Our structural efforts are driven by the following questions to explore the biology of peptide receptors of the class A (rhodopsin) GPCR family, using NTS1 as a model system. (i) How do peptide ligands interact with their respective peptide receptors? (ii) How does the binding of a peptide ligand translate into the structural changes within the receptor to allow the activation of the G protein (iii) How is specificity of G protein binding achieved? We have recently determined at 2.8A resolution the x-ray crystal structure of NTS1 bound to its peptide agonist in an active-like state. A number of strategies were implemented to achieve this: (i) Conformational thermostabilization generated a NTS1 mutant with greatly improved stability, locked into an agonist binding, active-like conformation. (ii) The use of the T4 lysozyme technology replacing the third inner loop promoted crystal contacts. (iii) Lipidic cubic phase crystallization resulted in highly diffracting crystals. The NTS1 structure has many hallmark features of an active-like receptor conformation such as an outward-tilted transmembrane helix 6 at the cytoplasmic surface and key conserved residues in positions characteristic for active but not for inactive GPCRs. The NT binding pocket is wide open on the extracellular surface of NTS1. The peptide agonist NT8-13, the C terminal portion of NT responsible for agonist-induced activation of the receptor, binds to NTS1 in an extended conformation nearly perpendicular to the membrane plane with the C-terminus oriented towards the receptor core. There is a striking difference between the binding mode of NT8-13 in NTS1 and the binding of small agonists in rhodopsin or beta-adrenergic receptors. NT8-13 does not penetrate the receptor as deeply compared to those small agonists, indicating that the mode of activation of NTS1 is subtly different from these receptors. As our future goal is to understand the molecular events that occur upon signaling of NTS1, we will pursue crystal structures of NTS1 in several signaling states. Specifically, we will obtain structures of NTS1 in the inactive state and the G protein-bound states, which will allow a detailed comparison of the similarities but importantly also differences between the signaling properties of GPCRs, which bind small molecule ligands deep within their transmembrane cores, and peptide receptors, which bind their ligands at the receptor surface.
Nehmé, Rony; Carpenter, Byron; Singhal, Ankita et al. (2017) Mini-G proteins: Novel tools for studying GPCRs in their active conformation. PLoS One 12:e0175642 |
Grisshammer, Reinhard (2017) New approaches towards the understanding of integral membrane proteins: A structural perspective on G protein-coupled receptors. Protein Sci 26:1493-1504 |
Lee, Sangbae; Mao, Allen; Bhattacharya, Supriyo et al. (2016) How Do Short Chain Nonionic Detergents Destabilize G-Protein-Coupled Receptors? J Am Chem Soc 138:15425-15433 |
Vaidehi, Nagarajan; Grisshammer, Reinhard; Tate, Christopher G (2016) How Can Mutations Thermostabilize G-Protein-Coupled Receptors? Trends Pharmacol Sci 37:37-46 |
Krumm, Brian E; Lee, Sangbae; Bhattacharya, Supriyo et al. (2016) Structure and dynamics of a constitutively active neurotensin receptor. Sci Rep 6:38564 |
Krumm, Brian E; Grisshammer, Reinhard (2015) Peptide ligand recognition by G protein-coupled receptors. Front Pharmacol 6:48 |
Xiao, Su; Shiloach, Joseph; Grisshammer, Reinhard (2015) Construction of recombinant HEK293 cell lines for the expression of the neurotensin receptor NTSR1. Methods Mol Biol 1272:51-64 |
Lee, Sangbae; Bhattacharya, Supriyo; Tate, Christopher G et al. (2015) Structural dynamics and thermostabilization of neurotensin receptor 1. J Phys Chem B 119:4917-28 |
Krumm, Brian E; White, Jim F; Shah, Priyanka et al. (2015) Structural prerequisites for G-protein activation by the neurotensin receptor. Nat Commun 6:7895 |
Lee, Sangbae; Bhattacharya, Supriyo; Grisshammer, Reinhard et al. (2014) Dynamic behavior of the active and inactive states of the adenosine A(2A) receptor. J Phys Chem B 118:3355-65 |
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