Interaction
strength and localization are critical parameters
controlling
the single-chain and condensed-state properties of intrinsically disordered
proteins (IDPs). Here, we decipher these relationships using coarse-grained
heteropolymers comprised of hydrophobic (H) and polar (P) monomers
as model IDPs. We systematically vary the fraction of P monomers X
P and employ two distinct particle-based models
that include either strong localized attractions between only H–H
pairs (HP model) or weak distributed attractions between both H–H
and H–P pairs (HP+ model). To compare different sequences and
models, we first carefully tune the attraction strength for all sequences
to match the single-chain radius of gyration. Interestingly, we find
that this procedure produces similar conformational ensembles, nonbonded
potential energies, and chain-level dynamics for single chains of
almost all sequences in both models, with some deviations for the
HP model at large X
P. However, we observe
a surprisingly rich phase behavior for the sequences in both models
that deviates from the expectation that similarity at the single-chain
level will translate to a similar phase-separation propensity. Coexistence
between dilute and dense phases is only observed up to a model-dependent X
P, despite the presence of favorable interchain
interactions, which we quantify using the second virial coefficient.
Instead, the limited number of attractive sites (H monomers) leads
to the self-assembly of finite-sized clusters of different sizes depending
on X
P. Our findings strongly suggest that
models with distributed interactions favor the formation of liquid-like
condensates over a much larger range of sequence compositions compared
to models with localized interactions.