Vibrational and Molecular Properties of Mg2+ Binding and Ion Selectivity in the Magnesium Channel MgtE.

Magnesium ions (Mg2+) are crucial for various biological processes. A bacterial Mg2+ channel, MgtE, tightly regulates the intracellular Mg2+ concentration. Previous X-ray crystal structures showed that MgtE forms a dimeric structure composed of a total of 10 transmembrane α helices forming a central pore, and intracellular soluble domains constituting a Mg2+ sensor. The ion selectivity for Mg2+ over Ca2+ resides at a central cavity in the transmembrane pore of MgtE, involving a conserved aspartate residue (Asp432) from each monomer. Here, we applied ion-exchange-induced difference FTIR spectroscopy to analyze the interactions between MgtE and divalent cations, Mg2+ and Ca2+. Using site-directed mutagenesis, vibrational bands at 1421 (Mg2+), 1407 (Mg2+), ∼1440 (Ca2+), and 1390 (Ca2+) cm-1 were assigned to symmetric carboxylate stretching modes of Asp432, involved in the ion coordination. Conservative modifications of the central cavity by Asp432Glu or Ala417Leu mutations resulted in the disappearance of the Mg2+-sensitive carboxylate bands, suggesting a highly optimized geometry for accommodating a Mg2+ ion. The dependency of the vibrational changes on Mg2+ and Ca2+ concentrations revealed the presence of a two different classes of binding sites: a high affinity site for Mg2+ ( Kd ≈ 0.3 mM) with low Ca2+ affinity ( Kd ≈ 80 mM), and a medium affinity site for Mg2+ ( Kd ≈ 2 mM) and Ca2+ ( Kd ≈ 6 mM), tentatively assigned to the central cavity and the sensor domain, respectively. With the aid of molecular dynamics simulation and normal-mode analysis by quantum chemistry, we confirm that changes in carboxylate bands of the high affinity binding site originate from Asp432 in the central cavity.

Structural properties determining low K+ affinity of the selectivity filter in the TWIK1 K+ channel.

Canonical K+ channels are tetrameric and highly K+-selective, whereas two-pore-domain K+ (K2P) channels form dimers, but with a similar pore architecture. A two-pore-domain potassium channel TWIK1 (KCNK1 or K2P1) allows permeation of Na+ and other monovalent ions, resulting mainly from the presence of Thr-118 in the P1 domain. However, the mechanistic basis for this reduced selectivity is unclear. Using ion-exchange-induced difference IR spectroscopy, we analyzed WT TWIK1 and T118I (highly K+-selective) and L228F (substitution in the P2 domain) TWIK1 variants and found that in the presence of K+ ions, WT and both variants exhibit an amide-I band at 1680 cm-1 This band corresponds to interactions of the backbone carbonyls in the selectivity filter with K+, a feature very similar to that of the canonical K+ channel KcsA. Computational analysis indicated that the relatively high frequency for the amide-I band is well explained by impairment of hydrogen bond formation with water molecules. Moreover, concentration-dependent spectral changes indicated that the K+ affinity of the WT selectivity filter was much lower than those of the variants. Furthermore, only the variants displayed a higher frequency shift of the 1680-cm-1 band upon changes from K+ to Rb+ or Cs+ conditions. High-speed atomic force microscopy disclosed that TWIK1's surface morphology largely does not change in K+ and Na+ solutions. Our results reveal the local conformational changes of the TWIK1 selectivity filter and suggest that the amide-I bands may be useful "molecular fingerprints" for assessing the properties of other K+ channels.

Theoretical analysis of the domain-swapped dimerization of cytochrome c: An MD and 3D-RISM approach.

The structural stability of a cytochrome c domain-swapped dimer compared with that of the monomer was investigated by molecular dynamics (MD) simulations and by three-dimensional reference interaction site model (3D-RISM) theory. The structural fluctuation and structural energy of cytochrome c were treated by MD simulations, and the solvation thermodynamics was treated by 3D-RISM theory. The domain-swapped dimer state is slightly less stable than the monomer state, which is consistent with experimental observations; the total free energy difference is calculated as 25 kcal mol-1. The conformational change and translational/rotational entropy change contribute to the destabilization of the dimer, whereas the hydration and vibrational entropy contribute to the stabilization. Further analyses on the residues located at the hinge loop for swapping were conducted, and the results reveal details at the molecular level of the structural and interaction changes upon dimerization.