Cell Biology · Unit 2: Membranes and compartments
Nuclear Architecture and Membraneless Compartments
The nucleus has no internal membranes, yet its chromosomes keep to their own regions and its nucleoplasm holds bodies with different jobs. This lesson describes chromosome territories and the two Hi-C compartments, the nucleolus and its smaller neighbours, and the proposal that many such bodies form by phase separation. Afterwards you can state what phase separation predicts, work a mass-balance test on concentration data, and say why round shapes, FRAP and hexanediol do not settle the mechanism.
Watch first Change the Amount, Watch the Bodies · 2:58
A human nucleus is only several micrometres across and holds roughly two metres of DNA, but it has no membranes inside it, and it is still not a uniform soup. Chromosomes keep to their own regions. Ribosomes are assembled in one place, splicing factors gather in others. So what holds things apart when there are no walls? This lesson separates the parts of that answer that are well supported from the parts that are still argued over.
Chromosomes keep to territories, mostly
During mitosis each chromosome is a compact rod. Afterwards it partly unpacks, but it does not spread through the whole nucleus. When whole chromosomes are labelled with fluorescent DNA probes, a method called chromosome painting, each one fills a region of its own, a chromosome territory. The DNA is packed as chromatin, DNA wound on histone proteins, and how tightly it is packed affects whether its genes are used, a topic covered in that lesson.
Picture balls of yarn packed in a box. Each ball keeps its own space, but where two balls press together, loose loops of one poke into the other. Whether territories really work that way was hard to see, because a light microscope blurs everything below a few hundred nanometres, as explained in that lesson. In 2006 Miguel Branco and Ana Pombo cut fixed human lymphocytes, activated with phytohemagglutinin, into frozen sections about 150 nm thick before painting them. The thin section removes most of the blur from above and below. Neighbouring territories overlapped at their edges, and how much two chromosomes overlapped correlated with how often that pair takes part in translocations measured in human lymphocytes after ex vivo irradiation. That is a correlation, not proof that overlap causes any given translocation.
A second view comes from Hi-C, a sequencing method. Chromatin is cross-linked in the cell, cut, and the ends are joined so that segments lying close in space become joined in one DNA molecule. Sequencing millions of these junctions gives a map of which parts of the genome touch. The 2009 Hi-C maps of human cells, at a resolution of one megabase, showed that open and closed chromatin segregate into two genome-wide compartments, now called A (open, gene-rich, mostly active) and B (closed, mostly quiet). Closed chromatin often lies against the nuclear lamina, the protein mesh under the nuclear envelope described in that lesson. Remember that Hi-C averages over millions of cells: it reports how often two regions are near each other, not where they sit in one nucleus.
Bodies without membranes: the nucleolus and its neighbours
A nuclear body is a region of the nucleoplasm where particular molecules are concentrated, with no membrane around it. The largest is the nucleolus, whose main job is ribosome biogenesis. It forms around the repeated genes for ribosomal RNA and has three parts, like an assembly line read from the inside out. The fibrillar centre holds the rDNA and the RNA polymerase I machinery. The dense fibrillar component around it, rich in fibrillarin, is where the newly made pre-rRNA begins to be processed. The outer granular component, rich in nucleophosmin (NPM1), is where ribosomal subunits are assembled before export. In nucleoli of Xenopus laevis oocytes, the fibrillarin-rich and NPM1-rich layers behave as two liquids that coexist without mixing.
Smaller bodies sit in the nucleoplasm around it. You can learn them by what they hold.
- Nuclear speckles are enriched in pre-mRNA splicing factors. Immunofluorescence usually shows about 20 to 50 per nucleus in mammalian cells, and their contents exchange with the surrounding nucleoplasm. In mouse embryonic stem cells, genes near speckles showed more co-transcriptional splicing than genes farther away, and in human HEK293T cells, tethering a reporter pre-mRNA to speckles increased its splicing. Splicing itself is covered in that lesson.
- Cajal bodies are marked by the protein coilin and contain components of the small nuclear ribonucleoproteins (snRNPs) that splice pre-mRNA. In an engineered mammalian cell system, tethering Cajal-body components to chromatin was enough to start apparently functional Cajal bodies from scratch.
- PML bodies are built from the PML protein. In cultured mammalian cells and mouse experiments, oxidation drove PML to multimerize and nucleate the bodies, which then enhanced stress-induced SUMO modification of partner proteins held inside them. The name comes from promyelocytic leukaemia, in which a fusion of PML with a retinoic acid receptor is associated with disrupted bodies.
- Paraspeckles are built on a long noncoding RNA, NEAT1. Mice lacking Neat1 have no paraspeckles yet were reported viable and fertile in the laboratory. Later work found milder defects, in pregnancy and lactation, so the bodies are not needed for survival under those conditions, which is not the same as doing nothing.
These facts are well supported: the bodies exist, they exchange molecules with the nucleoplasm, and several of them help with a job. How they form is a different question.
The phase-separation hypothesis and what it predicts
A biomolecular condensate is a membraneless body that concentrates proteins and nucleic acids. One proposed way to make one is liquid-liquid phase separation: above a certain concentration, a solution of molecules demixes into a dense phase and a dilute phase, as salad dressing separates into oil and vinegar. For proteins the driving force is thought to be multivalency, molecules with many weak binding sites (repeated domains, disordered regions, RNA) that stick to many partners at once. These are the weak, reversible bonds described in that lesson. The idea took hold after Brangwynne, Hyman and colleagues reported in 2009 that P granules in the one-cell embryo of the worm C. elegans fuse, flow and drip like liquid drops.
Phase separation is one way to make a local high concentration, not the only one. A protein can bind clustered sites, many copies of a DNA or RNA sequence in one place, and pile up there with no demixing. A protein can also bridge chromatin, cross-linking distant segments so the fibre collapses into a dense globule. All three make a bright spot in a microscope. They differ in what happens when you change the amount of protein.
Phase separation predicts three things. There is a threshold, the saturation concentration, below which no bodies form. Above it, the dilute phase is buffered: extra protein goes into the bodies, which grow, while the concentration outside stays at the threshold. And there is a boundary, so molecules should mix inside a body faster than they cross its edge. A simple mass balance turns the second prediction into numbers.
- Dilute phase
- Dense phase
- Bodies fill (φ)
An idealized model, in this sketch: one dense phase at 50 μM, a saturation concentration of 1 μM, a dilute phase held at that value, and made-up data. The number and places of the dots are arbitrary, only their total area means anything. Binding to clustered sites or bridging chromatin can also make bright spots, and a protein that fails this test may still phase separate as one part of a mixture of several components. A protein that passes has not been shown to need the body for any function. Keep the rule φ = (c_total − c_sat) / (c_dense − c_sat).
c_total = c_sat × (1 − φ) + c_dense × φ, so φ = (c_total − c_sat) / (c_dense − c_sat)
Here φ is the fraction of nuclear volume taken up by the dense phase.
Worked problem (made-up data, for illustration). A GFP-tagged nuclear protein is expressed in a cell line at total nuclear concentrations of 2, 4 and 8 μM. Assume one dense phase at 50 μM, a saturation concentration of 1 μM, and a dilute phase held at that value.
- The denominator is c_dense − c_sat = 50 − 1 = 49 μM.
- At 2 μM, φ = (2 − 1)/49 = 1/49 = 0.020, so bodies fill 2.0% of the nucleus. At 4 μM, φ = 3/49 = 6.1%. At 8 μM, φ = 7/49 = 14.3%.
- So the model predicts that the bodies grow sevenfold in volume between 2 and 8 μM while the nucleoplasm stays near 1 μM.
- Now compare two proteins. For protein A, the measured nucleoplasm is 1.0, 1.0 and 1.1 μM: it fits. For protein B it is 1.5, 2.8 and 5.9 μM. Divide by the totals: 1.5/2 = 0.75, 2.8/4 = 0.70, 5.9/8 = 0.74. Protein B keeps a roughly constant fraction outside the bodies, which fits partitioning onto binding sites better.
Treat the result with care. A protein that fails this test may still phase separate as one part of a mixture of several components, which need not buffer each one. A protein that passes has not been shown to need the body for any function.
Evidence that is not enough: round shapes, fusion, FRAP, hexanediol
Many early claims rested on three observations, and none of them separates the models. Round shapes and fusion arise for any soft body pulled by surface forces, and clusters on chromatin can look the same. FRAP, recovery of fluorescence after photobleaching (see that lesson), measures turnover: molecules that bind and unbind fixed sites also refill a bleached spot. And 1,6-hexanediol, an alcohol thought to weaken hydrophobic contacts, at 5% for 5 minutes strongly suppressed chromatin motion in live HeLa cells. A body that dissolves in it has not been shown to be a liquid.
Heterochromatin shows why the system matters. Purified Drosophila HP1a demixed in the test tube, and HP1a foci in early Drosophila embryos looked liquid-like, with mature domains proposed to contain liquid and stable parts. In mouse fibroblasts, by contrast, chromocentres behaved like collapsed chromatin globules rather than HP1 liquid pools. Purified mouse HP1α mixed with DNA turned turbid at midpoints of 45 μM untagged and 23 μM with a GFP tag. Those are test-tube numbers, not saturation concentrations in a cell, and they show that the tag alone can shift the result. Neither study speaks for all heterochromatin.
The threshold test has its own catch. In engineered Corelet experiments in living cells, local capture of a protein on a seed triggered phase separation below the global concentration needed for it, so a body on chromatin can form where the average level looks too low.
What is contested, then, is whether phase separation is the mechanism for a given body in a given living cell, and whether its material state matters for its job.
Design problem
A laboratory reports that protein X forms round nuclear foci that fuse, recover after photobleaching and dissolve in 1,6-hexanediol. It concludes that X drives a phase separation needed for transcription. What is wrong with the argument, and what would you do instead?
One way to do it
None of the three observations is diagnostic. Roundness, fusion and FRAP recovery also fit binding to clustered sites or chromatin bridging. Hexanediol at 5% for 5 minutes suppresses chromatin motion in live HeLa cells. In that system, Cajal-body foci fell from 2.98 to 0.84 per cell, a drop of (2.98 − 0.84)/2.98 = 2.14/2.98 = 71.8%, yet that drop says nothing about mechanism.
Instead, tag X at its endogenous locus so its level is normal. Raise and lower that level and measure concentrations inside and outside the foci, testing for a threshold and a buffered dilute phase as in the worked problem. Use half-body FRAP to ask whether X mixes inside a focus faster than it crosses the edge. Make a mutant that keeps DNA binding but loses its multivalent region, and see whether foci and transcription change together. Finally, test transcription separately from assembly, with a control that moves the same genes to or from the foci by another route, as Bhat and colleagues did for splicing at speckles. Only then can you ask whether the foci themselves, rather than protein X alone, are needed.
How we measure it
Cryo-FISH with chromosome paints
Fixed cells are cut into thin frozen sections, about 150 nm in the Branco and Pombo work, and whole chromosomes are labelled with fluorescent DNA probes. The thin section removes most out-of-focus light, so overlap between two territories can be measured rather than blurred.
Hi-C
Chromatin is cross-linked in the cell, cut, and re-joined so that segments close in space are ligated together, then the junctions are sequenced. The result is a genome-wide map of contact frequencies averaged over many cells, from which open and closed compartments can be read.
Half-body FRAP
Fluorescence is bleached in one half of a nuclear body and recovery is followed in both halves and in the surrounding nucleoplasm. Whether molecules refill the bleached half mainly from the other half or from outside tells internal mixing apart from exchange across the edge.
Concentration titration with endogenous tagging
The protein is tagged at its own genomic locus, then its level is raised or lowered, for example by inducible expression or induced degradation. Measuring concentrations inside and outside the bodies at each level tests whether there is a threshold and a buffered dilute phase.
Finish line
Test yourself
8 questions
Practice and MCAT-style, with explained answers.
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