See Figure 1B for 2 equivalent sites. LA, low affinity; HA, high affinity. (Top). Standard activation scheme; bind and gate transitions bracket AC (a LA closed state, Delcastillo, et al., 1957). In gate, both channel conductance and binding site affinity increase (ACLA⇄AOHA). Middle. Expanded activation scheme showing undetected intermediates inside bind and gate. In bind, the agonist arrives at the target by diffusion (diffuse) and forms an ultra-LA AC encounter complex, followed by the first stage of the induced fit (catch1) that forms ACLA. In gate (boxed), the second stage of the rearrangement (hold) forms ACHA, followed by additional rearrangements in distant domains (etc) that eventually lead to AOHA. Experimental KdC and KdO values are dominated by energy changes in the two stages of the induced fit. Bottom. Expansion of gating. The distribution of Φ values2 suggests that the global isomerization involves passage through 4 short-lived (~100 ns) CHA states (denoted with ‘) associated with sequential rearrangements of the ECD (twist), TMD (tilt) and gate region (dilation), followed by pore water/membrane movements to allow ion transit (pop); Φ value given below each transition (Purohit et al., 2013; Gupta et al., 2017). The only agonist dependent rearrangements are catch (AC⇄ACLA; ΔGLA) and hold (ACLA⇄AC’; DGHA-ΔGLA), stages of the induced fit linked in a LFER (Figure 2). Together, sojourns in the ensemble of CHA states appear in single-channel currents as a brief gap (F for ‘flip’) (Auerbach, 1993; Lape et al., 2008; Mukhtasimova et al., 2005; Shi et al., 2023). The longitudinally-decreasing, coarse gradient in Φ suggests that the channel-opening gating transition is a conformational cascade (‘wave’) that propagates from the agonist to the gate, block-wise (Grosman et al., 2000), perhaps as an extended LFER. To emphasize that in AChRs binding ispart of gating, we show that a CRC and synaptic decay time constant can be calculated from the agonist association rate constant, kon to C (catch) if η and L0 are known a priori. (A) CRC. For many agonists, koff,C ~15,000 s–1 (Jadey and Auerbach, 2012). Calculate (i) KdC~1.5 × 104 s–1/kon,C, (ii) KdO (Equation 2), (iii) L2 (Equation 1) and (iv) POmax and EC50 (Equation 4a, Equation 4b, Equation 4c, Equation 4d). For example, η=0.5 and L0=7.4 × 10–7 (at Vm=-100 mV). ACh: measure kon,C=108 M–1s–1, calculate KdC = 150 μM, KdO = 22 nM, L2=33, POmax = 0.97 and EC50=31 μM. Choline: measure konC = 5 × 106 M–1s–1, calculate KdC = 3 mM, KdO = 9 μM, L2=0.08, POmax = 0.08 and EC50=6.8 mM. The procedure can be reversed (konC can be estimated from a CRC). (B) Synaptic decay time constant (τ). In adult-type AChRs the diliganded channel-closing rate constant (b2) for many agonists is ~2500 s–1 (–100 mV and 23 °C) (Grosman et al., 2000). τ~0.4 (1+f2/2*koff), where f2 is the diliganded opening rate constant, f2=L2*2500 s–1. Using the above kon,C for ACh yields τ=1.5ms. That the agonist’s association rate constant can approximate POmax, EC50 and τ demonstrates the entanglement between binding and gating. Unlike diffusion, natural selection can adjust the catch ‘induced fit’ (kon,C) to fine tune physiological responses.
1Experimental evidence for catch in AChRs: kon to C is (i) slower than the limit set by diffusion, (ii) correlated with agonist potency rather than diffusion constant, (iii) slower than kon to O that is approximately diffusional (Nayak and Auerbach, 2017)3 and (iv) for choline highly temperature dependent (Gupta et al., 2017). Evidence that the hold stage of the induced fit occurs at the start of the global isomerization is that (i) Φ~0.95 for agonists and binding site residues (Purohit et al., 2013) (see below), and (ii) agonists increase the channel-opening rate constant (the affinity increase occurs before the transition state; Figure 1A).
2 Φ is log f2/log L2 for a series of perturbations and reports the free energy change of the perturbed location at the gating transition state (relative to A2O). In AChRs, a longitudinal, blocky, decreasing gradient in Φ (neurotransmitter site to gate) suggests the allosteric transition is a cascade of discrete domain rearrangements that connects A2C and A2O (Auerbach, 2005). Although Φ values sequence (1–0, early to late) and locate gating rearrangements, they do not provide temporal information or quantify energy coupling between domains.
3 The barrier that prevents agonists from forming ACLA by diffusioserves a purpose. In AChRs, kon,C correlates with agonist potency (Jadey and Auerbach, 2012; Jadey et al., 2011; Nayak and Auerbach, 2017), so the weak-agonist choline (present at the synapse at a high concentration) that would otherwise interfere with signaling is excluded from the pocket, preventing competitive antagonism. Extracellular cations compete with agonists to slow kon,C (Cs+>K+>Na+>Li+) (Akk and Auerbach, 1996), and the mutation εE184Q eliminates this competition (Akk et al., 1999). We hypothesize that the ions and agonist compete at the encounter complex site (for instance, K++C⇄KC) rather that the aromatic pocket. Agonist occupancy of the ultra-low-affinity AC binding site triggers the catch-and hold rearrangement.