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Molecular and Cellular Biology, January 2009, p. 538-546, Vol. 29, No. 2
0270-7306/09/$08.00+0 doi:10.1128/MCB.01343-08
Copyright © 2009, American Society for Microbiology. All Rights Reserved.

Department of Biochemistry and Biophysics,2 Department of Pathology, University of Rochester, Rochester, New York 146421
Received 22 August 2008/ Returned for modification 29 September 2008/ Accepted 28 October 2008
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Although the molecular mechanisms behind the formation of secondary and tertiary chromatin structures remain unclear, work employing model systems has shown that in vitro reconstituted nucleosome arrays containing only DNA and core histone proteins undergo the same initial salt-dependent condensations as native chromatin (17, 21). In solutions containing physiological concentrations of mono- and divalent cations, nucleosome arrays spontaneously fold into structures with the same hydrodynamic shape as the 30-nm-diameter chromatin fiber and reversibly self-associate into larger assemblies with characteristics of native tertiary chromatin structures (21, 45). Thus, the primary protein determinants defining these structures reside within the core histone proteins. Linker histones promote the salt-dependent folding and condensation of chromatin secondary and tertiary structures without altering the fundamental characteristics of these structures (8, 9, 25).
Hydrodynamic studies and electron microscopy observations have revealed that nucleosome arrays lacking the core histone N-terminal tail domains are unable to form 30-nm fibers and do not undergo fiber-fiber association in high-salt solutions (7, 16, 30, 39), indicating that these domains are essential for the formation of secondary and tertiary chromatin structures. Notably, each of the four N-terminal tail domains does not contribute equally to the folding and oligomerization of nucleosome arrays (19). Arrays lacking one or more of the histone tail domains showed characteristic extents of deficiency in both formation of the 30-nm fiber and interarray association, with arrays containing only the H3/H4 tails condensing better than those with only the H2A/H2B tails (39). More detailed characterization of the individual tails indicated that despite being the second-shortest tail overall, the H4 tail provides the largest contribution to stabilizing higher-order chromatin structures (12, 19). In comparison, the H3 tail contributes slightly less to both secondary and tertiary structure formation, while the H2A/H2B tails are the least significant but still important participants in the chromatin condensation processes (19).
Model nucleosome arrays have also been used to elucidate structural aspects of tertiary chromatin structures. Early on, Hansen's group used analytical velocity sedimentation methods to show that formation of self-associated tertiary structures is highly cooperative and reversible, paralleling the behavior of native chromatin (21, 30). They further showed that the initial step in the process involves self-association of monomeric nucleosome arrays (55 S) into oligomeric structures approximately 10 times larger than the arrays (about 500 S), without appreciable accumulation of species of intermediate sizes. As the salt is increased further, these
500-S structures continue to self-associate into extremely large complexes that sediment in excess of >>10,000 S. These observations provide a rigorous physicochemical basis for a simple microcentrifuge-based assay now routinely used to study self-association (5, 10, 25, 30, 33, 43). Association of linker histones also pushes the equilibrium toward the largest species (8, 30). Interestingly, while subsaturated arrays that have nucleosome-free gaps cannot undergo divalent cation-induced folding, they retain the ability to self-associate into tertiary structures, albeit at higher MgCl2 concentrations. The formation of such structures in vitro may reflect the continued association of transcriptionally active regions of chromatin in compact chromatin territories in vivo (41).
Chromatin plays an integral role in the regulation of gene expression and other processes typically by restricting access to genomic DNA. Thus, activation of gene expression involves transient decondensation of higher-order chromatin structures, facilitated by specific posttranslational modifications such as lysine acetylation within the histone tail domains or ATP-dependent chromatin remodeling (6, 20). Consistent with their essential roles in chromatin structure, the histone tail domains are the sites of most of the posttranslational modifications related to transcriptional activation, gene silencing, and the formation of heterochromatin (35, 42). Indeed, some posttranslational modifications, such as acetylation, are known to directly alter chromatin structure in preparation for transcriptional activation, presumably by altering interactions of the tail domains (1, 18, 39, 44). For example, hydrodynamic studies have shown that acetylation of the tail domains inhibits folding of nucleosome arrays into secondary and tertiary chromatin structures (18, 40, 43), with acetylation of H2B and H4 having the greatest effect on tertiary structure formation (43).
While interactions of the basic core histone tail domains with DNA have been well documented, evidence indicates that these domains also interact with protein targets in condensed chromatin. Quantitative analysis of surface charge density during salt-dependent folding of nucleosome arrays indicated that some of the tails participate in interactions with other histones, possibly involving tail-tail interactions in condensed structures (16). Indeed, a region in the N-terminal tail of H4 (amino acids [aa] 16 to 25) was found to contact a surface of the H2A/H2B dimer between highly ordered nucleosome core particles within a crystal lattice (11, 27). Additional evidence for this H4 tail-H2A interaction was later obtained with in vitro cross-linking experiments and interpreted as supporting a two-start model for the 30-nm fiber (13). Hydrodynamic studies showed that a deletion within the H4 tail near this region (aa residues 14 to 19) as well as the introduction of a single acetylated lysine residue into this region inhibited salt-dependent folding and self-association of model nucleosome arrays (12, 33). Furthermore, recent studies have indicated that nonallelic H2A variants change the ability of nucleosome arrays to fold and condense through alterations in this H4 tail-H2A interaction (15, 49).
Although the core histone tail domains are critical regulators of chromatin structure and play an essential role in the control of transcription and other processes, details of the molecular interactions of the tails and the mechanisms by which posttranslational modifications regulate tail structures and interactions remain poorly understood. Since the H4 tail plays a central role in defining higher-order chromatin structures, we investigated interactions of this domain during formation of secondary and tertiary chromatin structures with model nucleosome arrays. We find that the H4 tail mediates long-range interfiber interactions similar to those previously documented for the H3 tail domain (25). However, in contrast to the H3 tail domain, a region of the H4 tail near the histone fold domain exhibits interarray contacts to both DNA and protein targets in condensed chromatin structures. Moreover, linker histones strongly stimulate interarray interactions, but this stimulation is abrogated by acetylation within the tail domain. These results extend our understanding of critical long-range interactions of the H3 and H4 tail domains as well as provide new insights into the mechanisms underlying formation of higher-order chromatin structures.
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Expression of 3H-labeled H4 (*H4) proteins.
Recombinant H4 G2C and H4 V21C, which contain a single cysteine substituted for amino acids 2 and 21, respectively, were prepared based on Xenopus laevis major H4 as previously described (48). pET3a vectors containing sequences coding for these proteins were transformed into BL21(DE3) by standard methods. Transformed Escherichia coli was grown overnight in 5 ml of minimal medium and then transferred into 50 ml of fresh minimal medium. At an optical density at 600 nm of
0.6, expression was induced by isopropyl-β-D-thiogalactopyranoside, then 2.5 mCi of [3H]lysine was added 20 min after induction and the cells were grown for another 3 h (46). Incorporation of [3H]lysine into recombinant H4 was examined by analyzing bacterial proteins on sodium dodecyl sulfate-polyacrylamide gel electrophoresis (SDS-PAGE), soaking the gel in 1 M salicylic acid for 15 min, drying the gel, and performing detection by exposure to X-ray film at –70°C.
Acetylation of core histone proteins. Purification of the Piccolo v55 histone acetyltransferase (HAT) complex and acetylation reactions were performed as described previously (43). Briefly, components of the Piccolo complex were expressed in transformed BL21(DE3) cells and purified by nickel column chromatography. Activities of the Piccolo complex preparations vary in each purification, and trial serial titrations were necessary to optimize conditions for the acetylation reaction. The acetylation reactions were performed at 30°C in reaction buffer (25 mM Tris, pH 8.0, 0.1 mM EDTA, 150 mM NaCl, 10% glycerol, 1 mM phenylmethylsulfonyl fluoride, and 10 mM sodium butyrate) with a sufficient amount of acetyl-coenzyme A (10-fold the H4 protein concentration) as a cosubstrate. Briefly, 20 µl of 25 µM (H3/H4)2 was mixed with 10 µl of purified Piccolo v55 HAT complex and 1 µl of 5 mM acetyl-coenzyme A in a total volume of 200 µl. The extent of H4 acetylation was determined by Triton-acid-urea gel electrophoresis as described previously (43). Typically complete tetraacetylation of the H4 tail also resulted in some monoacetylation of H3.
Reconstitution and analysis of nucleosome arrays. Nucleosome array DNA templates, containing 12 tandem repeats of a 208-bp 5S rRNA sequence from Lytechinus variegatus, were reconstituted with core histone proteins by salt dialysis. Core histone proteins were mixed with DNA in a 1.2:1 ratio in 2 M NaCl/TE, followed by dialysis against 1 M NaCl/TE for 4 h, 0.75 M NaCl/TE for 3 h, and finally 10 mM Tris, 0.1 mM EDTA, and 0.1 mM EGTA overnight. The level of histone saturation was examined by EcoRI digestion and analysis of nucleosome and free DNA bands on nucleoprotein gels as described previously (25). The efficiency of self-association of nucleosome arrays into oligomeric structures in the presence of divalent cations is dependent on the level of saturation and was also used to gauge the extent of nucleosome occupancy (30). The 35-mer nucleosome array was reconstituted by the same method using a DNA fragment containing 35 tandem 5S rRNA gene repeats and core histone proteins purified from chicken erythrocytes as described previously (24).
UV-induced cross-linking and identification of interarray cross-linking. The 35-mer nucleosome array (8.1 µl, 0.2 mg/ml) was mixed with 8.1 µl of 12-mer nucleosome arrays (0.04 mg/ml) reconstituted with *H4 and APB-modified recombinant H4, followed by addition of 1.8 µl of 10x MgCl2 containing 10 mM Tris to attain final MgCl2 concentrations of 0 to 8 mM. The sample was placed inside a Falcon 5-ml polystyrene tube and enclosed in a 15-ml Pyrex 9820 glass tube. The sample was irradiated for 1 min at 365 nm on a VMR LM-20E light box. The irradiated samples were then adjusted to 0.01% SDS and 0.2 µg/ml ethidium bromide (EtBr), and the samples were separated on a 0.7% agarose gel (0.5x Tris-borate-EDTA, 0.01% SDS, 0.2 µg/ml EtBr). After UV photography, the gels were soaked in 45% methanol and 10% acetic acid, then 1 M sodium salicylate for 15 min, and then dried. The gels were exposed to Kodak MR film at –70°C for 1 to 2 weeks.
H4 tail-H2A cross-linking. The 12-mer nucleosome arrays or mononucleosomes (18 µl, 0.08 mg/ml) reconstituted with wild-type H2A or H2A G2C-fluorescein and *H4 V21C-APB were mixed with 2 µl of 10x MgCl2, and the samples were cross-linked as described above. The irradiated samples were directly analyzed on 15% SDS-PAGE. The fluorescent signals derived from H2A G2C-fluorescein were recorded by fluorography. The location of radioactivity of samples due to *H4 V21C-APB was monitored as described in the interarray cross-linking experiment. In competition experiments, the LANA and LRS (scrambled) peptide (10) were added to a 5- to 10-fold molar excess over nucleosome concentrations.
Linker histone binding assay. Purified recombinant Xenopus H1° was mixed with 8.1 µl of a 35-mer nucleosome array (0.2 mg/ml) and 8.1 µl of a 12-mer nucleosome array (0.04 mg/ml) in an approximately 1:1 H1 protein/nucleosome ratio as determined by SDS-PAGE with standards calibrated by amino acid analysis in the presence of 50 mM NaCl on ice for 3 h. The exact amount of H1 required to saturate the nucleosome arrays was empirically determined by centrifugation of H1-bound arrays at 13,000 rpm for 15 min in a microcentrifuge in the presence of 1.3 mM MgCl2 to precipitate oversaturated arrays (8). The stoichiometries of H1-bound 12-mer and 35-mer arrays were further confirmed by SDS-PAGE and a comparison to native chromatin samples.
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FIG. 1. Detection of interarray H4 tail-DNA interactions from a position near the N terminus of the H4 tail domain. (A) Scheme of histone H4 showing the location of cysteine substitution (H4 G2C) and the site of APB-cross-linker attachment. The related site on the H3 tail domain (H3 T6C) investigated previously is also shown. (B) The 12-mer nucleosome arrays reconstituted with *H4 G2C-APB were mixed with 35-mer arrays, and the extent of the MgCl2-dependent interarray H4 tail-DNA cross-linking was determined. Cross-linking reactions were carried out in 0, 2, 4, 6, and 8 mM MgCl2 (lanes 2 to 6, respectively) as indicated. The sample in lane 1 was incubated in 10 mM Tris without UV irradiation. Upper panel, EtBr-stained gel; lower panel, autoradiograph of the same gel. (C) Interarray cross-linking of the H4 tail domain was quantified and plotted as the fraction of total cross-linking at each MgCl2 concentration (diamonds). For comparison, data previously obtained with *H3 T6C-APB (squares) are also shown. (D) Chromatin compaction decreases intraarray cross-linking efficiency of H4 G2C-APB. The relative extent of cross-linking to the 12-mer template at various MgCl2 concentrations (25) (C) was determined and normalized to cross-linking in the absence of salt.
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We also noticed that increases in interarray interactions by the N-terminal region of the H4 tail domain during salt-dependent condensation of the nucleosome arrays were accompanied by a distinct loss of cross-linking to the 12-mer array. For example, at 8 mM MgCl2, cross-linking of the H4 tail to the 12-mer template drops to about 35% of the value observed in the absence of salt (Fig. 1D). By comparison, cross-linking of the N-terminal end of the H3 tail domain remained fairly constant for all levels of MgCl2, at about 80% of the value observed in the absence of salt. This result suggests that intraarray contacts of the H4 tail domain are lost upon salt-dependent condensation of the arrays, perhaps in favor of interarray contacts to the 35-mer template (Fig. 1C) or other targets (see below).
Previous work showed that the extent of interarray interactions detected for the H3 tail domain decreased as the probe was moved closer to the histone fold domain (25). We therefore tested whether the extent of interarray interaction is dependent upon location within the H4 tail domain by generating 12-mer arrays containing *H4 V21C-APB, in which the cross-linker is located near the histone fold domain of H4 (Fig. 2A). In contrast to an equivalent position in the H3 tail domain (Fig. 2A), arrays containing *H4 V21C-APB exhibited a significant fraction of total cross-links to the 35-mer DNA template in elevated MgCl2, similar to that observed for the N-terminal end of the H4 tail domain (Fig. 1C and 2B and C). However, it is important to note that cross-linking of *H4 V21C-APB to the DNA templates occurred with a much lower efficiency compared to that observed with other positions in either the H3 or H4 tail domains. For example, quantification of Fig. 2C shows that about 1% ± 0.3% of H4 V21C-APB was cross-linked to the 12-mer template, while about 20% ± 5% H4 G2C-APB or H3 T6C-APB (25) was cross-linked to this template.
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FIG. 2. Regions within the H3 and H4 tails near the histone fold domain exhibit distinctly different patterns of interactions. (A) A scheme of the H4 protein showing the site near the H4 histone fold domain (H4 V21C) modified by APB. The location of an analogous site in the H3 tail domain (H3 V35C) previously investigated is also shown. (B) The 12-mer nucleosome arrays were reconstituted with *H4 V21C-APB or *H3 V35C-APB and analyzed for interarray tail-DNA cross-linking as described in the legend to Fig. 1B. (C) Interarray cross-linking for regions near the histone fold domains in H4 (diamonds) and H3 (squares) was quantified and plotted as described in the legend to Fig. 1.
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FIG. 3. A region within the H4 tail interacts with H2A in both an intra- and internucleosomal fashion. The 12-mer nucleosome arrays reconstituted with H2A G2C-fluorescein and *H4 V21C-APB were incubated in 0, 1, 2, and 4 mM MgCl2 and then UV-irradiated (lanes 2 to 5). The sample in lane 1 was incubated in 10 mM Tris without UV irradiation. Cross-linking products observed by Coomassie blue staining (A), fluorography (B), and autoradiography (C) are shown. (D) Quantification of H2A-H4 cross-linked species in nucleosome arrays (squares) and mononucleosomes (diamonds). (E) Specific competition of H4-H2A cross-linking with LANA peptide. Cross-linking of arrays was carried out in the presence of the LANA or LRS peptide (10), and the extent of cross-linking was quantified and plotted relative to that in the absence of peptide. Errors represent ±1 standard deviation. (F and G) H4-H2A cross-linking in mononucleosomes analyzed by Coomassie blue staining (E) and fluorography (F).
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Acetylation of the histone tails can have a direct effect on higher-order chromatin structures, possibly by altering intra- or internucleosome interactions of the core histone tail domains (2, 18, 33, 40). Four lysines within the H4 tail domain can be acetylated, and hyperacetylated H4 is found in transcriptionally active chromatin (20). To examine the effect of acetylation of the H4 tail domain on tail-DNA and protein interactions, (H3/H4)2 tetramers were incubated with the Piccolo v55 HAT complex (32, 43), which resulted in quantitative tetraacetylation of H4 within the complex (Fig. 4A and B, lane 2). Consistent with published data (43), we found that arrays containing tetraacetylated *H4 G2C-APB exhibited a reduction in the propensity to undergo salt-dependent self-association, with an Mg50 for unacetylated and H4-acetylated arrays of 3.5 ± 0.5 mM and 5.2 ± 0.5 mM, respectively (plots not shown; see reference 42). However, cross-linking experiments with nucleosome arrays containing unacetylated and acetylated *H4 G2C-APB showed that acetylation had little effect on the extent of interarray interactions in 6 to 8 mM MgCl2 (Fig. 4D).
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FIG. 4. Effect of H4 acetylation on H4 tail-DNA interarray interactions. The 12-mer array was prepared with tetraacetylated *H4, and interarray cross-linking was analyzed as described in the legend to Fig. 1. (A) A scheme of H4 showing the four sites of acetylation in the tail domain. (B) A Triton-acid-urea gel showing H4 tetraacetylated and H3 monoacetylated by HAT Piccolo. Lane 1, nonacetylated H3/H4; lane 2, highly acetylated H3/H4; lane 3, moderately acetylated H3/H4 revealing various extents of H4 acetylation. (C and D) Analysis of interarray cross-linking mediated by control (squares) and tetraacetylated (diamonds) *H4 G2C-APB. Experimental conditions and data analysis were as described in the legend to Fig. 1.
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FIG. 5. Acetylation overrides H1 enhancement of interarray interactions of the H4 tail domain. (A) Arrays incubated in the absence (lanes 1 to 6) or presence (lanes 7 to 12) of H1 were assayed for interarray H4 tail-DNA cross-linking. The cross-linking assay was carried out as described in the legend to Fig. 1 except that each sample also contained 50 mM NaCl to facilitate H1 binding. (B) Interarray cross-linking in the absence (circles) and presence (diamonds) of H1 was quantified and plotted as indicated. Quantification of cross-linking for arrays in buffer without NaCl (squares) is shown for reference. Panel C is as described in panel B except that arrays contained acetylated H4.
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FIG. 6. Summary of H3 and H4 tail interactions. Intra-array and interarray interactions with DNA and histones detected for two positions in either tail domain are as indicated.
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Importantly, while we do detect interarray interactions between the interior of the H4 tail domain and DNA, the efficiency of cross-linking to DNA is significantly less than that detected from a site near the N-terminal end of the H4 tail (see above). Moreover, this region of the H4 tail domain (aa 16 to 25) has been shown to contact a pocket on the surface of H2A in crystals of nucleosome core particles and to form disulfide cross-links between nucleosomes with H2A in solution studies of nucleosome arrays containing specific cysteine substitution mutants of these proteins (13, 27). A 6-aa acidic patch (E56, E61, E64, D90, E91, and E92) on H2A forms multiple contacts with K16, R19, K20, and R23 on the H4 tail (11, 27), and H2A variants, which have a less-extensive acidic patch (e.g., H2A.Z and H2A.Bbd, respectively), have been shown to alter the propensity of nucleosome arrays to form higher-order chromatin structures, presumably through alterations in this H2A-H4 tail interaction (15, 49). Consistent with these observations, we find robust cross-linking between the interior region of the H4 tail and H2A, which increases significantly upon salt-dependent folding of the arrays (Fig. 3). Importantly, we find that cross-linking between H4 and H2A is competed by the LANA peptide, previously shown to bind strongly to the H2A pocket and displace the H4 tail but significantly less so by a peptide of similar composition but scrambled sequence (Fig. 3D). Thus, our results are consistent with a model whereby interaction of the H4 tail with the H2A pocket stimulates intramolecular folding of nucleosome arrays, while interarray interactions with DNA facilitate self-association, perhaps in an exclusive manner (10, 13, 15, 33, 49) (Fig. 6). For example, some H4 tails may contact H2A to facilitate the formation of secondary chromatin structures, while others may participate in longer-range interarray contacts to DNA to mediate formation of tertiary structures. This model is supported by studies showing that LANA peptide-mediated displacement of H4 from the H2A pocket stimulates self-association of arrays, presumably because the H4 tail is more available to contact interarray DNA targets (10), and the observation that alterations in the interaction between H2As and the H4 tail appear to exert opposite effects on chromatin folding and array self-association (15, 49).
Interestingly, we also detected H4 tail-H2A interactions in low-salt (10 mM Tris) conditions where the nucleosome arrays exist in fully extended conformations, with little opportunity for internucleosomal contacts (13, 31). We considered the possibility that these interactions represented previously undocumented intranucleosomal interactions. Indeed, the existence of intranucleosomal H4 tail-H2A interactions is supported by our cross-linking experiments with mononucleosomes (Fig. 3). Such interactions may be relevant in regions where chromatin is transiently decondensed due to nucleosome eviction or posttranslational modification (21). A recent study of the histone variant H2A.Bbd also suggested that the H4 tail might interact with the H2A pocket in an intranucleosomal manner (49). Nucleosome arrays containing H2A.Bbd exhibited an unusually extended conformation in low salt, suggesting that the DNA was partially unwrapped from the edges of the nucleosome, consistent with studies showing H2A.Bbd nucleosomes protect less than 147 bp of DNA from nuclease digestion (4, 14). Moreover, it was found that a restored acidic patch on the H2A.Bbd surface works together with the H4 tail to maintain an intact 29 S (normally extended) chromatin conformation in low salt in which the nucleosomes contain DNA that is fully wrapped around the histone octamers (49). These data, together with our cross-linking results, suggest that the H4 tail participates in intranucleosome contacts with the acidic patch to stabilize wrapping of DNA in the nucleosome. It is unclear whether this intranucleosome interaction competes with internucleosome interactions of the H4 tail facilitating formation of higher-order chromatin structures.
We also found that 12-mer arrays reconstituted with tetraacetylated H4 showed a lower tendency to self-associate in high MgCl2 concentrations, consistent with previous work (43). However, interarray interactions as detected by our cross-linking method did not appear to be reduced. Work by Hansen and colleagues has shown that self-association of arrays into tertiary structures occurs via a multistep process, with initial formation of soluble intermediates of
500 S in lower MgCl2, which then associate into complexes of thousands of S in higher MgCl2, which can be rapidly sedimented in a microcentrifuge (21, 30). Our cross-linking results suggest that interarray interactions of the H4 tail domain occur during this first step and that the extent of these interactions is not appreciably altered by acetylation of the tail domain. However, acetylation of the tail does appear to reduce the propensity of subsequent steps in the self-association process, such that higher levels of MgCl2 are required to achieve the same extent of sedimentable material. Thus, our results are consistent with the idea that tertiary chromatin structure formation is a multistep process, with the H4 tail domain making long-range interarray contacts to DNA during an initial step of this process.
Acetylation does appear to have a profound effect on the ability of H1 to stimulate interarray interactions by both the H3 (25) and H4 tail domains (Fig. 5). H1 might either directly interact with the tail domains, redirecting them to interarray locations, or indirectly increase interarray contacts by stabilizing formation of higher-order chromatin structures. Importantly, H1 enhanced interarray interactions of both the H3 and H4 tail domains without altering the maximum extent of interarray contacts generated by these tails observed in the absence of H1. This result is consistent with the idea that H1 stabilizes but does not appreciably alter the final condensed structure (8, 9). Interestingly, acetylation of either the H3 or H4 tail domain appears to override this stimulatory effect of H1, suggesting that the effects of this posttranslational modification are dominant over linker histones in regulating the stability of higher-order chromatin structures. It will be interesting in future work to determine whether this effect is due to acetylation of specific lysine residues or requires a simple threshold level of acetylation within the tail domains.
In conclusion, our results underscore the complex and diverse interactions of the H4 tail domain and are consistent with the idea that the tails perform multiple independent functions in chromatin (21). We have detected intranucleosome interactions of the H4 tail with H2A, consistent with a role for the H4 tail in stabilizing wrapping of DNA around the nucleosome (3, 49) and internucleosome and interarray contacts with both H2A and DNA, consistent with a role of the H4 tail in stabilizing secondary and tertiary chromatin structures (10, 19, 49) (Fig. 6). Moreover, our results highlight the fact that individual histone tail domains participate in distinct sets of interactions. For example, a region near the histone fold domain in the H3 tail interacts exclusively with DNA in an intranucleosomal fashion, while an analogous region in the H4 tail interacts both intra- and internucleosomally with both DNA and an acidic pocket on the surface of H2A (Fig. 6). It will be interesting in future experiments to dissect the contributions of each of these interactions to various states of chromatin structure.
This work was supported by NIH grant GM52426.
Published ahead of print on 10 November 2008. ![]()
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