Acetylcholine Receptor Gating at Extracellular Transmembrane Domain Interface: the Cys-Loop and M2–M3 Linker

Acetylcholine receptor channel gating is a propagated conformational cascade that links changes in structure and function at the transmitter binding sites in the extracellular domain (ECD) with those at a “gate” in the transmembrane domain (TMD). We used Φ-value analysis to probe the relative timing of the gating motions of α-subunit residues located near the ECD–TMD interface. Mutation of four of the seven amino acids in the M2–M3 linker (which connects the pore-lining M2 helix with the M3 helix), including three of the four residues in the core of the linker, changed the diliganded gating equilibrium constant (Keq) by up to 10,000-fold (P272 > I274 > A270 > G275). The average Φ-value for the whole linker was ∼0.64. One interpretation of this result is that the gating motions of the M2–M3 linker are approximately synchronous with those of much of M2 (∼0.64), but occur after those of the transmitter binding site region (∼0.93) and loops 2 and 7 (∼0.77). We also examined mutants of six cys-loop residues (V132, T133, H134, F135, P136, and F137). Mutation of V132, H134, and F135 changed Keq by 2800-, 10-, and 18-fold, respectively, and with an average Φ-value of 0.74, similar to those of other cys-loop residues. Even though V132 and I274 are close, the energetic coupling between I and V mutants of these positions was small (≤0.51 kcal mol−1). The M2–M3 linker appears to be the key moving part that couples gating motions at the base of the ECD with those in TMD. These interactions are distributed along an ∼16-Å border and involve about a dozen residues

Signal Transduction Pathways in the Pentameric Ligand-Gated Ion Channels

The mechanisms of allosteric action within pentameric ligand-gated ion channels (pLGICs) remain to be determined. Using crystallography, site-directed mutagenesis, and two-electrode voltage clamp measurements, we identified two functionally relevant sites in the extracellular (EC) domain of the bacterial pLGIC from Gloeobacter violaceus (GLIC). One site is at the C-loop region, where the NQN mutation (D91N, E177Q, and D178N) eliminated inter-subunit salt bridges in the open-channel GLIC structure and thereby shifted the channel activation to a higher agonist concentration. The other site is below the C-loop, where binding of the anesthetic ketamine inhibited GLIC currents in a concentration dependent manner. To understand how a perturbation signal in the EC domain, either resulting from the NQN mutation or ketamine binding, is transduced to the channel gate, we have used the Perturbation-based Markovian Transmission (PMT) model to determine dynamic responses of the GLIC channel and signaling pathways upon initial perturbations in the EC domain of GLIC. Despite the existence of many possible routes for the initial perturbation signal to reach the channel gate, the PMT model in combination with Yen's algorithm revealed that perturbation signals with the highest probability flow travel either via the β1-β2 loop or through pre-TM1. The β1-β2 loop occurs in either intra- or inter-subunit pathways, while pre-TM1 occurs exclusively in inter-subunit pathways. Residues involved in both types of pathways are well supported by previous experimental data on nAChR. The direct coupling between pre-TM1 and TM2 of the adjacent subunit adds new insight into the allosteric signaling mechanism in pLGICs. © 2013 Mowrey et al

Impact of the Synthetic Antiferromagnet in TMR Sensors for Improved Angular- Dependent Output

Tunneling magnetoresistive (TMR) sensors can precisely measure magnetic fields, being a key element in next-generation highly sensitive angular positioning systems. Still, when fields are applied in directions that differ from the easy axis, the interplay between all magnetic contributions becomes crucial. In this work, we investigate the angular-dependent output of TMR sensors, when operating under a field that saturates the free layer (FL). We have used synthetic antiferromagnets (SAFs) with tuned antiferromagnetic (Δ H) by changing the ferromagnetic (FM) layer thicknesses. The reference layer (RL) reversal field (H0+) was set between 57 and 260 mT. The results show that these SAF characteristics affect the angular-dependent FL saturation field, showing differences up to ≈6 mT when changing SAF magnetic moment. From R(H, θ) , and using a macrospin model, we evaluate the magnetization misalignment in-between FM layers. For the SAF with higher H+-, deviations up to 10°, are seen when operating at 100 mT ll H0+. Noticeably, we also observed a nonnegligible contribution of the SAF magnetization reversal to R(H,θ) even at the low external fields of 20 mT, with the deviations of ≈1° from ideal behavior, which is often overlooked. This study links the observed resistance deviations to specific magnetic couplings and intrinsic anisotropies. With this information, we are able to design the multilayers for controlled output inaccuracies or according to the maximum allowed errors in the application. Ultimately, an optimal saturation magnetic field is obtained to deliver the best angular performance in the TMR elements.</p

Mapping Heat Exchange in an Allosteric Protein

Nicotinic acetylcholine receptors (AChRs) are synaptic ion channels that spontaneously isomerize (i.e., gate) between resting and active conformations. We used single-molecule electrophysiology to measure the temperature dependencies of mouse neuromuscular AChR gating rate and equilibrium constants. From these we estimated free energy, enthalpy, and entropy changes caused by mutations of amino acids located between the transmitter binding sites and the middle of the membrane domain. The range of equilibrium enthalpy change (13.4 kcal/mol) was larger than for free energy change (5.5 kcal/mol at 25°C). For two residues, the slope of the rate-equilibrium free energy relationship (Φ) was approximately constant with temperature. Mutant cycle analysis showed that both free energies and enthalpies are additive for energetically independent mutations. We hypothesize that changes in energy associated with changes in structure mainly occur close to the site of the mutation, and, hence, that it is possible to make a residue-by-residue map of heat exchange in the AChR gating isomerization. The structural correlates of enthalpy changes are discussed for 12 different mutations in the protein

Subunit Symmetry at the Extracellular Domain-Transmembrane Domain Interface in Acetylcholine Receptor Channel Gating*

Transmitter molecules bind to synaptic acetylcholine receptor channels (AChRs) to promote a global channel-opening conformational change. Although the detailed mechanism that links ligand binding and channel gating is uncertain, the energy changes caused by mutations appear to be more symmetrical between subunits in the transmembrane domain compared with the extracellular domain. The only covalent connection between these domains is the pre-M1 linker, a stretch of five amino acids that joins strand β10 with the M1 helix. In each subunit, this linker has a central Arg (Arg3′), which only in the non-α-subunits is flanked by positively charged residues. Previous studies showed that mutations of Arg3′ in the α-subunit alter the gating equilibrium constant and reduce channel expression. We recorded single-channel currents and estimated the gating rate and equilibrium constants of adult mouse AChRs with mutations at the pre-M1 linker and the nearby residue Glu45 in non-α-subunits. In all subunits, mutations of Arg3′ had similar effects as in the α-subunit. In the ϵ-subunit, mutations of the flanking residues and Glu45 had only small effects, and there was no energy coupling between ϵGlu45 and ϵArg3′. The non-α-subunit Arg3′ residues had Φ-values that were similar to those for the α-subunit. The results suggest that there is a general symmetry between the AChR subunits during gating isomerization in this linker and that the central Arg is involved in expression more so than gating. The energy transfer through the AChR during gating appears to mainly involve Glu45, but only in the α-subunits