Superantigens (SAgs) are viral or bacterial proteins that act as potent T-cell stimulants and have been implicated in a number of human diseases, including toxic shock syndrome, diabetes mellitus and multiple sclerosis. The interaction of SAgs with the T-cell receptor (TCR) and major histocompatibility complex (MHC) proteins results in the stimulation of a disproportionately large fraction of the T-cell population. We report here the crystal structures of the beta-chain of a TCR complexed with the Staphylococcus aureus enterotoxins C2 and C3 (SEC2, SEC3). These enterotoxins, which cause both toxic shock and food poisoning, bind in an identical way to the TCR beta-chain. The complementarity-determining region 2 (CDR2) of the beta-chain and, to lesser extents, CDR1 and hypervariable region 4 (HV4), bind in a cleft between the two domains of the SAgs. Thus, there is considerable overlap between the SAg-binding site and the peptide/MHC-binding sites of the TCR. A model of a TCR-SAg-MHC complex constructed from the crystal structures of (1) the beta-chain-SEC3 complex, (2) a complex between staphylococcal enterotoxin B (SEB) and an MHC molecule, and (3) a TCR V(alpha) domain, reveals that the SAg acts as a wedge between the TCR and MHC to displace the antigenic peptide away from the TCR combining site. In this way, the SAg is able to circumvent the normal mechanism for T-cell activation by specific peptide/MHC complexes.
Superantigens (SAGs) are a class of immunostimulatory proteins of bacterial or viral origin that activate T cells by binding to the V beta domain of the T cell antigen receptor (TCR). The three-dimensional structure of the complex between a TCR beta chain (mouse V beta8.2) and the SAG staphylococcal enterotoxin B (SEB) at 2.4 A resolution reveals why SEB recognizes only certain V beta families, as well as why only certain SAGs bind mouse V beta8.2. Models of the TCR-SEB-peptide/MHC class II complex indicate that V alpha interacts with the MHC beta chain in the TCR-SAG-MHC complex. The extent of the interaction is variable and is largely determined by the geometry of V alpha/V beta domain association. This variability can account for the preferential expression of certain V alpha regions among T cells reactive with SEB.
Alanine scanning mutagenesis, double mutant cycles, and X-ray crystallography were used to characterize the interface between the anti-hen egg white lysozyme (HEL) antibody D1.3 and HEL. Twelve out of the 13 nonglycine contact residues on HEL, as determined by the high-resolution crystal structure of the D1.3-HEL complex, were individually truncated to alanine. Only four positions showed a DeltaDeltaG (DeltaGmutant - DeltaGwild-type) of greater than 1.0 kcal/mol, with HEL residue Gln121 proving the most critical for binding (DeltaDeltaG = 2.9 kcal/mol). These residues form a contiguous patch at the periphery of the epitope recognized by D1.3. To understand how potentially disruptive mutations in the antigen are accommodated in the D1.3-HEL interface, we determined the crystal structure to 1.5 A resolution of the complex between D1.3 and HEL mutant Asp18 --> Ala. This mutation results in a DeltaDeltaG of only 0.3 kcal/mol, despite the loss of a hydrogen bond and seven van der Waals contacts to the Asp18 side chain. The crystal structure reveals that three additional water molecules are stably incorporated in the antigen-antibody interface at the site of the mutation. These waters help fill the cavity created by the mutation and form part of a rearranged solvent network linking the two proteins. To further dissect the energetics of specific interactions in the D1.3-HEL interface, double mutant cycles were carried out to measure the coupling of 14 amino acid pairs, 10 of which are in direct contact in the crystal structure. The highest coupling energies, 2.7 and 2.0 kcal/mol, were measured between HEL residue Gln121 and D1.3 residues VLTrp92 and VLTyr32, respectively. The interaction between Gln121 and VLTrp92 consists of three van der Waals contacts, while the interaction of Gln121 with VLTyr32 is mediated by a hydrogen bond. Surprisingly, however, most cycles between interface residues in direct contact in the crystal structure showed no significant coupling. In particular, a number of hydrogen-bonded residue pairs were found to make no net contribution to complex stabilization. We attribute these results to accessibility of the mutation sites to water, such that the mutated residues exchange their interaction with each other to interact with water. This implies that the strength of the protein-protein hydrogen bonds in these particular cases is comparable to that of the protein-water hydrogen bonds they replace. Thus, the simple fact that two residues are in direct contact in a protein-protein interface cannot be taken as evidence that there necessarily exists a productive interaction between them. Rather, the majority of such contacts may be energetically neutral, as in the D1.3-HEL complex.
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