Volume 107, Issue 6, Pages (September 2014)

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Volume 107, Issue 6, Pages 1352-1363 (September 2014) Identification of Electric-Field-Dependent Steps in the Na+,K+-Pump Cycle  Laura J. Mares, Alvaro Garcia, Helge H. Rasmussen, Flemming Cornelius, Yasser A. Mahmmoud, Joshua R. Berlin, Bogdan Lev, Toby W. Allen, Ronald J. Clarke  Biophysical Journal  Volume 107, Issue 6, Pages 1352-1363 (September 2014) DOI: 10.1016/j.bpj.2014.05.054 Copyright © 2014 Biophysical Society Terms and Conditions

Figure 1 Immunoblot using C-terminal antibody against the α-subunit. Proteolytic cleavage, SDS-PAGE, and immunoblotting were performed as described under Materials and Methods. Incubation with trypsin was allowed to proceed for the indicated time intervals (minutes) before quenching with SDS sample buffer with TCA. Zero time indicates control samples where SDS sample buffer/TCA was added before addition of trypsin. Biophysical Journal 2014 107, 1352-1363DOI: (10.1016/j.bpj.2014.05.054) Copyright © 2014 Biophysical Society Terms and Conditions

Figure 2 Concentration dependencies of relative fluorescence changes, ΔF/F0, accompanying the addition of either BTEA chloride or KCl to Na+,K+-ATPase-containing membrane fragments (33 μg/mL or 0.23 μM) noncovalently labeled with RH421, 50 nM. In measurements in which either BTEA or K+ were added alone, F0 refers to the fluorescence level before the addition of either BTEA or K+ ions. In measurements in which K+ was added at a constant [BTEA], F0 refers to the fluorescence level before the addition of K+. The three titrations shown are: BTEA alone (Δ), K+ alone (●), and K+ in the presence of 4 mM BTEA (○). (Solid lines) Nonlinear least-squares fits to the data of Eq. 1, in the case of the BTEA titration, or Eq. 2 in the case of both K+ titrations. Each measurement for both K+ titrations was performed in triplicate; (plotted points) average value. Each measurement for the BTEA titration was performed once, but a much larger number of BTEA concentrations were used to allow for a statistical test on the significance of the small fluorescence increase observed. Biophysical Journal 2014 107, 1352-1363DOI: (10.1016/j.bpj.2014.05.054) Copyright © 2014 Biophysical Society Terms and Conditions

Figure 3 Electric field calculated for PDB:2ZXE due to binding of 2 K+ ions (a), and for PDB:3WGU due to binding of 3 Na+ ions (b), in units of 107 V/m (truncated at 20 × 107 V/m). (Solid vertical lines) Boundaries for the implicit membrane (dielectric constant εm = 2), with interfacial region (with εi = 80) indicated (between the dashed and solid lines). The protein was assigned a dielectric constant εp = 10 (with alternative εp = 2, shown in Fig. S1 and Fig. S2 in the Supporting Material). (Solid curves) Protein boundary. (Yellow circles) Bound ions. Additional calculations are provided in Fig. S1, Fig. S2, and Fig. S3. To see this figure in color, go online. Biophysical Journal 2014 107, 1352-1363DOI: (10.1016/j.bpj.2014.05.054) Copyright © 2014 Biophysical Society Terms and Conditions

Figure 4 (Schematic diagram) Membrane-bound RH421. Two possible scenarios are shown that could both lead to a decrease in the fluorescence of RH421, as observed when either Na+ or K+ ions are occluded by the phosphorylated enzyme. The movement of either positive charge toward the amino end of the molecule (scenario a) or negative charge away from the amino end (scenario b) would both lead to redistribution of electrons within the ground-state RH421 chromophore toward the amino nitrogen and a shift in its fluorescence excitation spectrum to shorter wavelengths, i.e., higher energy. Biophysical Journal 2014 107, 1352-1363DOI: (10.1016/j.bpj.2014.05.054) Copyright © 2014 Biophysical Society Terms and Conditions

Figure 5 Relation between membrane thickness and dipole potential, ψd. (A) (Left) A membrane is shown with disordered hydrocarbon chains, a relatively small width, low lipid dipolar packing density, and consequently a low ψd. (Right) The membrane has more ordered chains, a greater width, a higher dipole packing density, and consequently a higher ψd. Note: The dipoles shown in the lipid headgroup region represent the net dipole of all contributions to ψd, e.g., water dipoles, carbonyl dipoles, and charges on the headgroups themselves. They are not intended to represent the phosphocholine dipole alone. (B) Protein/membrane structural changes accompanying ion occlusion. (Left) The protein nonoccluded state is shown with a narrow hydrophobic thickness. This necessitates a deformation of surrounding lipid so that the lipid hydrocarbon chains are disordered and the membrane is thinned. The relatively low lipid packing density this produces is responsible for a low ψd. (Right) When the protein occludes ions, its hydrophobic thickness increases. This stretches the hydrocarbon chains of the lipids, increases the membrane thickness, and increases the lipid packing density; hence, ψd increases. Biophysical Journal 2014 107, 1352-1363DOI: (10.1016/j.bpj.2014.05.054) Copyright © 2014 Biophysical Society Terms and Conditions