Volume 105, Issue 1, Pages (April 2001)

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Volume 105, Issue 1, Pages 115-126 (April 2001) Dynamic Coupling between the SH2 and SH3 Domains of c-Src and Hck Underlies Their Inactivation by C-Terminal Tyrosine Phosphorylation  Matthew A. Young, Stefania Gonfloni, Giulio Superti-Furga, Benoit Roux, John Kuriyan  Cell  Volume 105, Issue 1, Pages 115-126 (April 2001) DOI: 10.1016/S0092-8674(01)00301-4

Figure 1 Structural Features of Src Family Kinases (Top) Schematic diagram illustrating inactive and assembled (left) and active (right) Src kinases. (bottom) The crystal structure of the inactive and assembled form of Hck. The connector between the SH3-SH2 connector is shown on the left Cell 2001 105, 115-126DOI: (10.1016/S0092-8674(01)00301-4)

Figure 2 Dynamic Motions Observed in Molecular Dynamics Simulations of Hck (Top) Cα atom traces of ten instantaneous structures from the 4 ns simulation of inactive and assembled Hck bound to PP1. Individual structures have been superimposed on the Cα atoms of the entire protein. (Bottom) Fluctuations in the simulation of three states of the enzyme: (i) The inactive and assembled structure (including SH2 and SH3) bound to PP1 (blue), (ii) the isolated kinase domain in the absence of the SH3 and SH2 domains bound to PP1 (green), and (iii) the isolated kinase domain in the absence of PP1 (red). RMS deviations from the crystal structure of the inactive form of Hck, calculated after superimposing the individual structures on the C-terminal lobe, are shown for the Cα atoms in the N-terminal lobe of the kinase domain Cell 2001 105, 115-126DOI: (10.1016/S0092-8674(01)00301-4)

Figure 3 Dynamic Correlations between the SH2 and SH3 Domains (a) A dynamic cross-correlation matrix for motions of all the Cα atoms over the course of the simulation of the inactive form of Hck. The correlations were calculated after superimposing each individual structure in the trajectory onto the C-terminal lobe of the kinase domain of the first structure. This procedure removes the correlations to the C-terminal lobe. The scale of the correlations is indicated on the spectrum on the right, with positive correlations plotted in the right lower half of the matrix and negative correlations plotted in the upper left half of the matrix. The correlation coefficient, Cij, between two atoms i and j, is defined as where Δ r ⇀i is the instantaneous fluctuation of the position of the ith atom with respect to its mean position. The boxed region is magnified in (b). (b) Magnified view of the correlation matrices for the simulations of the inactive, assembled state of Hck (top), the assembled state with Tyr527 in the C-terminal tail dephosphorylated and PP1 present (middle), and the assembled state with Tyr527 dephosphorylated and the nucleotide binding site empty (bottom). The region that is magnified shows the interdomain correlation coefficients between the Cα atoms of residue pairs that are in the SH3, SH2, and SH3-SH2 connector region (labeled “C”). Arrowheads mark regions in the SH3 and SH2 domains that are strongly correlated to the two other domains in the simulation of the inactive, assembled structure (top). Note that these interdomain correlations decrease in the simulations with Tyr527 dephosphorylated (middle and bottom). In particular, note that for the indicated regions, the connector is strongly correlated (indicated by red) to both the SH2 and the SH3 domains simultaneously, but that the simultaneous correlation of the connector to both domains is weaked when Tyr527 is dephosphorylated. (c) The most highly correlated residues in each of the three simulations described in (b) are indicated by red lines. Red lines are drawn connecting Cα atoms for pairs of residues with calculated correlation coefficients greater than 0.75. Correlations between pairs of residues in the same domain have been omitted for clarity. The N-lobe, C-lobe, activation loop, and catalytic loop were each considered as separate domains, and thus their correlations were not omitted Cell 2001 105, 115-126DOI: (10.1016/S0092-8674(01)00301-4)

Figure 3 Dynamic Correlations between the SH2 and SH3 Domains (a) A dynamic cross-correlation matrix for motions of all the Cα atoms over the course of the simulation of the inactive form of Hck. The correlations were calculated after superimposing each individual structure in the trajectory onto the C-terminal lobe of the kinase domain of the first structure. This procedure removes the correlations to the C-terminal lobe. The scale of the correlations is indicated on the spectrum on the right, with positive correlations plotted in the right lower half of the matrix and negative correlations plotted in the upper left half of the matrix. The correlation coefficient, Cij, between two atoms i and j, is defined as where Δ r ⇀i is the instantaneous fluctuation of the position of the ith atom with respect to its mean position. The boxed region is magnified in (b). (b) Magnified view of the correlation matrices for the simulations of the inactive, assembled state of Hck (top), the assembled state with Tyr527 in the C-terminal tail dephosphorylated and PP1 present (middle), and the assembled state with Tyr527 dephosphorylated and the nucleotide binding site empty (bottom). The region that is magnified shows the interdomain correlation coefficients between the Cα atoms of residue pairs that are in the SH3, SH2, and SH3-SH2 connector region (labeled “C”). Arrowheads mark regions in the SH3 and SH2 domains that are strongly correlated to the two other domains in the simulation of the inactive, assembled structure (top). Note that these interdomain correlations decrease in the simulations with Tyr527 dephosphorylated (middle and bottom). In particular, note that for the indicated regions, the connector is strongly correlated (indicated by red) to both the SH2 and the SH3 domains simultaneously, but that the simultaneous correlation of the connector to both domains is weaked when Tyr527 is dephosphorylated. (c) The most highly correlated residues in each of the three simulations described in (b) are indicated by red lines. Red lines are drawn connecting Cα atoms for pairs of residues with calculated correlation coefficients greater than 0.75. Correlations between pairs of residues in the same domain have been omitted for clarity. The N-lobe, C-lobe, activation loop, and catalytic loop were each considered as separate domains, and thus their correlations were not omitted Cell 2001 105, 115-126DOI: (10.1016/S0092-8674(01)00301-4)

Figure 4 Displacements of the SH3 Domain Relative to N-Terminal Lobe of Kinase Each panels shows five instantaneous structures, superimposed on the N-terminal lobe of the kinase domain, for the protein with Tyr527 phosphorylated and PP1 bound at the nucleotide binding site (top), for Tyr527 dephosphorylated and displaced from the SH2 domain (middle), and the same, with PP1 was removed (bottom) Cell 2001 105, 115-126DOI: (10.1016/S0092-8674(01)00301-4)

Figure 5 Response of the SH2 Domain in a Targeted Molecular Dynamics Trajectory that Moves the Activation Loop from the Inactive to the Active Conformation The RMS deviation of the restrained atoms (the activation loop, residues 404 to 421) from the structure of the target is shown in black (dashed line). The plot fails to reach zero due to the fact that, in this analysis, the structures were superimposed on the C-lobe of the kinase domain rather than just the restraint set. RMS deviations of the atoms in the N-terminal lobe of the kinase relative to the conformation of the crystal structure of the inactive form are shown in red. Displacement of the Cα atom of Arg175, a critical residue in the SH2 domain that coordinates the phosphotyrosine, is shown in blue. Individual structures at the beginning, middle, and end of the simulation are also shown Cell 2001 105, 115-126DOI: (10.1016/S0092-8674(01)00301-4)

Figure 6 Effect of the Triple Glycine Mutation in Simulations of c-Src (a) Simulation of wild-type c-Src. (b) Simulation of a c-Src variant in which Ser142, Ala145, and Glu146 are replaced by glycine. In each case, a plot indicating the most highly correlated residues (see Figure 3c) is shown on the left, and the final structure, after 4 ns of dynamics, is shown on the right. Note the altered structure of the SH3-SH2 connector in the simulation of the mutant Cell 2001 105, 115-126DOI: (10.1016/S0092-8674(01)00301-4)

Figure 7 S. pombe Based Growth Assay of the Ability of Csk to Properly Downregulate Wild-Type and SH3-SH2 Connector Mutant Forms of c-SRC (a) Growth curves of S. pombe cells expressing wild-type and mutant forms of c-Src from the inducible nmt1 promoter of the pRSP vector (as indicated) and pAU (empty vector) or pAU-Csk. The y axis is logarithmic. Under the conditions used, expression of Src takes around 20 hr post-induction to reach maximal accumulation. (b) Immunoblots of lysates prepared from S. pombe 22 hr post-induction show the levels of Src and Csk proteins accumulated Cell 2001 105, 115-126DOI: (10.1016/S0092-8674(01)00301-4)