(
A) Defining the localization of anion binding sites 1 (green), 2 (magenta) and 3 (yellow) for MD simulations. For reference, the loop down conformation of WT CK1δ is represented as ribbons (cyan). (
B) Residue Y225 displays more conformational freedom in the
tau mutant (right panel) than in WT CK1δ (left panel). Populations of the gauche+ (g+), trans (t) and gauche- (g-) rotamers for Y225 from MD simulations of the loop up and loop down conformations of WT and
tau kinase are depicted. (
C-D) Stability of the activation loop assessed by the Root Mean Square Deviation (RMSD) of residues 168–175 with respect to the loop down conformation (RMSD
down, blue) or to the loop up conformation (RMSD
up, magenta) as observed in the crystal structures. For both systems, the Site 2 anion was removed computationally before beginning MD simulations. Panel C, WT CK1δ
loop down; D,
tau CK1δ
loop down; both show RMSDs superimposed from all five MD replicas. (
E-F) Dynamics of the L-EF loop obtained from Gaussian Accelerated MD simulations in WT CK1δ (panel E) and
tau mutant (panel F) when the activation loop in the ‘down’ conformation and the second anion binding site has been removed computationally. The RMSD was calculated for the backbone atoms of residues 213–224 for each independent replica (gray, n = 5) and then averaged (green). The molecular representations show crystallographic structures of the enzyme (in gray) superimposed with several snapshots of the loop L-EF extracted from the Gaussian Accelerated MD (GaMD) simulations (in green). When present, sulfate anions are represented by van der Waals spheres. G, Volumetric analysis of the Site 1 binding site (gray sphere), substrate binding cleft (golden sphere) and Site 2 anion binding site (rose sphere) during the GaMD simulations. In each system, the volumes were calculated for snapshots extracted from the GaMD trajectories every 2 ns, using POVME 3.0 (
Wagner et al., 2017). Water and ions were computationally removed prior to volume calculations.