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Simple ternary complex model

B. Simple Ternary Complex Model General Considerations. 105... [Pg.95]

The simple ternary complex model (Fig. 2A) describes the binding of ligands to GPCRs, leading to the activation of G protein (De Lean et ah, 1980 Lefkowitz et at, 1993). This model is based on the four equilibrium reactions that account for all of the thermodynamically possible interactions between the three species ligand, GPCR, and G protein. [Pg.105]

Analysis of the soluble G-bead assembly provides a complementary classification of full and partial agonists, based on their distinct abilities to assemble ternary complexes (LRG). It appears that the behavior of receptors and entire ligand families can be described by the simple ternary complex model alone (Fig. 2A). The analysis provides estimates for the ligand-dependent equilibrium constants that govern the simple ternary complex model. Unique, potentially intermediate, conformational states of the receptor defined by interactions with a particular ligand are characterized by individual binding constants. While these data do not directly show these different conformational states, the bead system appears to act as a... [Pg.115]

Fig. 5. Conceptual schematic of the receptor conformational states elicited by binding to partial (L, ) or full (Ly) agonists, and a depiction of the correlation between the various conformational states and their ability to bind with G proteins. Solid lines show the conformational distributions hypothesized from soluble ternary complex data analyzed by the simple ternary complex model. When a partial agonist binds with a receptor (L R) in this model, the receptor forms a conformational state which has an intermediate affinity for G protein, consequendy leading to formation of intermediate amounts of L RG. On the other hand, the dotted line represents the potential receptor conformations induced by a partial agonist consistent with the extended ternary complex model, which includes the isomerization of receptor between R and R, the only receptor conformation allowed to bind with G protein. For this model, the interactions of a partial agonist with a receptor would result in two populations of ligand-bound receptors with only one (LR ) able to bind with G protein. The x-axis is analogous to the cooperativity factor a. Fig. 5. Conceptual schematic of the receptor conformational states elicited by binding to partial (L, ) or full (Ly) agonists, and a depiction of the correlation between the various conformational states and their ability to bind with G proteins. Solid lines show the conformational distributions hypothesized from soluble ternary complex data analyzed by the simple ternary complex model. When a partial agonist binds with a receptor (L R) in this model, the receptor forms a conformational state which has an intermediate affinity for G protein, consequendy leading to formation of intermediate amounts of L RG. On the other hand, the dotted line represents the potential receptor conformations induced by a partial agonist consistent with the extended ternary complex model, which includes the isomerization of receptor between R and R, the only receptor conformation allowed to bind with G protein. For this model, the interactions of a partial agonist with a receptor would result in two populations of ligand-bound receptors with only one (LR ) able to bind with G protein. The x-axis is analogous to the cooperativity factor a.
Here, the agonist-receptor complex (AR) combines with a G-protein (G) to form a ternary complex (ARG ), which can initiate further cellular events, such as the activation of adenylate cyclase. However, this simple scheme (the ternary complex model) was not in keeping with what was already known about the importance of isomerization in receptor activation (see Sections 1.2.3 and 1.4.3), and it also failed to account for findings that were soon to come from studies of mutated receptors. In all current models of G-protein-coupled receptors, receptor activation by isomerization is assumed to occur so that the model becomes ... [Pg.31]

A measurement system that is able to quantitatively determine the interactions of receptor and G protein has the potential for more detailed testing of ternary complex models. The soluble receptor systems, ([l AR and FPR) described in Section II, allow for the direct and quantitative evaluation of receptor and G protein interactions (Simons et al, 2003, 2004). Soluble receptors allow access to both the extracellular ligandbinding site and the intracellular G protein-binding site of the receptor. As the site densities on the particles are typically lower than those that support rebinding (Goldstein et al, 1989), simple three-dimensional concentrations are appropriate for the components. Thus, by applying molar units for all the reaction components in the definitions listed in Fig. 2A, the units for the equilibrium dissociation constants are molar, not moles per square meter as for membrane-bound receptor interactions. These assemblies are also suitable for kinetic analysis of ternary complex disassembly. [Pg.108]

Figure 1 Representation of the simple ternary allosteric complex model of interaction of a ligand A with an allosteric agent X at a receptor R. (From Ref. 2.)... Figure 1 Representation of the simple ternary allosteric complex model of interaction of a ligand A with an allosteric agent X at a receptor R. (From Ref. 2.)...
It has already been noticed (see 3.9.4) that according to the mentioned concepts several ternary compounds may be considered as the result of a sort of structural interaction between binary compounds. As a consequence some regular trend could also be predicted for their occurrence in their phase diagrams and in the description (and perhaps modelling) of their thermodynamic properties. A few details about this type of structural relationships will be considered in the following and, in this introduction, examples of blocks of simple structural types and of their combination in more complex types will be described. [Pg.629]

Content. After a brief overview of molecular collisions and interactions, dipole radiation, and instrumentation (Chapter 2), we consider examples of measured collision-induced spectra, from the simplest systems (rare gas mixtures at low density) to the more complex molecular systems. Chapter 3 reviews the measurements. It is divided into three parts translational, rototranslational and rotovibrational induced spectra. Each of these considers the binary and ternary spectra, and van der Waals molecules we also take a brief look at the spectra of dense systems (liquids and solids). Once the experimental evidence is collected and understood in terms of simple models, a more theoretical approach is chosen for the discussion of induced dipole moments (Chapter 4) and the spectra (Chapters 5 and 6). Chapters 3 through 6 are the backbone of the book. Related topics, such as redistribution of radiation, electronic collision-induced absorption and emission, etc., and applications are considered in Chapter 7. [Pg.19]

A minimal model for self-replication is shown in Scheme 12.23. The replicator (R) must be able to recognise and bind at least two different precursor components (Cl and C2) in a ternary (three component) complex, and to accelerate their chemical reaction with each other to produce a product that is a copy of the original R. Such a simple system will always be in competition with the uncatalysed binary reaction of Cl and C2. [Pg.852]

An interesting investigation of the ternary mixture H2S + C02+CH4 was performed by Ng et al. (1985). Although much of this study was at temperatures below those of interest in acid gas injection, it provides data useful for testing phase-behavior prediction models. The multiphase equilibrium that Ng et al. observed for this mixture, including multiple critical points for a mixture of fixed composition, should be of interest to all engineers working with such mixtures. It demonstrates that the equilibria can be complex, even for relatively simple systems. [Pg.89]

A reasonable thermodynamic model was tried to explain the effect of fluoride concentration on the MgO solubility in the MgCl2-NaCl-NaF ternary melts. However, both the activity model used to calculate the activity of MgCl2 and MgF2 and the understanding of the Mg-O-Cl(F) complexes formed in the melt seemed to be too simple to give a reasonable mechanism for MgO solubility in these complicated melts. [Pg.58]

Recent simulation work on chemical patterns has moved beyond simple line-space patterns to consider more complex stmctures. Stoykovich et al. explored the self-assembly of a ternary blend consisting AB diblock, A homopolymer, and B homopolymer over complex chemical patterns with simulation and experiment. In this work, simulations were particularly useful to illustrate the distribution of homopolymer to regions of the chemical pattern that would otherwise nudeate defects in the block copolymer. Similar simulations were used to model the distribution of nanopartides in a block copolymer film above chemical patterns. ... [Pg.246]

Similar models can be developed for more complex systems such as ternary and quaternary alloys. As an example, we will consider a modified regular solution model for quaternary alloys proposed by K. Onabe [8]. This model does not include some of the detailed treatment in the Ichimura calculation [6] described in Section 6.2.1. Specifically, it does not include strain and assumes a random alloy entropy. However, the calculation is simple, illustrative of the behavior of multinary alloys, and can easily be extended to include the strain and entropy terms. [Pg.249]


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