Biomolecular condensate

Biomolecular condensates are a class of non-membrane bound organelles and organelle subdomains, specified by physical concepts that date back a long way. As with other organelles, biomolecular condensates are specialized subunits of the cell. However, unlike many organelles, biomolecular condensate composition is not controlled by a bounding membrane. Instead they can form through a range of different processes, the most well-known of which is phase separation of proteins, RNA and other biopolymers into either colloidal emulsions, liquid crystals, solid crystals or aggregates within cells.
History.
Micellar theory.
The micellar theory of Carl Nägeli was developed from his detailed study of starch granules in 1858. Amorphous substances such as starch and cellulose were proposed to consist of building blocks, packed in a loosely crystalline array to form which he later termed “micelles”. Water could penetrate between the micelles, and new micelles could form in the interstices between old micelles. The swelling of starch grains and their growth was described by a molecular-aggregate model, which he also applied to the cellulose of the plant cell wall. The modern usage of 'micelle' refers strictly to lipids, but its original usage clearly extended to other types of biomolecule, and this legacy is reflected to this day in the description of milk as being composed of 'casein micelles'.
Colloidal phase separation theory.
The term 'colloid' was coined by Wolfgang Ostwald and defined by Thomas Graham in 1861 to describe the behaviour of certain biological macromolecules (starch, albumin, gelatin, etc) and inorganic molecules as slowly diffusing components of cloudy liquid solution-suspensions that were blocked by semi-permeable membranes, while the physics of phase separation was described by Josiah Willard Gibbs in his landmark paper titled "On the Equilibrium of Heterogeneous Substances", published in parts between 1875 and 1878. Influenced by Willard Gibbs, important contributions were also made by Johannes Diderik van der Waals, who in 1890 published a treatise on the "Theory of Binary Solutions".
The concept of intracellular colloids as an organizing principle for the compartmentalization of living cells dates back to the end of the 19th century, beginning with William Bate Hardy and Edmund Beecher Wilson who described the cytoplasm (then called 'protoplasm') as a colloid. Around the same time, Thomas Harrison Montgomery Jr. described the morphology of the nucleolus, an organelle within the nucleus, which has subsequently been shown to form through intracellular phase separation. WB Hardy linked formation of biological colloids with phase separation in his study of globulins, stating that: "The globulin is dispersed in the solvent as particles which are the colloid particles and which are so large as to form an internal phase", and further contributed to the basic physical description of oil-water phase separation. 
Colloidal phase separation as a driving force in cellular organisation appealed strongly to Stephane Leduc, who wrote in his influential 1911 book "The Mechanism of Life": "Hence the study of life may be best begun by the study of those physico-chemical phenomena which result from the contact of two different liquids. Biology is thus but a branch of the physico-chemistry of liquids; it includes the study of electrolytic and colloidal solutions, and of the molecular forces brought into play by solution, osmosis, diffusion, cohesion, and crystallization." 
The primordial soup theory of the origin of life, proposed by Alexander Oparin in Russian in 1924 (published in English in 1936) and by J.B.S. Haldane in 1929, suggested that life was preceded by the formation of what Haldane called a "hot dilute soup" of "colloidal organic substances", and which Oparin referred to as 'coacervates' (after de Jong ) - particles composed of two or more colloids which might be protein, lipid or nucleic acid. These ideas strongly influenced the subsequent work of Sidney W. Fox on proteinoid microspheres.
Molecular biology.
In 1922, Hermann Staudinger refined the colloidal association theory of Thomas Graham by proposing that certain colloids were composed of high molecular weight polymers (chains linked by covalent bonds), which he termed 'macromolecules' to distinguish them from colloidal clusters of lower molecular weight molecules. So strongly held was colloidal association theory that even Emil Fischer, who had concluded that proteins are polypeptides formed by covalent bonds between amino acid units in 1906, initially refused to believe in the existence of high molecular weight polymers. Staudinger eventually received the Nobel Prize in 1953. Importantly, the discovery of high molecular weight macromolecular polymers cast doubt on the universality of colloidal phase separation in biology, despite the fact that individual polymers could still be observed to associate by clustering and phase separation to form colloids, liquid crystals, solid crystals or aggregates. 
A far greater impact occurred when Frederick Sanger determined the amino acid sequence of Insulin and Linus Pauling, Robert Corey and Herman Branson correctly proposed the alpha helix and beta sheet as the primary structural motifs in protein secondary structure, while Max Perutz and John Kendrew analysed the 3D structure of myoglobin and later haemoglobin. These breakthroughs in protein structure determination led to a general focus of biologists on atomic-scale amino acid sequence- and 3D conformation-specific protein-protein interactions of a lock and key model type, usually between defined numbers of interacting subunits within a stoichiometric complex. Together with Staudinger's Nobel Prize in 1953 this new approach led to a reduced interest in biopolymers as colloids in biology, apart from their propensity to form solid crystals for structure determination by X-ray crystallography. Nevertheless, the fields of colloid chemistry and polymer physics continued unabated to characterise the non-stoichiometric interactions occurring during colloidal, liquid crystal and other phase behaviour of macromolecular polymers, particularly synthetic polymers developed for industrial applications.
Support from other disciplines.
When cell biologists largely abandoned colloidal phase separation, it was left to relative outsiders - agricultural scientists and physicists - to make further progress in the study of phase separating biomolecules in cells.
Beginning in the early 1970s, Harold M Farrell Jr. at the US Department of Agriculture developed a colloidal phase separation model for milk casein micelles that form within mammary gland cells before secretion as milk.
Also in the 1970s, physicists Tanaka & Benedek at MIT identified phase-separation behaviour of gamma-crystallin proteins from lens epithelial cells and cataracts in solution, which Benedek referred to as 'protein condensation'. 
In the 1980s and 1990s, Athene Donald's polymer physics lab in Cambridge extensively characterised phase transitions / phase separation of starch granules from the cytoplasm of plant cells, which behave as liquid crystals.
In 1991, Pierre-Gilles de Gennes received the Nobel Prize in Physics for developing a generalized theory of phase transitions with particular applications to describing ordering and phase transitions in polymers. Unfortunately, de Gennes wrote in "Nature" that polymers should be distinguished from other types of colloids, even though they can display similar clustering and phase separation behaviour, a stance that has been reflected in the reduced usage of the term colloid to describe the higher-order association behaviour of biopolymers in modern cell biology and molecular self-assembly.
Phase separation revisited.
Advances in confocal microscopy at the end of the 20th century identified proteins, RNA or carbohydrates localising to many non-membrane bound cellular compartments within the cytoplasm or nucleus which were variously referred to as 'puncta/dots', 'signalosomes', 'granules', 'bodies', 'assemblies', 'paraspeckles', 'purinosomes', 'inclusions', 'aggregates' or 'factories'. During this time period (1995-2008) the concept of phase separation was re-borrowed from colloidal chemistry & polymer physics and proposed to underlie both cytoplasmic and nuclear compartmentalization.
Since 2009, further evidence for biomacromolecules undergoing intracellular phase transitions (phase separation) has been observed in many different contexts, both within cells and in reconstituted "in vitro" experiments.
The newly coined term "biomolecular condensate" refers to biological polymers (as opposed to synthetic polymers) that undergo self assembly via clustering to increase the local concentration of the assembling components, and is analogous to the physical definition of condensation. 
In physics, condensation typically refers to a gas-liquid phase transition. 
In biology the term 'condensation' is used much more broadly and can also refer to liquid-liquid phase separation to form colloidal emulsions or liquid crystals within cells, and liquid-solid phase separation to form gels, sols, or suspensions within cells as well as liquid-to-solid phase transitions such as DNA condensation during prophase of the cell cycle or protein condensation of crystallins in cataracts. With this in mind, the term 'biomolecular condensates' was deliberately introduced to reflect this breadth (see below). Since biomolecular condensation generally involves oligomeric or polymeric interactions between an indefinite number of components, it is generally considered distinct from formation of smaller stoichiometric protein complexes with defined numbers of subunits, such as viral capsids or the proteasome - although both are examples of spontaneous molecular self-assembly or self-organisation. 
Mechanistically, it appears that the conformational landscape (in particular, whether it is enriched in extended disordered states) and multivalent interactions between intrinsically disordered proteins (including cross-beta polymerisation), and/or protein domains that induce head-to-tail oligomeric or polymeric clustering, might play a role in phase separation of proteins.
Examples.
Many examples of biomolecular condensates have been characterized in the cytoplasm and the nucleus that are thought to arise by either liquid-liquid or liquid-solid phase separation.
Nuclear condensates.
Other nuclear structures including heterochromatin and DNA condensation in condensed mitosis chromosomes form by mechanisms similar to phase separation, so can also be classified as biomolecular condensates.
Lipid enclosed organelles and lipoproteins are not considered condensates.
Typical organelles or endosomes enclosed by a lipid bilayer are not considered biomolecular condensates. In addition, lipid droplets are surrounded by a lipid monolayer in the cytoplasm, or in milk, or in tears, so appear to fall under the 'membrane bound' category. Finally, secreted LDL and HDL lipoprotein particles are also enclosed by a lipid monolayer. The formation of these structures involves phase separation to from colloidal micelles or liquid crystal bilayers, but they are not classified as biomolecular condensates, as this term is reserved for non-membrane bound organelles.
Liquid-liquid phase separation (LLPS) in biology.
Liquid biomolecular condensates.
Liquid-liquid phase separation (LLPS) generates a subtype of colloid known as an emulsion that can coalesce to from large droplets within a liquid. Ordering of molecules during liquid-liquid phase separation can generate liquid crystals rather than emulsions. In cells, LLPS produces a liquid subclass of biomolecular condensate that can behave as either an emulsion or liquid crystal.
The term biomolecular condensates was introduced in the context of intracellular assemblies as a convenient and non-exclusionary term to describe non-stoichiometric assemblies of biomolecules. The choice of language here is specific and important. It has been proposed that many biomolecular condensates form through liquid-liquid phase separation (LLPS) to form colloidal emulsions or liquid crystals in living organisms, as opposed to liquid-solid phase separation to form crystals/aggregates in gels, sols or suspensions within cells or extracellular secretions. However, unequivocally demonstrating that a cellular body forms through liquid-liquid phase separation is challenging, because different material states (liquid vs. gel vs. solid) are not always easy to distinguish in living cells. The term "biomolecular condensate" directly addresses this challenge by making no assumption regarding either the physical mechanism through which assembly is achieved, nor the material state of the resulting assembly. Consequently, cellular bodies that form through liquid-liquid phase separation are a subset of biomolecular condensates, as are those where the physical origins of assembly are unknown. Historically, many cellular non-membrane bound compartments identified microscopically fall under the broad umbrella of biomolecular condensates. 
In physics, phase separation can be classified into the following types of colloid, of which biomolecular condensates are one example:
In biology, the most relevant forms of phase separation are either liquid-liquid or liquid-solid, although there have been reports of gas vesicles surrounded by a phase separated protein coat in the cytoplasm of some microorganisms.
Wnt signalling.
One of the first discovered examples of a highly dynamic intracellular liquid biomolecular condensate with a clear physiological function were the supramolecular complexes (Wnt signalosomes) formed by components of the Wnt signaling pathway. The Dishevelled (Dsh or Dvl) protein undergoes clustering in the cytoplasm via its DIX domain, which mediates protein clustering (polymerisation) and phase separation, and is important for signal transduction. The Dsh protein functions both in planar polarity and Wnt signalling, where it recruits another supramolecular complex (the Axin complex) to Wnt receptors at the plasma membrane. The formation of these Dishevelled and Axin containing droplets is conserved across metazoans, including in "Drosophila", "Xenopus", and human cells.
P granules.
Another example of liquid droplets in cells are the germline P granules in "Caenorhabditis elegans". These granules separate out from the cytoplasm and form droplets, as oil does from water. Both the granules and the surrounding cytoplasm are liquid in the sense that they flow in response to forces, and two of the granules can coalesce when they come in contact. When (some of) the molecules in the granules are studied (via fluorescence recovery after photobleaching), they are found to rapidly turnover in the droplets, meaning that molecules diffuse into and out of the granules, just as expected in a liquid droplet. The droplets can also grow to be many molecules across (micrometres) Studies of droplets of the "Caenorhabditis elegans" protein LAF-1 "in vitro" also show liquid-like behaviour, with an apparent viscosity formula_1Pa s. This is about a ten thousand times that of water at room temperature, but it is small enough to enable the LAF-1 droplets to flow like a liquid. Generally, interaction strength (affinity) and valence (number of binding sites) of the phase separating biomolecules influence their condensates viscosity, as well as their overall tendency to phase separate.