Skip to main content
. 2005 Aug;14(8):2095–2102. doi: 10.1110/ps.051577605

Table 1.

Structure statistics for AAH26994.1

RMSD (Å) with respect to mean:
    Heavy backbone atoms (residues 4–98) 0.55 ± 0.11
    All heavy atoms (residues 4–98) 1.22 ± 0.19
No. of experimental restraints
    Intra-residue NOEs 1039
    Inter-residue sequential NOEs (|i–j| = 1) 296
    Inter-residue medium range NOEs (1<|i–j|<5) 655
    Inter-residue long range NOEs (|i–j|>4) 229
    Total NOEs 2219
    Dihedral angle restraints 96
    H-bond restraints 46
Restraint violationsa
    NOE distances with violations >0.3 Å 3.2 ± 0.9
    Dihedrals with violations >3° 1.07 ± 0.17
RMSD for experimental restraintsb
    All distance restraints (2315) (Å) 0.037 ± 0.008
    Torsion angles (96) (°) 1.07 ± 0.17
CNS energies from SAc
    Fvdw (kcal mol−1) −950 ± 32
    Felec (kcal mol−11)d −3610 ± 102
RMSD (Å) from idealized covalent geometry
    Bonds (°) 0.0045 ± 0.00
    Angles (°) 0.62 ± 0.02
    Impropers (°) 1.76 ± 0.07
Ramachandran analysis (residues 1–101)
    Residues in the favored region (%) 75.0
    Residues in additional allowed regions (%) 18.5
    Residues in generously allowed regions (%) 3.72
    Residues in disallowed regions (%) 2.8

Based on the 20 best structures and obtained by simulated annealing in CNS followed by refinement in explicit water using NOE distance restraints, dihedral angle restraints, bonds, angles, impropers, dihedral angle, van der Waals, and electrostatic energy terms.

aNo distances were violated by >0.5 Å, and no dihedral angle restraints were violated by >5°.

b The number of each class of experimental restraints is given in parentheses.

c Force constants were described in Materials and Methods.

d The Lennard-Jones 6–12 and coulomb energy terms were calculated within CNS using the OPLS nonbonded parameters (as described in Materials and Methods).