Sequence and Crowding Effects in the Aggregation of a 10-Residue Fragment Derived from Islet Amyloid Polypeptide  Eva Rivera, John Straub, D. Thirumalai 

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Sequence and Crowding Effects in the Aggregation of a 10-Residue Fragment Derived from Islet Amyloid Polypeptide  Eva Rivera, John Straub, D. Thirumalai  Biophysical Journal  Volume 96, Issue 11, Pages 4552-4560 (June 2009) DOI: 10.1016/j.bpj.2009.03.039 Copyright © 2009 Biophysical Society Terms and Conditions

Figure 1 (a) Probability distribution of θ values for the two monomers in the 36-mM simulation. (b) Probability of finding each residue of the hIAPP sequence in a β-strand configuration for the 36-mM simulation. The results are averaged over both monomers. Biophysical Journal 2009 96, 4552-4560DOI: (10.1016/j.bpj.2009.03.039) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 2 (a) Free energy profiles as a function of the center-of-mass distance, RCM, among the hIAPP β-sheet dimer at concentrations of 61.3 mM (black), 36.4 mM (red), and 20.7 M (green). The black dashed lines define the three regions for Cp = 61.3 mM and the red dashed line defines the two regions for Cp = 36.4 mM. (b) Projection of the hIAPP dimer onto the first and second principal component axes at 61.3 mM (left) and 36.4 mM (right). Boxes have been drawn to cluster structures with similar features. (c) The number of backbone hydrogen bonds between the two hIAPP monomers at a particular RCM for Cp = 61.3 mM (left) and Cp = 36.4 mM (right). The free energy profile (red) and the average number of waters within 7 Å of the monomers (blue) has been overlaid on both plots. Biophysical Journal 2009 96, 4552-4560DOI: (10.1016/j.bpj.2009.03.039) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 3 (a) Free energy profiles for separating the hIAPP (red) and rIAPP (black) β-sheet dimers in a 61.3 mM solution (left) and a 36.4 mM solution (right). (b) Contact maps for the hIAPP and rIAPP simulations Cp = 61.3 mM and Cp = 36.4 mM. The x axis represents the residues of the A monomer and the y axis represents residues of the B monomer. Two residues were considered to be in contact if their centers-of-mass were within 6 Å. The scale on the right gives the number of times a particular residue pair was found to be in contact, averaged over 5500 structures. Biophysical Journal 2009 96, 4552-4560DOI: (10.1016/j.bpj.2009.03.039) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 4 Comparison of the structural characteristics for the hIAPP monomers at Cp = 28 mM (bottom), the hIAPP monomers at Cp = 36 mM (middle), and the rIAPP monomers at Cp = 36 mM (top). (a) Number of backbone hydrogen bonds present between the monomers; (b) histogram of the sampled center-of-mass distances for the monomers where the bin size is 1 Å; (c) histogram of the sampled radii of gyration for the monomers where the bin size is 0.5 Å; and (d) the number of contacts between residues of the monomers. Two residues were considered to be in contact if their centers-of-mass were within 6 Å. Biophysical Journal 2009 96, 4552-4560DOI: (10.1016/j.bpj.2009.03.039) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 5 Residue-residue contact map for hIAPP and rIAPP dimers at Cp = 36 mM and Cp = 28 mM. The x axis represents the residues of the A monomer and the y axis represents residues of the B monomer. Two residues were considered to be in contact if their centers-of-mass were within 6 Å. The scale on the right gives the number of times a particular residue pair was found to be in contact, averaged over 10,000 structures. Biophysical Journal 2009 96, 4552-4560DOI: (10.1016/j.bpj.2009.03.039) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 6 (a) Hydrogen bond distance between 1), the amide hydrogen on leucine 27 of monomer A with the carbonyl oxygen on leucine 27 of monomer B (black), and 2), the amide hydrogen on leucine 27 of monomer A with the carbonyl oxygen of valine 26 on monomer B (red). (b) Projection of the rIAPP simulation at Cp = 28 mM onto the first and second principal component axes. (c) (Bottom) Atomic Solvation Parameters solvation free energy for the two rIAPP monomers in the truncated octahedron simulation. (Top) The end-to-end distance of monomer B of rIAPP. Biophysical Journal 2009 96, 4552-4560DOI: (10.1016/j.bpj.2009.03.039) Copyright © 2009 Biophysical Society Terms and Conditions