Quantitative analysis of single-molecule force spectroscopy on folded chromatin fibers

Single-molecule techniques allow for picoNewton manipulation and nanometer accuracy measurements of single chromatin fibers. However, the complexity of the data, the heterogeneity of the composition of individual fibers and the relatively large fluctuations in extension of the fibers complicate a structural interpretation of such force-extension curves. Here we introduce a statistical mechanics model that quantitatively describes the extension of individual fibers in response to force on a per nucleosome basis. Four nucleosome conformations can be distinguished when pulling a chromatin fiber apart. A novel, transient conformation is introduced that coexists with single wrapped nucleosomes between 3 and 7 pN. Comparison of force-extension curves between single nucleosomes and chromatin fibers shows that embedding nucleosomes in a fiber stabilizes the nucleosome by 10 k_BT. Chromatin fibers with 20- and 50-bp linker DNA follow a different unfolding pathway. These results have implications for accessibility of DNA in fully folded and partially unwrapped chromatin fibers and are vital for understanding force unfolding experiments on nucleosome arrays.     

Influence of DNA end structure on the mechanism of initiation of DNA unwinding by the Escherichia coli RecBCD and RecBC helicases

Escherichiacoli RecBCD is a bipolar DNA helicase possessing two motor subunits (RecB, a 3′-to-5′ translocase, and RecD, a 5′-to-3′ translocase) that is involved in the major pathway of recombinational repair. Previous studies indicated that the minimal kinetic mechanism needed to describe the ATP-dependent unwinding of blunt-ended DNA by RecBCD in vitro is a sequential n-step mechanism with two to three additional kinetic steps prior to initiating DNA unwinding. Since RecBCD can “melt out” ∼ 6 bp upon binding to the end of a blunt-ended DNA duplex in a Mg²⁺-dependent but ATP-independent reaction, we investigated the effects of noncomplementary single-stranded (ss) DNA tails [3′-(dT)₆ and 5′-(dT)₆ or 5′-(dT)₁₀] on the mechanism of RecBCD and RecBC unwinding of duplex DNA using rapid kinetic methods. As with blunt-ended DNA, RecBCD unwinding of DNA possessing 3′-(dT)₆ and 5′-(dT)₆ noncomplementary ssDNA tails is well described by a sequential n-step mechanism with the same unwinding rate (mk_U = 774 ± 16 bp s^− 1) and kinetic step size (m = 3.3 ± 1.3 bp), yet two to three additional kinetic steps are still required prior to initiation of DNA unwinding (k_C = 45 ± 2 s^− 1). However, when the noncomplementary 5′ ssDNA tail is extended to 10 nt [5′-(dT)₁₀ and 3′-(dT)₆], the DNA end structure for which RecBCD displays optimal binding affinity, the additional kinetic steps are no longer needed, although a slightly slower unwinding rate (mk_U = 538 ± 24 bp s^− 1) is observed with a similar kinetic step size (m = 3.9 ± 0.5 bp). The RecBC DNA helicase (without the RecD subunit) does not initiate unwinding efficiently from a blunt DNA end. However, RecBC does initiate well from a DNA end possessing noncomplementary twin 5′-(dT)₆ and 3′-(dT)₆ tails, and unwinding can be described by a simple uniform n-step sequential scheme, without the need for the additional k_C initiation steps, with a similar kinetic step size (m = 4.4 ± 1.7 bp) and unwinding rate (mk_obs = 396 ± 15 bp s^− 1). These results suggest that the additional kinetic steps with rate constant k_C required for RecBCD to initiate unwinding of blunt-ended and twin (dT)₆-tailed DNA reflect processes needed to engage the RecD motor with the 5′ ssDNA.     

Tetrameric Structure of Centromeric Nucleosomes in Interphase Drosophila Cells

Centromeres, the specialized chromatin structures that are responsible for equal segregation of chromosomes at mitosis, are epigenetically maintained by a centromere-specific histone H3 variant (CenH3). However, the mechanistic basis for centromere maintenance is unknown. We investigated biochemical properties of CenH3 nucleosomes from Drosophila melanogaster cells. Cross-linking of CenH3 nucleosomes identifies heterotypic tetramers containing one copy of CenH3, H2A, H2B, and H4 each. Interphase CenH3 particles display a stable association of approximately 120 DNA base pairs. Purified centromeric nucleosomal arrays have typical “beads-on-a-string” appearance by electron microscopy but appear to resist condensation under physiological conditions. Atomic force microscopy reveals that native CenH3-containing nucleosomes are only half as high as canonical octameric nucleosomes are, confirming that the tetrameric structure detected by cross-linking comprises the entire interphase nucleosome particle. This demonstration of stable half-nucleosomes in vivo provides a possible basis for the instability of centromeric nucleosomes that are deposited in euchromatic regions, which might help maintain centromere identity.     

N-terminal phosphorylation of HP1α increases its nucleosome-binding specificity

Heterochromatin protein 1 (HP1) is an evolutionarily conserved chromosomal protein that binds to lysine 9-methylated histone H3 (H3K9me), a hallmark of heterochromatin. Although HP1 phosphorylation has been described in several organisms, the biological implications of this modification remain largely elusive. Here we show that HP1''s phosphorylation has a critical effect on its nucleosome binding properties. By in vitro phosphorylation assays and conventional chromatography, we demonstrated that casein kinase II (CK2) is the kinase primarily responsible for phosphorylating the N-terminus of human HP1α. Pull-down assays using in vitro-reconstituted nucleosomes showed that unmodified HP1α bound H3K9-methylated and H3K9-unmethylated nucleosomes with comparable affinity, whereas CK2-phosphorylated HP1α showed a high specificity for H3K9me3-modified nucleosomes. Electrophoretic mobility shift assays showed that CK2-mediated phosphorylation diminished HP1α''s intrinsic DNA binding, which contributed to its H3K9me-independent nucleosome binding. CK2-mediated phosphorylation had a similar effect on the nucleosome-binding specificity of fly HP1a and S. pombe Swi6. These results suggested that HP1 phosphorylation has an evolutionarily conserved role in HP1''s recognition of H3K9me-marked nucleosomes.     

Expression of a GABAB - Receptor in Olfactory Sensory Neurons of Sensilla trichodea on the Male Antenna of the Moth Heliothis virescens

In the olfactory pathway of Drosophila, a GABA_B receptor mediated presynaptic gain control mechanism at the first synapse between olfactory sensory neurons (OSNs) and projection neurons has been suggested to play a critical role in setting the sensitivity and detection range of the sensory system. To approach the question if such a mechanism may be realized in the pheromone recognition system of male moths in this study attempts were made to explore if moth''s pheromone-responsive cells express a GABA_B- receptor. Employing a combination of genome analysis, RT-PCR experiments and screening of an antennal cDNA library we have identified a cDNA which encodes the GABA_B-R1 receptor of Heliothis virescens. Moreover, based on the HvirGABA_B-R1 sequence we could predict a GABA_B-R1 protein from genome sequences of the silkmoth Bombyx mori. To assess whether HvirGABA_B-R1 is expressed in OSNs of male antenna we performed whole-mount in situ hybridization (WM-ISH) experiments. Several HvirGABA_B-R1 positive cells were visualized under long sensilla trichodea, known to contain pheromone-responsive OSNs. In parallel it was shown that cells under long trichoid hairs were labelled with pheromone receptor specific probes. In addition, the HvirGABA_B-R1 specific probe also labelled several cells under shorter olfactory sensilla, but never stained cells under mechanosensory/gustatory sensilla chaetica. Together, the results indicate that a GABA_B receptor is expressed in pheromone-responsive OSNs of H. virescens and suggest a presynaptic gain control mechanism in the axon terminals of these cells.     

A critical epitope for substrate recognition by the nucleosome remodeling ATPase ISWI

The ATPase ISWI is the catalytic core of several nucleosome remodeling complexes, which are able to alter histone–DNA interactions within nucleosomes such that the sliding of histone octamers on DNA is facilitated. Dynamic nucleosome repositioning may be involved in the assembly of chromatin with regularly spaced nucleosomes and accessible regulatory sequence elements. The mechanism that underlies nucleosome sliding is largely unresolved. We recently discovered that the N-terminal ‘tail’ of histone H4 is critical for nucleosome remodeling by ISWI. If deleted, nucleosomes are no longer recognized as substrates and do not stimulate the ATPase activity of ISWI. We show here that the H4 tail is part of a more complex recognition epitope which is destroyed by grafting the H4 N-terminus onto other histones. We mapped the H4 tail requirement to a hydrophilic patch consisting of the amino acids R₁₇H₁₈R₁₉ localized at the base of the tail. These residues have been shown earlier to contact nucleosomal DNA, suggesting that ISWI recognizes an ‘epitope’ consisting of the DNA-bound H4 tail. Consistent with this hypothesis, the ISWI ATPase is stimulated by isolated H4 tail peptides ISWI only in the presence of DNA. Acetylation of the adjacent K₁₂ and K₁₆ residues impairs substrate recognition by ISWI.     

Motor-Substrate Interactions in Mycoplasma Motility Explains Non-Arrhenius Temperature Dependence

Mycoplasmas exhibit a novel, substrate-dependent gliding motility that is driven by ∼400 “leg” proteins. The legs interact with the substrate and transmit the forces generated by an assembly of ATPase motors. The velocity of the cell increases linearly by nearly 10-fold over a narrow temperature range of 10-40°C. This corresponds to an Arrhenius factor that decreases from ∼45 k_BT at 10°C to ∼10 k_BT at 40°C. On the other hand, load-velocity curves at different temperatures extrapolate to nearly the same stall force, suggesting a temperature-insensitive force-generation mechanism near stall. In this article, we propose a leg-substrate interaction mechanism that explains the intriguing temperature sensitivity of this motility. The large Arrhenius factor at low temperature comes about from the addition of many smaller energy barriers arising from many substrate-binding sites at the distal end of the leg protein. The Arrhenius dependence attenuates at high temperature due to two factors: 1), the reduced effective multiplicity of energy barriers intrinsic to the multiple-site binding mechanism; and 2), the temperature-sensitive weakly facilitated leg release that curtails the power stroke. The model suggests an explanation for the similar steep, sub-Arrhenius temperature-velocity curves observed in many molecular motors, such as kinesin and myosin, wherein the temperature behavior is dominated not by the catalytic biochemistry, but by the motor-substrate interaction.     

盐离子作用下组蛋白变体H2A.Z增强核小体结构的稳定性

真核生物染色质的基本结构组成单元是核小体,基因组DNA被压缩在染色质中,核小体的存在通常会抑制转录、复制、修复和重组等发生在DNA模板上的生物学过程。组蛋白变体H2A.Z可以调控染色质结构进而影响基因的转录过程,但其详细的调控机制仍未研究清楚。为了比较含有组蛋白变体H2A.Z的核小体和常规核小体在盐离子作用下的稳定性差异,本文采用Förster共振能量转移的方法检测氯化钠、氯化钾、氯化锰、氯化钙、氯化镁等离子对核小体的解聚影响。实验对Widom 601 DNA序列进行双荧光Cy3和Cy5标记,通过荧光信号值的变化来反映核小体的解聚变化。Förster共振能量转移检测结果显示:在氯化钠、氯化钾、氯化锰、氯化钙和氯化镁作用下,含有组蛋白变体H2A.Z的核小体解聚速度相比于常规核小体要慢,且氯化钙、氯化锰和氯化镁的影响更明显。电泳分析结果表明,在75℃条件下含有组蛋白变体H2A.Z的核小体的解聚速率明显低于常规核小体。采用荧光热漂移检测(fluorescence thermal shift analysis , FTS)进一步分析含有组蛋白变体H2A.Z核小体的稳定性,发现两类核小体的荧光信号均呈现2个明显的增长期,含有组蛋白变体H2A.Z核小体的第1个荧光信号增速期所对应的温度明显高于常规核小体,表明核小体中H2A.Z/H2B二聚体的解聚变性温度要高于常规的H2A/H2B二聚体,含有组蛋白变体H2A.Z核小体的热稳定性高。研究结果均表明,含有组蛋白变体H2A.Z的核小体的结构比常规核小体的结构稳定。     

Electron heat transport through the plasma-electrode boundary in weakly ionized plasma

The average electron thermal energies in the emission flux from the electrode into the plasma, ? ₁, and from the plasma toward the electrode, ? ₂, are determined for the cases of large and small values of the coefficient of kinetic reflection. It is shown that these energies vary within the ranges 0.5k _B T _c < ? ₁ < 2k _B T _c and 0.5k _B T _e < ? ₂ < 2k _B T _e , where T _c and T _e are the temperatures of the cathode and plasma electrons, respectively. The obtained values can be used to formulate the boundary conditions for the hydrodynamic equations at the electrode or a dielectric wall.