNA↗

Polymer chain models of DNA and chromatin.

Many properties of the genome in the cell nucleus can be understood by modeling DNA and chromatin as a flexible polymer chain. This article introduces into current models for such a coarse-grained description and reviews some recent results from our own group. Examples given are the unrolling of DNA from the histone core and the response of the 30 nm chromatin fiber to mechanical stretching.

Cell Nucleus↗

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.

Actin Cytoskeleton↗

Characterization of simian virus 40 on its infectious entry pathway in cells using fluorescence correlation spectroscopy.

SV40 (simian virus 40) is a double-stranded DNA virus and is strongly oncogenic in experimental animals. SV40 enters cells by atypical endocytosis mediated by caveolae, transporting the virus to its usual destination, namely the endoplasmic reticulum. The cellular mechanisms of capsid disassembly (uncoating) and deliverance of the viral genome into the cellular nucleus remain unknown. Here, we study (i) the formation of caveolae after viral infection and the diffusion of caveosome vesicles in the cytoplasm and (ii) the capsid disassembly and the mobility of the viral genome on its way to the nucleus, using fluorescence correlation spectroscopy. To follow the viral genome and capsids separately, the histone components of SV40 minichromosomes were labelled with enhanced yellow fluorescent protein and the capsid was labelled with a fluorescent red dye, Alexa568. We characterized the diffusion of caveosomes, the capsid disassembly process in the cytoplasm and the mobility of the viral genome in the nucleus, using two kinds of permissive cells.

Animals↗

Detection of NGF-receptors TrkA and p75NTR in human tumor cell lines and effect of NGF on the growth characteristic of the UT-7/EPO cell line.

The receptors for nerve growth factor (NGF)--TrkA and p75NTR--were detected at the mRNA and the protein level in various human tumor cell lines. The NGF receptor TrkA was found on all examined tumor cell lines and is not restricted to cells belonging to the nervous system. NGF did not influence the proliferation rate of TrkA-positive cells NMB, K562, UT-7/EPO and PC-12. After NGF induction, the production level of the differentiation marker c-fos was increased in UT-7/EPO and PC- 12 cells. NGF-treatment of the UT-7/EPO cells and deprivation of erythropoietin (EPO) led to the new adherent cell line UT-7/NGF. Although UT-7/NGF showed a similar growth curve as UT-7/EPO, there were differences in the pattern of adhesion molecules and of the cytoskeleton. The effect of NGF on the cytoskeleton could not be induced in other human cell lines like NMB or KTCTL-30. TrkA inhibition with K252a--a blocker of Trk-induced receptor kinase--suggests, that the NGF signal may be transduced by the TrkA receptor in UT-7/NGF cells. This indicates that NGF is a decisive mediator of cellular adhesion.

Blotting, Western↗

Trajectory of nucleosomal linker DNA studied by fluorescence resonance energy transfer.

While the structure of the nucleosome core is known in atomic detail, the precise geometry of the DNA beyond the core particle is still unknown. We have used fluorescence resonance energy transfer (FRET) for determining the end-to-end distance of DNA fragments assembled with histones into nucleosomes. The DNA of a length of 150-220 bp was labeled with rhodamine-X on one end and fluorescein or Alexa 488 on the other. Assembling nucleosomes on these DNA fragments leads to a measurable energy transfer. The end-to-end distance computed from the FRET increases from 60 +/- 5 A at 150 bp to 75 +/- 5 A at 170 bp without measurable change above it. These distances are compatible with different geometries of the linker DNA, all having in common that no crossing can be observed up to 220 bp. Addition of H1 histone leads to an increase in energy transfer, indicating a compaction of the linker DNA toward the nucleosome.

Animals↗

Rotational dynamics of curved DNA fragments studied by fluorescence polarization anisotropy.

The rotational dynamics of short DNA fragments with or without intrinsic curvature were studied using time-resolved phase fluorimetry of intercalated ethidium with detection of the anisotropy. Parameters determined were the spinning diffusion coefficient of the DNA fragments about the long axis and the zero-time ethidium fluorescence anisotropy. We find a significant decrease in the spinning diffusion coefficient for all curved fragments compared to the straight controls. This decrease is likewise evident in rotational diffusion coefficients computed from DNA structures obtained by a curvature prediction program for these sequences. Using a hinged-cylinder model, we can identify the change in rotational diffusion coefficient with a permanent bend of 13-16 degrees per helix turn for the sequences studied. Moreover, for some of the curved fragments an increased flexibility has to be assumed in addition to the permanent bend in order to explain the data.

Algorithms↗

Intrachain reactions of supercoiled DNA simulated by Brownian dynamics.

We considered an irreversible biochemical intrachain reaction of supercoiled DNA as a random event that occurs, with certain probability, at the instant of collision between two reactive groups bound to distant DNA sites. Using the Brownian dynamics technique, we modeled this process for a supercoiled DNA molecule of 2.5 kb length in dilute aqueous solution at an NaCl concentration of 0.1 M. We calculated the mean reaction time tau(Sigma) as a function of the intrinsic second-order rate constant k(I), the reaction radius R, and the contour separation S of the reactive groups. At the diffusion-controlled limit (k(I) --> infinity), the kinetics of reaction are determined by the mean time tau(F) of the first collision. The dependence of tau(F) on R is close to inversely proportional, implying that the main contribution to the productive collisions is made by bending of the superhelix axis. At sufficiently small k(I), the mean reaction time can be satisfactory approximated by tau(Sigma) = tau(F)(app) + 1/(k(I)c(L)), where c(L) is the local concentration of one reactive group around the other, and tau is an adjustable parameter, which we called the apparent time of the first collision. The value of tau depends on R very weakly and is approximately equal to the mean time of the first collision caused by mutual reptation of two DNA strands forming the superhelix. The quasi-one-dimensional reptation process provides the majority of productive collisions at small k(I) values.

Algorithms↗

Diffusion-controlled intrachain reactions of supercoiled DNA: Brownian Dynamics simulations.

The Brownian Dynamics technique was used to model a diffusion-controlled intramolecular reaction of supercoiled DNA (2500 basepairs) in 0.1 M sodium chloride solution. The distance between the reactive groups along the DNA contour was 470 basepairs. The reaction radius was varied from 6 to 20 nm. The results are presented in terms of the probability distribution P(F)(t) of the first collision time. The general form of the function P(F)(t) could be correctly predicted by a simple analytical model of one-dimensional diffusion of the superhelix ends along the DNA contour. The distribution P(F)(t) is essentially non-exponential: within a large initial time interval, it scales as P(F)(t) approximately t(-1/2), which is typical for one-dimensional diffusion. However, the mean time of the first collision is inversely proportional to the reaction radius, as in three dimensions. A visual inspection of the simulated conformations showed that a considerable part of the collisions is caused by the bending of the superhelix axis in the regions of the end loops, where the axis is most flexible. This fact explains why the distribution P(F)(t) combines the features of one- and three-dimensional diffusion. The simulations were repeated for a DNA chain with a permanent bend of 100 degrees in the middle position between the reactive groups along the DNA contour. The permanent bend changes dramatically the form of the distribution P(F)(t) and reduces the mean time of the first collision by approximately one order of magnitude.

Biophysical Phenomena↗

Computation of writhe in modeling of supercoiled DNA.

We describe four previously unpublished methods allowing the computation of the writhe for a supercoiled DNA molecule modeled by a polymer chain consisting of straight segments. These methods are compared with each other in terms of computational efficiency and the scope of their applicability is discussed.

Biomechanical Phenomena↗

The effect of the DNA conformation on the rate of NtrC activated transcription of Escherichia coli RNA polymerase.sigma(54) holoenzyme.

The transcription activator protein NtrC (nitrogen regulatory protein C) can catalyze the transition of Escherichia coli RNA polymerase complexed with the sigma 54 factor (RNAP.sigma(54)) from the closed complex (RNAP.sigma(54) bound at the promoter) to the open complex (melting of the promoter DNA). This process involves phosphorylation of NtrC (NtrC-P), assembly of an octameric NtrC-P complex at the enhancer sequence, interaction of this complex with promoter-bound RNAP.sigma(54) via DNA looping, and hydrolysis of ATP. We have used this system to study the influence of the DNA conformation on the transcription activation rate in single-round transcription experiments with superhelical plasmids as well as linearized templates. Most of the templates had an intrinsically curved DNA sequence between the enhancer and the promoter and differed with respect to the location of the curvature and the distance between the two DNA sites. The following results were obtained: (i) a ten- to 60-fold higher activation rate was observed with the superhelical templates as compared to the linearized conformation; (ii) the presence of an intrinsically curved DNA sequence increased the activation rate of linear templates about five times; (iii) no systematic effect for the presence and/or location of the inserted curved sequence was observed for the superhelical templates. However, the transcription activation rate varied up to a factor of 10 between some of the constructs. (iv) Differences in the distance between enhancer and promoter had little effect for the superhelical templates studied. The results were compared with theoretical calculations for the dependence of the contact probability between enhancer and promoter expressed as the molar local concentration j(M). A correlation of j(M) with the transcription activation rate was observed for values of 10(-8) M<j(M)<10(-6) M and a kinetic model for NtrC-P-catalyzed open complex formation was developed.

Bacterial Proteins↗

Sequence-dependent elastic properties of DNA.

Harmonic elastic constants of 3-11 bp duplex DNA fragments were evaluated using four 5 ns unrestrained molecular dynamics simulation trajectories of 17 bp duplexes with explicit inclusion of solvent and counterions. All simulations were carried out with the Cornell et al. force-field and particle mesh Ewald method for long-range electrostatic interactions. The elastic constants including anisotropic bending and all coupling terms were derived by analyzing the correlations of fluctuations of structural properties along the trajectories. The following sequences have been considered: homopolymer d(ApA)(n) and d(GpG)(n), and alternating d(GPC)(n) and d(APT)(n). The calculated values of elastic constants are in very good overall agreement with experimental values for random sequences. The atomic-resolution molecular dynamics approach, however, reveals a pronounced sequence-dependence of the stretching and torsional rigidity of DNA, while sequence-dependence of the bending rigidity is smaller for the sequences considered. The earlier predicted twist-bend coupling emerged as the most important cross-term for fragments shorter than one helical turn. The calculated hydrodynamic relaxation times suggest that damping of bending motions may play a role in molecular dynamics simulations of long DNA fragments. A comparison of elasticity calculations using global and local helicoidal analyses is reported. The calculations reveal the importance of the fragment length definition. The present work shows that large-scale molecular dynamics simulations represent a unique source of data to study various aspects of DNA elasticity including its sequence-dependence.

Algorithms↗

Anomalous diffusion of fluorescent probes inside living cell nuclei investigated by spatially-resolved fluorescence correlation spectroscopy.

We have investigated spatial variations of the diffusion behavior of the green fluorescent protein mutant EGFP (F64L/S65T) and of the EGFP-beta-galactosidase fusion protein in living cells with fluorescence correlation spectroscopy. Our fluorescence correlation spectroscopy device, in connection with a precision x-y translation stage, provides submicron spatial resolution and a detection volume smaller than a femtoliter. The fluorescence fluctuations in cell lines expressing EGFP are caused by molecular diffusion as well as a possible internal and a pH-dependent external protonation process of the EGFP chromophore. The latter processes result in two apparent nonfluorescent states that have to be taken into account when evaluating the fluorescence correlation spectroscopy data. The diffusional contribution deviates from ideal behavior and depends on the position in the cell. The fluorescence correlation spectroscopy data can either be evaluated as a two component model with one fraction of the molecules undergoing free Brownian motion with a diffusion coefficient approximately five times smaller than in aqueous solution, and another fraction diffusing one or two orders of magnitude slower. This latter component is especially noticeable in the nuclei. Alternatively, we can fit the data to an anomalous diffusion model where the time dependence of the diffusion serves as a measure for the degree of obstruction, which is large especially in nuclei. Possible mechanisms for this long tail behavior include corralling, immobile obstacles, and binding with a broad distribution of binding affinities. The results are consistent with recent numerical models of the chromosome territory structure in the cell nucleus.

Animals↗

Salt-dependent compaction of di- and trinucleosomes studied by small-angle neutron scattering.

Using small-angle neutron scattering (SANS), we have measured the salt-dependent static structure factor of di- and trinucleosomes from chicken erythrocytes and from COS-7 cells. We also determined the sedimentation coefficients of these dinucleosomes and dinucleosomes reconstituted on a 416-bp DNA containing two nucleosome positioning sequences of the 5S rDNA of Lytechinus variegatus at low and high salt concentrations. The internucleosomal distance d was calculated by simulation as well as Fourier back-transformation of the SANS curves and by hydrodynamic simulation of sedimentation coefficients. Nucleosome dimers from chicken erythrocyte chromatin show a decrease in d from approximately 220 A at 5 mM NaCl to 150 A at 100 mM NaCl. For dinucleosomes from COS-7 chromatin, d decreases from 180 A at 5 mM to 140 A at 100 mM NaCl concentration. Our measurements on trinucleosomes are compatible with a compaction through two different mechanisms, depending on the salt concentration. Between 0 and 20 mM NaCl, the internucleosomal distance between adjacent nucleosomes remains constant, whereas the angle of the DNA strands entering and leaving the central nucleosome decreases. Above 20 mM NaCl, the adjacent nucleosomes approach each other, similar to the compaction of dinucleosomes. The internucleosomal distance of 140-150 A at 100 mM NaCl is in agreement with distances measured by scanning force microscopy and electron microscopy on long chromatin filaments.

Animals↗

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.

Circular Dichroism↗

Compartmentalization of interphase chromosomes observed in simulation and experiment.

Human interphase chromosomes were simulated as a flexible fiber with excluded volume interaction, which represents the chromatin fiber of each chromosome. For the higher-order structures, we assumed a folding into 120 kb loops and an arrangement of these loops into rosette-like subcompartments. Chromosomes consist of subcompartments connected by small fragments of chromatin. Number and size of subcompartments correspond with chromosome bands in early prophase. We observed essentially separated chromosome arms in both our model calculations and confocal laser scanning microscopy, and measured the same overlap in simulation and experiment. Overlap, number and size of chromosome 15 subcompartments of our model chromosomes agree with subchromosomal foci composed of either early or late replicating chromatin, which were observed at all stages of the cell cycle and possibly provide a functionally relevant unit of chromosome territory compartmentalization. Computed distances of chromosome specific markers both on Mb and 10-100 Mb scale agree with fluorescent in situ hybridization measurements under different preparation conditions.

Cell Cycle↗

Superhelical DNA studied by solution scattering and computer models.

We present here recent results on the structure of superhelical DNA and its changes with salt concentration between 0.01 and 1.5 M NaCl. Scattering curves of two different superhelical DNAs were determined by static light scattering. The measured radii of gyration do not change significantly with salt concentration. Small-angle neutron scattering, together with calculations from a Monte Carlo model, allows to determine the superhelix diameter. Measured and simulated scattering curves agreed almost quantitatively. Experimentally we find that the diameter decreases from 16.0 +/- 0.9 nm at 10 mM to 9.0 +/- 0.7 nm at 100 mM NaCl. The superhelix diameter from the simulated conformations decreased from 18.0 +/- 1.5 nm at 10 mM to 9.4 +/- 1.5 nm at 100 mM NaCl. At higher salt concentrations up to 1.5 M NaCl, the diameter stays constant at 9 nm.

Computer Simulation↗

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.

Bacterial Proteins↗