Stoichiometric versus stochastic interaction in models of liquid-liquid phase separation.
Stoichiometric versus stochastic interaction in models of liquid-liquid phase separation.
复制标题
液-液相分离模型中的化学计量与随机相互作用。
DOI:
10.1016/j.bpj.2021.12.008
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发表时间:
2022
影响因子:
3.4
通讯作者:
Ghosh,Kingshuk
中科院分区:
文献类型:
--
作者:
Ghosh,Kingshuk
Under appropriate temperature and concentration conditions, chargeneutral homopolymer solutions can segregate into two distinct phases: a polymer-dilute (solvent-rich) and a polymer-dense phase (1, 2). This phenomenon, known as liquid-liquid phase separation (LLPS), is widespread in hetero-polymeric protein solutions as well. The LLPS of folded proteins has been well known for many decades (3, 4). In contrast, the LLPS of newly found classes of proteins that do not fold into unique ‘‘native’’structures, intrinsically disordered proteins (IDPs) or proteins with intrinsically disordered regions (IDRs), has been reported only in the last decade. Although recently discovered, there is growing interest in LLPS of IDPs and IDRs due to their critical role in a multitude of biological processes including the formation of membraneless organelles (5). In many instances, the presence of only lowcomplexity domains in the participating proteins is sufficient for the solution system to undergo phase separation. However, inside a cell, phase separation is often multicomponent, involving different IDP or IDR sequences and often RNA as well. Complexation between different biomolecules near the infinitely dilute limit, far from the solution behavior described above, is another example of multicomponent phenomena that dictate biological function. Complexation is well known to take place between two types of folded proteins or between a disordered and a folded protein, and it has been recently reported that two types of disordered proteins can also form a disordered complex (6). Complexation between two oppositely charged synthetic polymers is well known and a topic of active interest in materials science applications (7, 8) as well. A defining feature of complexation between two types (A and B) of molecules is adherence to a fixed stoichiometry; for example, m number of A and n number of B molecules can form a complex AmBn. Given the preponderance of complexation and LLPS in biology, it is likely that a two-component biopolymer system in solution (three component including the solvent) can undergo both complexation and LLPS (at higher concentration). How do we bridge the two regimes and couple the two different processes? Lin, Chan, and colleagues provide a deeply insightful discussion of this problem by combining mathematical modeling and experiments (9). The richness and the difficulty of the problem can be appreciated by recognizing the sets of all allowed interactions. The LLPS of a two-component (A and B) biopolymer system is typically driven by homotypic (A À A, B À B) and heterotypic (A À B) interactions, in addition to polymer-solvent interactions. When A and B are both IDPs or IDRs, the interactions are typically labile or ‘‘stochastic,’’primarily due to substantial disorder and conformational fluctuations. However, if A and B form complexes, an additional component (complexed molecules, ie, AmBn) arises. Complexes are typically expected to lose substantial conformational entropy, limiting the ability to form ‘‘stochastic’’interactions between two complexes. Consequently, complexes may interact in a more ‘‘specific’’manner. How do these two types of interactions—specific versus stochastic—dictate LLPS? Do stoichiometric complexes form first and subsequently interact in a specific manner to drive LLPS? Or does the process of LLPS involve both ‘‘specific’’and ‘‘nonspecific or stochastic’’interactions?The article (9) by Lin et al. answers these fundamental questions by studying the model system of two proteins, Syn-Gap and PSD-95, that complex with a 3: 2 stoichiometry and serve as the simplest model of postsynaptic densities (PSD). Previous …