Volume 97, Issue 6, Pages (June 1999)

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Volume 97, Issue 6, Pages 791-803 (June 1999) Structure of a Heterophilic Adhesion Complex between the Human CD2 and CD58 (LFA-3) Counterreceptors  Jia-huai Wang, Alex Smolyar, Kemin Tan, Jin-huan Liu, Mikyung Kim, Zhen-yu J Sun, Gerhard Wagner, Ellis L Reinherz  Cell  Volume 97, Issue 6, Pages 791-803 (June 1999) DOI: 10.1016/S0092-8674(00)80790-4

Figure 1 hCD2–CD58 Crystal Lattice Molecular packing in the hCD2–hCD58 crystal is shown with hCD2 molecules forming one layer in blue and hCD58 molecules forming another layer in yellow. hCD2-A, hCD58-A, hCD2-B, and hCD58-B molecules are labeled. The XZ plane of the unit cell is shown as viewed along the y axis. The figure was generated with SETOR (Evans 1993). Cell 1999 97, 791-803DOI: (10.1016/S0092-8674(00)80790-4)

Figure 2 Ribbon Drawing of the hCD2–hCD58 Complex in Stereo CD2 is in blue, and hCD58 is in yellow. The β strands in both molecules were defined by the program DSSP (Kabsch and Sander 1983) and labeled in black. The figure was generated using the program MOLSCRIPT (Kraulis 1991). Cell 1999 97, 791-803DOI: (10.1016/S0092-8674(00)80790-4)

Figure 3 Structure-Based Alignment of hCD2, hCD58, and Related IgSF Members Both domain 1 and domain 2 residues are indicated. Pound signs denote interface contact residues in the hCD2–hCD58 structure; asterisks mark residues in interface contacts in the hCD2–hCD2 structure; up arrows define the last residue of domains. Those underlined and labeled strands were assigned based on the crystal structures. Numbering corresponds to hCD2 and hCD58 residues. Residues shaded in red are structurally conserved within the CD2 subfamily. Cell 1999 97, 791-803DOI: (10.1016/S0092-8674(00)80790-4)

Figure 4 hCD2–hCD58 Interaction Interface (a) Stereo view of charged residues across the hCD2–hCD58 interface. The positive residues are in dark blue, and the negative residues are in deep red using a ball-and-stick format. The main chain Cα of hCD2 and hCD58 are traced in blue and yellow lines, respectively. The figure was generated using the program MOLSCRIPT (Kraulis 1991). (b) hCD2–hCD58 complex showing hCD2 electrostatic potential surface representation and hCD58 as a ribbon diagram. (c) hCD2–hCD58 showing hCD58 electrostatic potential surface representation and hCD2 as a ribbon diagram. The view of the hCD2–hCD58 complex in (c) is rotated 180° around the vertical axis with respect to the view in (b). Four selected pairs of charged residues (each pair labeled in a distinct color) involved in the interaction between hCD2 and hCD58 (as listed in Table 2) are indicated on the surfaces to demonstrate their charge complementarity and relative positions on hCD2 (b) or hCD58 (c). (d) Modeled hCD2-hCD48 complex. hCD2 is shown as a ribbon diagram and hCD48 as an electrostatic potential surface representation. The orientation of hCD2 is the same as that in (c). The distribution of the electrostatic potential across the surface of hCD48 contrasts greatly to that of hCD58 shown in (c). The electrostatic potential in (b), (c), and (d) is shown at the molecular surfaces and colored from dark blue (most positive) to deep red (most negative) according to the local electrostatic potential on a relative scale. These figures were prepared using the program GRASP (Nicholls et al. 1991). Cell 1999 97, 791-803DOI: (10.1016/S0092-8674(00)80790-4)

Figure 4 hCD2–hCD58 Interaction Interface (a) Stereo view of charged residues across the hCD2–hCD58 interface. The positive residues are in dark blue, and the negative residues are in deep red using a ball-and-stick format. The main chain Cα of hCD2 and hCD58 are traced in blue and yellow lines, respectively. The figure was generated using the program MOLSCRIPT (Kraulis 1991). (b) hCD2–hCD58 complex showing hCD2 electrostatic potential surface representation and hCD58 as a ribbon diagram. (c) hCD2–hCD58 showing hCD58 electrostatic potential surface representation and hCD2 as a ribbon diagram. The view of the hCD2–hCD58 complex in (c) is rotated 180° around the vertical axis with respect to the view in (b). Four selected pairs of charged residues (each pair labeled in a distinct color) involved in the interaction between hCD2 and hCD58 (as listed in Table 2) are indicated on the surfaces to demonstrate their charge complementarity and relative positions on hCD2 (b) or hCD58 (c). (d) Modeled hCD2-hCD48 complex. hCD2 is shown as a ribbon diagram and hCD48 as an electrostatic potential surface representation. The orientation of hCD2 is the same as that in (c). The distribution of the electrostatic potential across the surface of hCD48 contrasts greatly to that of hCD58 shown in (c). The electrostatic potential in (b), (c), and (d) is shown at the molecular surfaces and colored from dark blue (most positive) to deep red (most negative) according to the local electrostatic potential on a relative scale. These figures were prepared using the program GRASP (Nicholls et al. 1991). Cell 1999 97, 791-803DOI: (10.1016/S0092-8674(00)80790-4)

Figure 4 hCD2–hCD58 Interaction Interface (a) Stereo view of charged residues across the hCD2–hCD58 interface. The positive residues are in dark blue, and the negative residues are in deep red using a ball-and-stick format. The main chain Cα of hCD2 and hCD58 are traced in blue and yellow lines, respectively. The figure was generated using the program MOLSCRIPT (Kraulis 1991). (b) hCD2–hCD58 complex showing hCD2 electrostatic potential surface representation and hCD58 as a ribbon diagram. (c) hCD2–hCD58 showing hCD58 electrostatic potential surface representation and hCD2 as a ribbon diagram. The view of the hCD2–hCD58 complex in (c) is rotated 180° around the vertical axis with respect to the view in (b). Four selected pairs of charged residues (each pair labeled in a distinct color) involved in the interaction between hCD2 and hCD58 (as listed in Table 2) are indicated on the surfaces to demonstrate their charge complementarity and relative positions on hCD2 (b) or hCD58 (c). (d) Modeled hCD2-hCD48 complex. hCD2 is shown as a ribbon diagram and hCD48 as an electrostatic potential surface representation. The orientation of hCD2 is the same as that in (c). The distribution of the electrostatic potential across the surface of hCD48 contrasts greatly to that of hCD58 shown in (c). The electrostatic potential in (b), (c), and (d) is shown at the molecular surfaces and colored from dark blue (most positive) to deep red (most negative) according to the local electrostatic potential on a relative scale. These figures were prepared using the program GRASP (Nicholls et al. 1991). Cell 1999 97, 791-803DOI: (10.1016/S0092-8674(00)80790-4)

Figure 5 Molecular Surface Representation of the Model of hCD2–hCD58 Ectodomain Interaction The model was constructed based on crystal structures of hCD2–hCD58, hCD2–hCD2, and homology modeling of the second domain of hCD58. The two views are representative of the same complex rotated ∼120° around the vertical axis. The position of the N-linked glycans attached to asparagine residues are shown in dark blue with the first glycan linked to Asn-65 of hCD2 in pink. The T113 mAb–binding site is shown in red. GRASP surface representations of hCD2 and hCD58 are shown in light blue and yellow, respectively. Cell 1999 97, 791-803DOI: (10.1016/S0092-8674(00)80790-4)