The intranuclear environment

Self-assembly of promoter DNA and RNA Pol II machinery into transcriptionally active biomolecular condensates

Transcription in the nucleus occurs in a concentrated, dense environment, and no reasonable biochemical facsimile of this milieu exists. Such a biochemical environment would be important for further understanding transcriptional regulation. We describe here the formation of dense, transcriptionally active bodies in vitro with only nuclear extracts and promoter DNA. These biomolecular condensates (BMCs) are 0.5 to 1 μm in diameter, have a macromolecular density of approximately 100 mg/ml, and are a consequence of a phase transition between promoter DNA and nuclear extract proteins. BMCs are physically associated with transcription as any disruption of one compromised the other. The BMCs contain RNA polymerase II and elongation factors, as well as factors necessary for BMC formation in vivo. We suggest that BMCs are representative of the in vivo nuclear environment and a more physiologically relevant manifestation of the preinitiation complex/elongation machinery.

Thermodynamic Study of Interactions of Distamycin A with Chromatin in Rat Liver Nuclei in the Presence of Polyamines

We studied the thermodynamics of melting of isolated rat liver nuclei with different degrees of chromatin condensation determined by the concentration of polyamines (PA) and the solution ionic strength, as well as the effect of the antibiotic distamycin A (DM) on melting. Differential scanning calorimetry (DSC) profiles of nuclear preparations contained three peaks that reflected melting of three main chromatin domains. The number of peaks did not depend on the degree of condensation; however, nuclei with more condensed chromatin had a higher total enthalpy. DM stabilized peaks II and III corresponding to the melting of relaxed and topologically strained DNA, respectively, but destabilized peak I corresponding to the melting of nucleosome core histones. At the saturating concentration (DM/DNA molar ratio = 0.1), DM increased T_m of peaks II and III by ~5°C and decreased T_m of peak I by ~2.5°C. Based on the dependence of ΔH on DM concentration, we established that at low DM/DNA ratio (≤0.03), when DM interacted predominantly with AT-rich DNA regions, the enthalpy of peak II decreased in parallel with the increase in the enthalpy of peak III, which indicated that DM induces structural transitions in the nuclear chromatin associated with the increase in torsional stress in DNA. An increase in free energy under saturation conditions was equal to the change in the free energy of DM interaction with DNA. However, the increase in the enthalpy of melting of the nuclei in the presence of DM was much greater than the enthalpy of titration of nuclei with DM. This indicates a significant increase in the strength of interaction between the two DNA strands apparently due, among other things, to changes in the torsional stress of DNA in the nuclei. Titration of the nuclei with increasing PA concentrations resulted in the decrease in the number of DM-binding sites and the non-monotonous dependence of the enthalpy and entropy contribution to the binding free energy on the PA content. We suggested that the observed differences in the thermodynamic parameters were due to the different width of the minor groove in the nuclear chromatin DNA, which depends on PA concentration.

Differential scanning calorimetric study of antibiotic distamycin A binding with chromatin within isolated rat liver nuclei

CONTEXT

Natural oligopeptide antibiotic distamycin A (Dst) biosynthesized by Streptomyces distallicus is traditionally used in medical practice as an anti-inflammatory and antitumour drug.

OBJECTIVE

Dst was investigated for its effect on the structural components of native chromatin directly within isolated rat liver nuclei in the presence of physiologically significant cations (magnesium or spermine and spermidine).

MATERIALS AND METHODS

Differential scanning calorimetry (DSC) was used to study the Dst action at molar ratio Dst/DNA = 0.1 and 0.15 mM Dst on the melting profile of nuclei suspension in different conditions.

RESULTS

Results showed that the thermodynamic parameters of control nuclei in the presence of polyamines or Mg²⁺were different. The incubation of nuclei with Dst raised transition temperatures of relaxed (peak II) and topologically constrained DNA (peak III) by 6-8 °C and decreased by 2-4 °C that of core-histones (peak I). The total excess transition enthalpy (ΔH_exc) in buffer with polyamines (24.7 kJ/mol DNA nucleotides) increased by1.5 times versus control but in buffer with Mg²⁺, the value of ΔH_exc (35.8 kJ/mol DNA nucleotides) remained unchanged.

CONCLUSIONS

The association of Dst with chromatin in the nucleus weakens histone-DNA contacts and causes additional strengthening of interaction between two complementary DNA chains. Our results contribute towards validation of DSC to test drug ability to modulate chromatin structure in the physiological environment and to clarify the mechanism of these modulations.

Connecting the dots: the effects of macromolecular crowding on cell physiology

The physicochemical properties of cellular environments with a high macromolecular content have been systematically characterized to explain differences observed in the diffusion coefficients, kinetics parameters, and thermodynamic properties of proteins inside and outside of cells. However, much less attention has been given to the effects of macromolecular crowding on cell physiology. Here, we review recent findings that shed some light on the role of crowding in various cellular processes, such as reduction of biochemical activities, structural reorganization of the cytoplasm, cytoplasm fluidity, and cellular dormancy. We conclude by presenting some unresolved problems that require the attention of biophysicists, biochemists, and cell physiologists. Although it is still underappreciated, macromolecular crowding plays a critical role in life as we know it.

Extraction of histone H1 and decondensation of nuclear chromatin with various Mg-dependent organization levels under treatment with polyglutamic acid and distamycin

Chromatin in rat liver nuclei under conditions of low ionic strength (20-25 mM) and [Mg2+] from 2 to 5 mM has a condensed structure (100-200 nm globules) and gives the same CD signal (320-340 nm) at interaction with the antibiotic distamycin A (DM). Reducing [Mg2+] to 1 mM leads to chromatin decondensation to 30 nm structures and increases the CD signal. Poly-L-glutamic acid (PG) at weight ratio PG/DNA = 6 and in the presence of 5 mM Mg2+ extracts only about 1/8 of nuclear histone H1, preserving a condensed chromatin structure. Removal of about 1/4 of H1 at 3 mM Mg2+ leads to chromatin decondensation to 30 nm fibrils. Extraction of about half of histone H1 at [Mg2+] ≤ 2 mM results in chromatin refolding to nucleosome fibrils. PG-decondensation leads to a significant increase in the CD signal. The main H1 extraction occurs in 1-2 min, but at all Mg2+ concentrations the more slowly PG extracted fraction is found comprising 5-7% of nuclear H1. About 25% of leaving nuclear H1 can be extracted by PG in the presence of saturating DM concentration (molar DM/DNA = 0.1). H1 release depends significantly on the PG concentration. However, even at high weight ratio PG/DNA = 30 and DM/DNA = 0.1, about 5-10% of histone H1 remained in the nuclei. Decondensation of chromatin in the nucleus is not always proportional to the yield of extracted histone H1 and is weakened in the presence of positively charged DM or high concentrations of PG. Our results show that the interaction of DM with chromatin depends primarily on chromatin packaging, while PG extraction depends on [Mg2+] supporting this packaging.

The crowded nucleus

The principles that determine the organization of the nucleus have become clearer in recent years, largely because of new insights into polymer, colloid, and soft-matter science. Macromolecules, together with the giant linear polymers that form the chromosomes, are confined at high concentrations within the nuclear envelope and their interactions are influenced strongly by short-range depletion or entropic forces which are negligible in dilute systems, in addition to the more familiar van der Waals, electrostatic, steric, hydrogen bonding, and hydrophobic forces. The studies described in this volume are consistent with the model that this complex and concentrated mixture of macromolecules is maintained in a delicate equilibrium by quite simple although unsuspected physicochemical principles. The sensitivity of this equilibrium to perturbation may underlie the controversies about the existence of a nuclear matrix or scaffold. In this volume, we underline the importance for cell biologists of being familiar with current work in colloid, polymer, soft matter, and nanoscience. This chapter presents a brief background to the aspects of the nucleus that are considered in detail in subsequent chapters.

Changes to cellular water and element content induced by nucleolar stress: investigation by a cryo-correlative nano-imaging approach

The cell is a crowded volume, with estimated mean mass percentage of macromolecules and of water ranging from 7.5 to 45 and 55 to 92.5 %, respectively. However, the concentrations of macromolecules and water at the nanoscale within the various cell compartments are unknown. We recently developed a new approach, correlative cryo-analytical scanning transmission electron microscopy, for mapping the quantity of water within compartments previously shown to display GFP-tagged protein fluorescence on the same ultrathin cryosection. Using energy-dispersive X-ray spectrometry (EDXS), we then identified various elements (C, N, O, P, S, K, Cl, Mg) in these compartments and quantified them in mmol/l. Here, we used this new approach to quantify water and elements in the cytosol, mitochondria, condensed chromatin, nucleoplasm, and nucleolar components of control and stressed cancerous cells. The water content of the control cells was between 60 and 83 % (in the mitochondria and nucleolar fibrillar centers, respectively). Potassium was present at concentrations of 128-462 mmol/l in nucleolar fibrillar centers and condensed chromatin, respectively. The induction of nucleolar stress by treatment with a low dose of actinomycin-D to inhibit rRNA synthesis resulted in both an increase in water content and a decrease in the elements content in all cell compartments. We generated a nanoscale map of water and elements within the cell compartments, providing insight into their changes induced by nucleolar stress.

The dynamic pathway of nuclear RNA in eukaryotes

The passage of mRNA molecules from the site of synthesis, through the nucleoplasm and the nuclear pore, en route to the cytoplasm, might appear straightforward. Nonetheless, several decades of detailed examination of this pathway, from high resolution electron microscopy in fixed specimens, through the development of immuno-detection techniques and fluorescence toolkits, to the current era of live-cell imaging, show this to be an eventful journey. In addition to mRNAs, several species of noncoding RNAs travel and function in the nucleus, some being retained within throughout their lifetime. This review will highlight the nucleoplasmic paths taken by mRNAs and noncoding RNAs in eukaryotic cells with special focus on live-cell data and in concurrence with the biophysical nature of the nucleus.

Simulation of mRNA diffusion in the nuclear environment

A mathematical model is devised to study the diffusion of mRNA in the nucleus from the site of synthesis to a nuclear pore where it is exported to the cytoplasm. This study examines the role that nuclear structure can play in determining the kinetics of export by considering models in which elements of the nuclear skeleton and confinement by chromatin direct the mRNA movement. As a rule, a dense chromatin layer favours rapid export by reducing the effective volume for diffusion. However, it may also result in a heavy tail in the export time distribution because of the low mobility of molecules that accidentally find their way deep into the dense layer. An anisotropic solid-state transport system can also assist export. There exist both an optimal ratio of the anisotropy and an optimal depth of the solid-state transport layer that favour rapid export.