2022
DOI: 10.1101/2022.03.30.486367
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Protein structural transitions critically transform the network connectivity and viscoelasticity of RNA-binding protein condensates but RNA can prevent it

Abstract: Biomolecular condensates, some of which are liquid-like during health, can age over time becoming gel-like pathological systems. Ageing of RNA-binding protein condensates can emerge from the progressive accumulation of inter-protein β-sheets. To bridge microscopic understanding of such time-dependent transformation with the modulation of FUS and hnRNPA1 condensate viscoelasticity, we develop a multiscale simulation approach. Our method integrates atomistic simulations with sequence-dependent coarse-grained mod… Show more

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Cited by 2 publications
(16 citation statements)
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“…Furthermore, LARKS abundance is also critical for controlling droplet densification upon maturation, where the relative increase in density is 2.5 times higher from 1-LARKS to 3-LARKS low-complexity domains. These results are consistent with previous in silico observations for FUS-LCD and A1-LCD-hnRNPA1 aged condensates, where the higher concentration of LARKS within the FUS-LCD sequence led to higher densification upon maturation compared to A1-LCD-hnRNPA1 droplets 31 . Recently, FUS-LCD ageing-driven densification through β -sheet aggregation has been confirmed 11,65 .…”
Section: Resultssupporting
confidence: 93%
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“…Furthermore, LARKS abundance is also critical for controlling droplet densification upon maturation, where the relative increase in density is 2.5 times higher from 1-LARKS to 3-LARKS low-complexity domains. These results are consistent with previous in silico observations for FUS-LCD and A1-LCD-hnRNPA1 aged condensates, where the higher concentration of LARKS within the FUS-LCD sequence led to higher densification upon maturation compared to A1-LCD-hnRNPA1 droplets 31 . Recently, FUS-LCD ageing-driven densification through β -sheet aggregation has been confirmed 11,65 .…”
Section: Resultssupporting
confidence: 93%
“…Furthermore, as reported in Fig. 1(b), the relatively high interaction strengths among structured LARKS that we obtain here for TDP-43 are also consistent with all-atom PMF calculations for NUP-98 55 , hnRNPA1 31 and FUS 32 , previously reported by us. For all these proteins, a dramatic increase in binding energy from the disordered state (where interaction energies typically correspond to 3-8 k B T per peptide, suggesting that thermal fluctuations can easily break them) is observed upon the formation of the canonical β -sheet stacking (~30-45 k B T of interaction per peptide).…”
Section: Resultssupporting
confidence: 92%
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