Observing a Lipid-Dependent Alteration in Single Lactose Permeases

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Observing a Lipid-Dependent Alteration in Single Lactose Permeases Tetiana Serdiuk, Junichi Sugihara, Stefania A. Mari, H. Ronald Kaback, Daniel J. Müller  Structure  Volume 23, Issue 4, Pages 754-761 (April 2015) DOI: 10.1016/j.str.2015.02.009 Copyright © 2015 Elsevier Ltd Terms and Conditions

Structure 2015 23, 754-761DOI: (10.1016/j.str.2015.02.009) Copyright © 2015 Elsevier Ltd Terms and Conditions

Figure 1 Unfolding of LacY Using SMFS Reveals Two Classes of FD Curves (A) Schematic representation of SMFS with LacY in a phospholipid bilayer. Pushing the AFM stylus onto the protoliposomes unspecifically attaches the LacY terminal end to the stylus (left). Withdrawal of the cantilever increases the distance D between the AFM stylus and lipid membrane and applies a mechanical force F to the permease (middle). Further withdrawal of the AFM stylus induces the sequential unfolding of LacY (right). During this process, an FD curve is recorded. (B and C) Typical FD curves, each one corresponding to the unfolding of a single WT LacY from POPE:POPG lipid (ratio 3:1) membranes. FD curves show two classes of force peak patterns, which differ in whether they have not (B) or have (C) an additional force peak at distances ranging from 60 to 80 nm (gray shaded area). To increase the probability of attaching the C-terminal end to the AFM stylus, the C terminus of LacY was elongated by a 36-aa-long unstructured polyGly polypeptide followed by a His8-tag. SMFS experiments were performed in 50 mM potassium phosphate (KPi) (pH 7.2) and at 25°C. See also Figure S1. Structure 2015 23, 754-761DOI: (10.1016/j.str.2015.02.009) Copyright © 2015 Elsevier Ltd Terms and Conditions

Figure 2 LacY Reconstituted in POPE:POPG (Ratio 3:1) Membranes Shows One Major and One Minor Force Peak Pattern (A and B) Density plots of superimposed FD curves classified into the two distinct force peak patterns observed upon unfolding of WT LacY in PE:PG lipid membranes. WLC fits corresponding to the mean contour lengths of each force peak are represented by colored curves. n gives the number of classified superimposed and analyzed FD curves. (C and D) Contour length histogram of force peaks detected in class 1 (C) and class 2 (D) FD curves. Histograms were fitted with a Gaussian mixture model (Kawamura et al., 2013). Each colored Gaussian distribution gives the mean contour length of a force peak class. Ten force peak classes were found for the class 1 FD curves (A and C). Eleven force peak classes were found for the class 2 FD curves (B and D). The black solid line shows the sum of weighted contour lengths for all force peak classes. The dashed line represents the uniform baseline noise. Colored numbers at each WLC curve and histogram peak represent the mean contour length in aa ± SD. Structure 2015 23, 754-761DOI: (10.1016/j.str.2015.02.009) Copyright © 2015 Elsevier Ltd Terms and Conditions

Figure 3 LacY Reconstituted in POPG Membranes Shows Two Distinct Unfolding Patterns (A and B) Density plots of superimposed FD curves reveal two distinct force peak patterns matching either class 1 (A) or class 2 (B) FD curves. FD curves were recorded upon unfolding of WT LacY in PG membranes. WLC fits corresponding to the mean contour lengths of each force peak are represented by colored curves. n gives the number of classified, superimposed, and analyzed FD curves. (C and D) Contour length histogram of force peaks detected in class 1 (C) and class 2 (D) FD curves. Histograms were fitted with a Gaussian mixture model (Kawamura et al., 2013). Each colored Gaussian distribution gives the mean contour length of a force peak class. Ten force peak classes were found for the class 1 FD curves (A and C). Eleven force peak classes were found for the class 2 FD curves (B and D). The black solid line shows the sum of weighted contour lengths for all force peak classes. The dashed line represents the uniform baseline noise. Colored numbers at each WLC curve and histogram peak represent the mean contour length in aa ± SD. See also Figures S2 and S3. Structure 2015 23, 754-761DOI: (10.1016/j.str.2015.02.009) Copyright © 2015 Elsevier Ltd Terms and Conditions

Figure 4 Effect of PE and PG on the Stable Structural Segments in LacY (A and B) Structural segments were mapped to the secondary structures of WT LacY in native (A) and inverted (B) topologies. Stable structural segments mapped in (A) and (B) were detected in the class 1 and class 2 FD curves, respectively. (A) Secondary structure model of LacY (PDB ID code 1PV7) mapped with 10 (class 1 FD curves) structural segments S1–S10 (native topology) and (B) with 11 (class 2 FD curves) structural segments S1–S4, S5∗, S6∗, S6∗∗, S7∗, S8, S9, S10 (inverted topology). Each mean contour length of a force peak class (see histograms of Figures 2 and 3) assigns the beginning of a structural segment (arrows pointing to aa). The numbers at arrows show the mean contour lengths of a force peak class (in aa), numbers in square brackets indicate the aa position counted from the C-terminal end, and numbers in parentheses give the aa position from the N-terminal end. Each of these numbers distinguishes the end of the previous and the beginning of the next stable structural segment. The length of polyGly tag and His-tag was considered for mapping. If the beginning/end of a stabilizing structural segment locates on the mica-facing side of the membrane or within the membrane, the thickness of the membrane is taken into account. Transmembrane helices are labeled I to XII, cytoplasmic loops are labeled C1 to C5, and periplasmic loops are labeled P1 to P6. Structure 2015 23, 754-761DOI: (10.1016/j.str.2015.02.009) Copyright © 2015 Elsevier Ltd Terms and Conditions

Figure 5 Schematic Model of the Free Energy Landscape of the Native and Inverted LacY Topology in the Presence and Absence of PE In the mixture of PE and PG (ratio 3:1), LacY preferably (95%) shows the native fold required for lactose transport. The free energy landscape (red landscape), which has been adapted according to Bogdanov and Dowhan (2012), is shaped so that the inverted topology is rarely adopted by LacY (5%). In the absence of PE (blue landscape), the anionic PG alters the energy landscape of LacY so that native and inverted topologies become energetically favorable. Thus, embedded in PG, the probabilities of LacY adopting the native or the inverted conformation are almost equal. Values give the probabilities of detecting one or both LacY topologies. Structure 2015 23, 754-761DOI: (10.1016/j.str.2015.02.009) Copyright © 2015 Elsevier Ltd Terms and Conditions