Intrinsic stiffness and [THETA]-solvent regime in intrinsically disordered proteins: Implications for liquid-liquid phase separation

Liquid-liquid phase separation (LLPS) exhibited by intrinsically disordered proteins (IDPs) depends on the solvation state around the [THETA]-regime, which separates good from poor solvent. Experimentally, the [THETA]-solvent regime of the finite length (N) IDPs, as probed by small angle X-ray scatt...

Full description

Saved in:
Bibliographic Details
Published inPNAS nexus Vol. 4; no. 2
Main Authors Baidya, Lipika, Kremer, Kurt, Reddy, Govardhan
Format Journal Article
LanguageEnglish
Published Oxford University Press 01.02.2025
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:Liquid-liquid phase separation (LLPS) exhibited by intrinsically disordered proteins (IDPs) depends on the solvation state around the [THETA]-regime, which separates good from poor solvent. Experimentally, the [THETA]-solvent regime of the finite length (N) IDPs, as probed by small angle X-ray scattering (SAXS) and single molecular fluorescence resonance energy transfer (smFRET), is in disagreement. Using computer simulations of a coarse-grained IDP model, we address the effect of chain length on the [THETA]-regime of IDPs with polar side chains (polyglutamine) and hydrophobic side chains (polyleucine) subject to varying concentrations of cosolvents [C], urea (denaturant) or trimethylamine N-oxide (protective osmolyte) in water. Due to their intrinsic stiffness, these IDPs are always expanded on short-length scales, independent of the solvent quality. As a result, for short IDP sequences ([approximately equal to]10 to 25 residues), their propensity to exhibit LLPS cannot be inferred from single-chain properties. Further, for finite-size IDPs, the cosolvent concentration to attain the [THETA]-regime ([[C.sub.[THETA]]]) extracted from the structure factor emulating SAXS and pair distances mimicking smFRET differs. They converge to the same cosolvent concentration only at large N, indicating that finite size corrections vary for different; IDP properties. We show that the radius of gyration (Rg) of the IDPs in the [THETA]-solvent regime satisfies the scaling relation Rg = Nf (c N), which can be exploited to accurately extract [[C.sub.[THETA]]] (c = ([C]/[[C.sub.[THETA]]] - 1)). We demonstrate the importance of finite size aspects originating from the chain stiffness and thermal blob size in analyzing IDP properties to identify the [THETA]-solvent regime. Keywords: finite-size effect, molecular dynamics simulations, condensate formation, coil-globule transition, amyloid formation
ISSN:2752-6542
2752-6542
DOI:10.1093/pnasnexus/pgaf039