Table 1

MOLPROBITY analysis of glut1 homology models

WTGly286AspΔIle4351SUK
Clashscore* (percentile16.58 (49th) 17.65 (44th) 15.54 (55th) 75.37 (0) 
Poor rotamers, % 2.03 1.52 2.54 5.58 
Ramachandran outliers, % 0.00 0.00 0.00 1.84 
Ramachandran favored, % 95.93 96.36 97.00 88.98 
Cβ deviations > 0.25Å 20 21 17 27 
MolProbity score (percentile§2.23 (55th) 2.13 (64th) 2.18 (60th) 3.49 (2nd) 
Residues with bad bonds, % 0.00 0.00 0.00 1.42 
Residues with bad angles, % 0.21 0.43 0.21 3.25 
WTGly286AspΔIle4351SUK
Clashscore* (percentile16.58 (49th) 17.65 (44th) 15.54 (55th) 75.37 (0) 
Poor rotamers, % 2.03 1.52 2.54 5.58 
Ramachandran outliers, % 0.00 0.00 0.00 1.84 
Ramachandran favored, % 95.93 96.36 97.00 88.98 
Cβ deviations > 0.25Å 20 21 17 27 
MolProbity score (percentile§2.23 (55th) 2.13 (64th) 2.18 (60th) 3.49 (2nd) 
Residues with bad bonds, % 0.00 0.00 0.00 1.42 
Residues with bad angles, % 0.21 0.43 0.21 3.25 

Included are details of the MOLPROBITY analysis of our glut1 homology models (WT, wild-type glut1; Gly286Asp glut1; ΔrIle435 glut1) and of a previously published glut1 model (PDB ID 1SUK23 ). 1SUK is consistent with practically all biochemical and mutagenesis data but contains significant deviations from ideal geometry when analyzed by state-of-the-art validation software. MOLPROBITY24  ranks 1SUK in the second percentile of crystallographic structures determined at approximately 2-Å resolution (whereby the 100th percentile is the best). In contrast, our refined model of wild-type glut1 is ranked in the 55th percentile.

*

Clashscore is the number of serious steric overlaps (> 0.4 Å) per 1000 atoms.

One-hundredth percentile is the best among structures of comparable resolution; 0 percentile is the worst (N = 715; 2.00 Å ± 0.25 Å).

MolProbity score is defined as 0.425 74 × log(1+clashscore) + 0.329 96 × log[(1 + max(0pctRotOut-1)] + 0.249 79 × log[1 + max(0,100-pctRamaFavored-2)] + 0.5.

§

One-hundredth percentile is the best among structures of comparable resolution; 0 percentile is the worst (N = 12 522; 2.00 Å ± 0.25 Å).

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