Jack A. Logan's research while affiliated with Yale University and other places

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Publications (2)


FIG. 3. (a) The vibrational density of states (VDOS) D(ω n ), where ω n is the frequency, of the C α atoms in the HS+HP model at T /ϵ r = 10 −8 for all α and β in Fig. 2. (b) Participation ratio p r (ω n ) plotted versus ω n . The average total nonbonded repulsive potential energy per atom ⟨V r /N⟩ increases from blue to red on a logarithmic scale.
Protein folding as a jamming transition
  • Preprint
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May 2024

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49 Reads

Alex T. Grigas

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Zhuoyi Liu

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Jack A. Logan

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[...]

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Proteins fold to a specific functional conformation with a densely packed hydrophobic core that controls their stability. We develop a geometric, yet all-atom model for proteins that explains the universal core packing fraction of $\phi_c=0.55$ found in experimental measurements. We show that as the hydrophobic interactions increase relative to the temperature, a novel jamming transition occurs when the core packing fraction exceeds $\phi_c$. The model also recapitulates the global structure of proteins since it can accurately refold to native-like structures from partially unfolded states.

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Protein folding as a jamming transition

May 2024

·

7 Reads

Proteins fold to a specific functional conformation with a densely packed hydrophobic core that controls their stability. We develop a geometric, yet all-atom model for proteins that explains the universal core packing fraction of $\phi_c=0.55$ found in experimental measurements. We show that as the hydrophobic interactions increase relative to the temperature, a novel jamming transition occurs when the core packing fraction exceeds $\phi_c$. The model also recapitulates the global structure of proteins since it can accurately refold to native-like structures from partially unfolded states.