Clathrin-mediated endocytosis and lysosomal cleavage of hepatitis B virus capsid-like core particles

The hepatitis B virus (HBV) core particle serves as a protective capsid shell for the viral genome and is highly immunogenic. Recombinant capsid-like core particles are used as effective carriers of foreign T and B cell epitopes and as delivery vehicles for oligonucleotides. The core monomer contains an arginine-rich C terminus that directs core particle attachment to cells via membrane heparan sulfate proteoglycans. Here we investigated the mechanism of recombinant core particle uptake and its intracellular fate following heparan sulfate binding. We found that the core particles are internalized in an energy-dependent manner. Core particle uptake is inhibited by chlorpromazine and by cytosol acidification known to block clathrin-mediated endocytosis but not by nystatin, which blocks lipid raft endocytosis. Particle uptake is abolished by expression of dominant negative forms of eps15 and Rab5, adaptors involved in clathrin-mediated endocytosis and early endosome transport, respectively. Endocytosed particles are transported to lysosomes where the core monomer is endoproteolytically cleaved into its distinct domains. Using protease inhibitors, cathepsin B was identified as the enzyme responsible for core monomer cleavage. Finally we found that monomer cleavage promotes particle dissociation within cells. Together, our results show that HBV capsid-like core particles are internalized through clathrin-mediated endocytosis, leading to lysosomal cleavage of the core monomer and particle dissociation.     

Ethidium bromide binding to core particle: comparison with native chromatin.

Ethidium bromide intercalation into DNA of nuclease digested erythrocyte chromatin and core particle, was followed at low ionic strength by fluorescence measurements, equilibrium dialysis using 14C labelled dye, circular dichroism and electron microscopy. High affinity binding sites in the chromatin are no more present in the core particle, i.e. when the linker is removed. In the case of core particle, a cooperative process occurs, accompanied by a partial stripping of the DNA from the core histone. Finally two populations of core particles can be detected by electron microscopy as far as their binding properties are concerned.     

Chromatin core particle obtained by selective cleavage of histones H3 and H4 by clostripain

A new chromatin core particle characterized by a half-proteolyzed octamer is obtained by controlled digestion of the native core particle by clostripain. The proteolyzed histones correspond to four polypeptide fragments which are tentatively assigned to H2A[4-129], H2B[1-125], H3[27-135] and H4[18-102] on the basis of electrophoretic evidence and the known specificity of clostripain for arginyl residues. Despite the loss of the N-terminal regions of histones H3 and H4, the partially proteolyzed core particle retains the structural conformation of the native one as shown by circular dichroism. As expected, this half-proteolyzed core particle presents an intermediate accessibility to polycations, such as spermidine, in comparison with that observed with the native core particle and a fully proteolyzed core particle. The latter includes the polypeptide fragments H2A[12-129], H2B[21-125], H3[27-135] and H4[20-102].     

Characterization of hepatitis B virus capsid particle assembly in Xenopus oocytes.

Little is known about the assembly of the 28-nm nucleocapsid or core particle of hepatitis B virus. Here we show that this assembly process can be reconstituted in Xenopus oocytes injected with a synthetic mRNA encoding the hepatitis B virus capsid protein (p21.5). Injected oocytes produce both a nonparticulate p21.5 species (free p21.5) and capsid particles. We describe rapid and simple methods for fractionating these species on a small scale either with step gradients of 10 to 60% (wt/vol) sucrose or by centrifugation to pellet the particles, and we characterize the oocyte core particles. Free p21.5 exhibits chemical and physical properties distinctly different from those of particles. Free p21.5 is partially cleaved by proteinase K, whereas core particles are almost completely resistant to cleavage. This suggests that the carboxyl-terminal protamine region, the main target for proteases within p21.5, is exposed in free p21.5 but faces the interior of the p21.5 core particle. Finally, pulse-chase experiments demonstrated that free p21.5 can be chased almost quantitatively into core particles, establishing that free p21.5 is fully competent to form particles and represents an assembly intermediate on the pathway for core particle formation. However, core particle assembly appears very dependent on p21.5 concentration and is rapidly compromised if the p21.5 concentration is lowered. The advantages of oocytes for studying assembly are discussed.     

A chromatin core particle obtained by selective cleavage of histones by clostripain.

Rat liver chromatin core particles digested with clostripain yield a structurally well-defined nucleoprotein particle with an octameric core made up of fragmented histone species (designated H'2A, H'2B, H'3 and H'4, respectively) after selective loss of a sequence segment located in the N-terminal region of each core histone. Sequential Edman degradation and carboxypeptidase digestion unambiguously establish that histones H2A, H2B, H3 and H4 are selectively cleaved at the carboxyl side of Arg 11, Lys 20, Arg 26 and Arg 19 respectively and that the C-terminal sequences remain unaffected. Despite the loss of the highly basic N-terminal regions, including approximately 17% of the total amino acids, the characteristic structural organization of the nucleosome core particle appears to be fully retained in the proteolyzed core particle, as judged by physicochemical and biochemical evidence. Binding of spermidine to native and proteolyzed core particles shows that DNA accessibility differs markedly in both structures. As expected the proteolyzed particle, which has lost all the in vivo acetylation sites, is not enzymatically acetylated, in contrast to the native particle. However, proteolyzed histones act as substrates of the acetyltransferase in the absence of DNA, as a consequence of the occurrence of potential acetylation sites in the core histones thus rendered accessible. The possible role of the histone N-terminal regions on chromatin structure and function is discussed in the light of the present observations with the new core particle obtained by clostripain proteolysis.     

Protein L20 from the large subunit of Escherichia coli ribosomes is an assembly protein

When 50 S subunits from Escherichia coli are incubated in the presence of 4.3 m-LiCl, the resulting 4.3c core particle quantitatively lacks L20 in addition to other proteins. The 4.3c core can be reconstituted to an active 50 S subunit in the presence of total 50 S proteins by means of the second step incubation of the two-step reconstitution procedure. This finding indicates that the conformation of the 4.3c core is at least equivalent to the conformation of the reconstitution intermediate RI₅₀¹(1) particle, which is exclusively formed in the first-step incubation. It follows that L20 is not necessary for the maintenance of the 4.3c core conformation. In contrast, the total reconstitution of an active 50 S particle from (23 S + 5 S) RNA and a protein preparation lacking L20 was fully dependent on the addition of L20. However, when the 4.3c core, which does not contain L20, is reconstituted with the same protein fraction, the activity of the resulting particle did not depend on the presence of L20. Thus, L20 is essential for the early assembly (occurring in the first-step incubation) but plays no role either in the late assembly steps, or the functions of the mature 50 S particle.Heat treatment of the 4.3c core distorts the 4.3c core conformation and leads to particles with lower s values. The degradation of the 4.3c core conformation is reduced when L20 is added. A further stabilization is obtained by the addition of (L20 + L24). Thus, L20 is dispensable for the maintenance of the 4.3c core conformation, but stabilizes this conformation.     

Fluorescence anisotropy decay of ethidium bound to nucleosome core particles. 2. The torsional motion of the DNA is highly constrained and sensitive to pH

The effects of pH on the torsional flexibility of DNA bound to nucleosome core particles were investigated by using time-resolved fluorescence anisotropy decays of intercalated ethidium. The decays were collected by using time-resolved single-photon counting and were fit to a model developed by J. M. Schurr [(1984) Chem. Phys. 84, 71-96] with a nonlinear least-squares-fitting algorithm developed for this purpose. As the torsional flexibility of DNA is affected by the presence of an intercalating dye, the decays were studied at different ethidium bromide to core particle binding ratios. Because we see large increases in DNA flexibility and in the rotational diffusion coefficient at binding ratios of 0.6 ethidium/core particle and above, we conclude that, under these conditions, the DNA begins to detach from the protein. At lower binding ratios, we observe only small changes in the anisotropy decay. The torsional parameters obtained are a function of N, the number of base pairs of DNA between points of attachment to the histone core. Only if N is greater than 30 base pairs is the torsional rigidity of DNA on a nucleosome core particle higher than that for DNA free in solution. Also, for reasonable values of N (less than 30), the friction felt by the DNA on a core particle is much higher than that felt by free DNA. This indicates that the region of the DNA to which the ethidium binds is highly constrained in its motions. pH changes nearly neutrality at moderate ionic strengths (100 mM) have a substantial effect on the fluorescence anisotropy decays, particularly at early times. These analyses indicated that the observed change on increasing pH can be attributed either to a loosening of the contacts between the DNA and the histone core (increasing N) or to a substantial relaxing of the torsional rigidity of the DNA.     

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.     

Binding of ethidium to the nucleosome core particle. 2. Internal and external binding modes

We have previously reported that the binding of ethidium bromide to the nucleosome core particle results in a stepwise dissociation of the structure which involves the initial release of one copy each of H2A and H2B (McMurray & van Holde, 1986). In this report, we have examined the absorbance and fluorescence properties of intercalated and outside bound forms of ethidium bromide. From these properties, we have measured the extent of external, electrostatic binding of the dye versus internal, intercalation binding to the core particle, free from contribution by linker DNA. We have established that dissociation is induced by the intercalation mode of binding to DNA within the core particle DNA, and not by binding to the histones or by nonintercalative binding to DNA. The covalent binding of [3H]-8-azidoethidium to the core particle clearly shows that less than 1.0 adduct is formed per histone octamer over a wide range of input ratios. Simultaneously, analyses of steady-state fluorescence enhancement and fluorescence lifetime data from bound ethidium complexes demonstrate extensive intercalation binding. Combined analyses from steady-state fluorescence intensity with equilibrium dialysis or fluorescence lifetime data revealed that dissociation began when approximately 14 ethidium molecules are bound by intercalation to each core particle and less than 1.0 nonintercalated ion pair was formed per core particle.     

Microdosimetric structure of heavy ion tracks in tissue

Summary Energy dissipation in tracks of high energy heavy ions in tissue shows a lateral spread of several to many microns depending on the energy of the primary particle. Complete dosimetric characterization, therefore, requires in addition to the Linear Energy Transfer (LET) information on the radial energy distribution. The theory of track structure distinguishes two regions: core and penumbra. The core is a narrow central zone with a radius in tissue far below 1 micron where energy deposition occurs mainly in processes of excitation and electron plasma oscillation. According to the Equipartition Principle, half of the total energy dissipation accrues in this manner. The penumbra is a peripheral zone enveloping the core where energy deposition occurs mainly in ionization events by energetic secondary electrons released by the primary particle in the center of the core traveling at rather high speed thus spreading laterally. The extension of the penumbra depends in a complex manner on the maximum transferable energy to electrons which in turn depends on the speed of the primary particle. Local energy density in the penumbra decreases with the square of increasing radius. It therefore amounts only to a very small fraction of the core density already a few microns away from the center. In general terms, track structure can be described as exhibiting a core of enormous energy density with lateral dimensions remaining entirely on the submicroscopic level surrounded by a penumbra where energy density drops precipitously to very small levels. The relationships are illustrated with micrographs of different sections of a heavy particle track in nuclear emulsion and their counterpart graphical plots.     

Hyperacetylation of core histones does not cause unfolding of nucleosomes. Neutron scatter data accords with disc shape of the nucleosome

Recent studies report that the frictional resistance of partially acetylated core particles increases when the number of acetyl groups/particle exceeds 10 (Bode, J., Gomez-Lira, M. M. & Schr?ter, H. (1983) Eur. J. Biochem. 130, 437-445). This was attributed to an opening of the core particle though other explanations, e.g. unwinding of the DNA ends were also suggested. Another possible explanation is that release of the core histone N-terminal domains by acetylation increased the frictional resistance of the particle. Neutron scatter studies have been performed on core particles acetylated to different levels up to 2.4 acetates/H4 molecule. Up to this level of acetylation the neutron scatter data show no evidence for unfolding of the core particle. The fundamental scatter functions for the envelope shape and internal structure are identical to those obtained previously for bulk core particles. The structure that gave the best fit to these fundamental scatter functions was a flat disc of diameter 11-11.5 nm and of thickness 5.5-6 nm with 1.7 +/- 0.2 turns of DNA coiled with a pitch of 3.0 nm around a core of the histone octamer. The data analysis emphasizes the changes in pair distance distribution functions at relatively low contrasts, particularly when the protein is contrast matched and DNA dominates the scatter. Under these conditions there is no evidence for the unwinding of long DNA ends in the hyperacetylated core particles. The distance distribution functions go to zero between 11.5 and 12 nm which gives the maximum chord length in a particle of dimension, 11 nm X 5.5 nm. The distance distribution function for the histone octamer contains 85% of the vectors within the 7.0-nm diameter of the histone core. 15% of the histone vectors lie between 7.0 and 12.0 nm, and these are attributed to the N-terminal domains of the core histones which extend out from the central histone core. Histone vectors extending beyond 7.0 nm are necessary to account for the measured radius of gyration of the histone core of 3.3 nm. A similar value of 3.2 nm is calculated for the recent ellipsoidal shape of 11.0 X 6.5 X 6.5 nm from the crystal structure of the octamer. However, the nucleosome model based on this structure is globular, roughly 11 nm in diameter, which does not accord with the flat disc shape core particle obtained from detailed neutron scatter data nor with the cross-section radii of gyration of the histone and DNA found previously for extended chromatin in solution.     

Orientation of the pigments in Photosystem II: low-temperature linear-dichroism study of a core particle and of its chlorophyll-protein subunits isolated from Synechococcus sp.

The orientation of the pigments in the Photosystem II core particle isolated from the thermophilic cyanobacterium Synechococcus sp. has been investigated by linear dichroism spectroscopy at 10 K of macroscopically oriented samples. The absorbance (A), linear dichroism (LD) and LD/A spectra are remarkably similar to those previously reported for a core complex isolated from Chlamydomonas reinhardtii (Biochim. Biophys. Acta 850 (1986) 156–161). The spectra of the Synechococcus core particle are compared to the corresponding spectra obtained on its two main constituent chlorophyll-protein complexes CP2-b (photochemically active) and CP2-c (photochemically inactive). The various features seen in the spectra of the core particle appear well segregated into the spectra of one or the other of the two subparticles without significant loss of orientation of the pigments. The orientation of the chlorophyll macrocycles, with the Y and X optical axis preferentially parallel and perpendicular to the plane of largest cross-section of the particle, respectively, is very similar in the two subparticles. CP2-b contains mainly the beta-carotene pool absorbing around 505 and 470 nm, which is oriented close to the membrane plane, while CP2-c contains the beta-carotene pool absorbing around 495 and 465 nm and oriented closer to the normal to the membrane plane. A shoulder at 682 nm in the absorbance and linear dichroism spectra of the core complex is fully segregated in the spectra of CP2-c, thus excluding the possibility that this spectral feature could be assigned to the primary donor of PS II. A negative linear dichroism component peaking around 691 nm (LD 691) in the core particle is mainly segregated in CP2-b together with the photoactive pheophytin acceptor molecule responsible for the 544 nm positive linear dichroism signal (LD 544). While the ratio of the amplitudes LD 691/LD 544 is approximately the same for the core particle and for the CP2-b complex, the amplitude of LD 691 is significantly reduced in CP2-b compared to the core particle.     

Thermal transition of core particle is not a two-state process

Thermal transition of core particle which occurs before melting of DNA and can be followed by circular dichroism is not a two-state process; it is the result of two processes which cannot be dissociated in static experiments: unfolding of core particles is immediately followed by their aggregation. It is thus impossible to get thermodynamic parameters of core particle unfolding from its thermal transition monitored by circular dichroism. Thermal denaturation kinetics of core particles gives some information about their stability. Finally core particle structure is more stable in chromatin than in its isolated state.     

Nucleosome core particle self-assembly kinetics and stability at physiological ionic strength

Micrococcal nuclease, DNase I, and trypsin have been employed to study the kinetics of core particle self-assembly by salt jump from 2.0 to 0.2 M NaCl. A few seconds after the initiation of the reassociation reaction, the bulk of core particle DNA becomes protected from digestion by micrococcal nuclease, whereas free DNA, under the same conditions, is completely hydrolyzed. The central and C-terminal regions of core histones are also protected from trypsin digestion immediately after the 2.0-0.2 M NaCl salt jump. Moreover, the extent of degradation produced by trypsin is the same for samples digested a few seconds after the salt jump and for samples digested 20 min after the salt jump. With DNase I, minor structural differences have been detected between samples obtained at different times during the reaction. However, even in this case our results indicate that many of the characteristic histone-DNA contacts within the core particle are made a few seconds after the initiation of the self-assembly reaction. Furthermore, core particles have been labeled with the fluorescent reagent N-(1-pyrenyl)maleimide (NPM), which was previously used as a sensitive probe for nucleosome conformation. Extensive DNase I or trypsin digestion of NPM-labeled core particles in 0.2 M NaCl does not produce significant changes in excimer fluorescence. This allows us to conclude that the covalent continuity of DNA is not required for the maintenance of the folded conformation of the core particle and that the trypsin-resistant domains of core histones play a fundamental role in the stabilization of this structure.     

The structure of hepadnaviral core antigens. Identification of free thiols and determination of the disulfide bonding pattern.

A set of wild-type and mutant human, woodchuck, and duck hepatitis viral core proteins have been prepared and used to study the free thiol groups and the disulfide bonding pattern present within the core particle. Human (HBcAg) and woodchuck (WHcAg) core proteins contain 4 cysteine residues, whereas duck (DHcAg) core protein contains a single cysteine residue. Each of the cysteines of HBcAg has been eliminated, either singly or in combinations, by a two-step mutagenesis procedure. All of the proteins were shown to have very similar physical and immunochemical properties. All assemble into essentially identical core particle structures. Therefore disulfide bonds are not essential for core particle formation. No intra-chain disulfide bonds occur. Cys107 is a free thiol buried within the particle structure, whereas Cys48 is present partly as a free sulfhydryl which is exposed at the surface of the particle. Cys61 is always and Cys48 is partly involved in interchain disulfide bonds with the identical residues of another monomer, whereas Cys183 is always involved in a disulfide bond with the Cys183 of a different monomer. WHcAg has the same pattern of bonding, whereas DHcAg lacks any disulfide bonds, and the single free sulfhydryl, Cys153 which is equivalent to Cys107 of HBcAg, is buried.     

Molecular modelling study of changes induced by netropsin binding to nucleosome core particles.

It is well known that certain sequence-dependent modulators in structure appear to determine the rotational positioning of DNA on the nucleosome core particle. That preference is rather weak and could be modified by some ligands as netropsin, a minor-groove binding antibiotic. We have undertaken a molecular modelling approach to calculate the relative energy of interaction between a DNA molecule and the protein core particle. The histones particle is considered as a distribution of positive charges on the protein surface that interacts with the DNA molecule. The molecular electrostatic potentials for the DNA, simulated as a discontinuous cylinder, were calculated using the values for all the base pairs. Computing these parameters, we calculated the relative energy of interaction and the more stable rotational setting of DNA. The binding of four molecules of netropsin to this model showed that a new minimum of energy is obtained when the DNA turns toward the protein surface by about 180 degrees, so a new energetically favoured structure appears where netropsin binding sites are located facing toward the histones surface. The effect of netropsin could be explained in terms of an induced change in the phasing of DNA on the core particle. The induced rotation is considered to optimize non-bonded contacts between the netropsin molecules and the DNA backbone.     

Production of hepatitis B virus nucleocapsidlike core particles in Xenopus oocytes: assembly occurs mainly in the cytoplasm and does not require the nucleus.

The location of hepatitis B virus (HBV) nucleocapsid (core particle) assembly in infected cells remains controversial. Some lines of evidence implicate the nucleus; others favor the cytoplasm. Via injection of a synthetic mRNA encoding the HBV nucleocapsid protein (p21.5), we have expressed both unassembled p21.5 and nucleocapsidlike core particles in Xenopus oocytes. Subcellular fractionation reveals that approximately 91% of the unassembled p21.5 and 95% of the core particles are cytoplasmic, with only 9 and 5%, respectively, in the nucleus. We present evidence showing that unassembled p21.5 equilibrates between nucleus and cytoplasm by passive diffusion and that intact core particles do not enter the nucleus. To examine the role of the nucleus in core particle formation, we expressed p21.5 in surgically anucleate oocytes. We show that anucleate oocytes support efficient core particle formation, indicating that (i) the nucleus is not essential for assembly and (ii) the cytoplasm can assemble most core particles found in oocytes. On the basis of our data, we propose that in oocytes, most core particle assembly (up to 95%) occurs in the cytoplasm, but that at least approximately 5% of the cellular core particles are assembled in the nucleus and remain there. We discuss the implications of these findings for the formation of replication-competent core particles in infected cells.     

Purification and phosphorylation of initiation factor eIF-2 from rabbit skeletal muscle

Core particle DNA unfolding and refolding are followed by stopped-flow circular dichroism technique. When core particles are dissociated in the stopped-flow cuvette, the high CD deviation corresponding to the dissociated state is reached in the first millisecond, which means that the dissociation process is completed within the dead time of the apparatus which is ～1 ms. The same conclusion can be drawn when core particles are reassociated, since the low CD value, typical of the associated state, is immediately reached. Similarly histone release from chromatin is a very fast process. We also include some points of discussion about core particle assembly process.     

Analysis of the binding of high mobility group protein 17 to the nucleosome core particle by 1H NMR spectroscopy

The binding of high mobility group (HMG) protein 17 to the nucleosome core particle has been studied in D2O solution using 1H NMR at 500 MHz. Spectra were obtained for purified HMG 17, purified nucleosome core particles, and the reconstituted HMG 17-nucleosome core particle complex at 0.1, 0.2, 0.3, and 0.4 M NaCl. Subtraction of the core particle spectra from spectra of the core particle reconstituted with HMG 17 demonstrated those regions of HMG 17 which interact with the nucleosome at different ionic strengths; the resonance peaks of interacting groups are broadened due to their restricted mobility. At 0.1 M NaCl, the mobility of all the amino acid side chains of HMG 17 was restricted, indicating complete binding of HMG 17 to the much larger nucleosome core particle. At 0.2 M NaCl most of the amino acids were free with the exception of arginine and proline which are confined to or predominant in the basic central region of HMG 17. These amino acids were completely free only at 0.4 M NaCl. We conclude that the entire HMG 17 molecule interacts with the nucleosome core particle at physiological ionic strength. The acidic COOH-terminal region of HMG 17 is released from interaction with the core histones at an NaCl concentration between 0.1 and 0.2 M and so binds weakly at physiological ionic strength. The basic central region binds more strongly to the core particle DNA, being completely released only at much higher ionic strength, between 0.3 and 0.4 M NaCl.     

Packaging of up to 240 subunits of a 17 kDa nuclease into the interior of recombinant hepatitis B virus capsids

The icosahedral nucleocapsid of hepatitis B virus (HBV) consists of multiple subunits of a single 183 amino acids (aa) core protein encasing the viral genome. However, recombinant core protein alone also forms capsid-like particles. We have recently shown that a 238 aa protein centrally inserted into the core protein can be displayed on the particle surface. Here we demonstrate that replacement of the C-terminal basic domain by the 17 kDa Staphylococcus aureus nuclease also yields particles but that in these the foreign domains are located in the interior. The packaged nuclease is enzymatically active, and the chimeric protein forms mosaic particles with the wild-type core protein. Hence the HBV capsid is useful as a molecular platform which, dependent on the fusion site, allows foreign protein domains to either be packaged into or be exposed on the exterior of the particle. These results are of relevance for the use of the HBV capsid as a vaccine carrier, and as a target for antiviral therapy.