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. Author manuscript; available in PMC: 2012 Jul 21.
Published in final edited form as: J Phys Chem C Nanomater Interfaces. 2011 Jul 21;115(28):13775–13785. doi: 10.1021/jp202965h

Figure 10. Local RMSD of a representative structure (Figure 9) relative to the 100 structures with lowest constraint energy.

Figure 10

To show the dispersion among structures, we superimposed the Cα atoms of every overlapping 3mer in the representative structure and each of the 100 structures with lowest Econstraint, and calculated the RMSD of the central Cα atom in the 3mer. The color bar is in angstroms and corresponds to the opaque profile defining LRAP's shape. LRAP pictured from C-terminus (left) to N-terminus (right).