Tag: HS-AFM height spectroscopy

Correlation of membrane protein conformational and functional dynamics

Membrane proteins (MPs) reside in the plasma membrane and perform various biological processes including ion transport, substrate transport, and signal transduction.*

Function-related conformational changes in membrane proteins occur in times scales ranging from nanoseconds to seconds.*

Obtaining time-resolved dynamic information of MPs in their membrane environment is still a major challenge.*

Although High Speed Atomic Force Microscopy (HS-AFM) images label-free samples such as DNA, soluble proteins, MPs, and intrinsically disordered proteins at ~1n~m lateral, ~0.1 nm vertical and ~100 ms temporal solution in aqueous environment and at ambient temperature and pressure, its temporal resolution is too slow to characterize many dynamic biological processes.*

In order to overcome this limitation Raghavendar Reddy Sanganna Gari, Joel José Montalvo-Acosta, George R. Heath, Yining Jiang, Xiaolong Gao, Crina M. Nimigean, Christophe Chipot and Simon Scheuring in their article Correlation of membrane protein conformational and functional dynamics use High Speed Atomic Force Microscopy Height Spectroscopy ( HS-AFM-HS) to characterize the microsecond timescale conformational changes of an integral-MP model system, i.e., the outer membrane protein G (OmpG) in a membrane environment.*

The positioning of the AFM tip is guided by HS-AFM imaging immediately before HS-AFM-HS-operation.*

NanoWorld Ultra-Short Cantilevers (USC) of the USC-F1.2-k0.15 type were used for the HS-AFM and HS-AFM-HS presented in the article.*

Figure 1 from “Correlation of membrane protein conformational and functional dynamics” by R.R. Sanganna Gari et al: HS-AFM imaging of OmpG in lipid bilayers at pH 7.6 and pH 5.0. a OmpG at pH 7.6 (Supplementary movie 1, left; frame rate: 200 ms per frame). A OmpG dimer is highlighted with dashed outline in all frames. Arrowheads in t = 11.6 s: Loop-6 fluctuating over the lumen. Arrowhead in t = 12.0 s: Fully open state. b Correlation average (n = 2752) of the HS-AFM movie frames (344 frames recorded over 68.8 s, full color scale: 0.0 nm < height < 1.25 nm, where the membrane level was set to 0.0 nm). c Correlation average of OmpG dimers. The topography outline (based on the molecular structure in 1e), serves as a visual guide to locate loop-6 and loop-2 in the topography and is highlighted by the dashed outline (the position of loop-6 is indicated by the asterisk based on its location in the structure (e)). Inner dashed outline show barrel lumen. d Standard deviation (std) map (n = 2752) from the averaging process in (b) (full color scale from blue to red: 0.05 nm < std < 0.19 nm) and topography outlines as in (c). e X-ray structure (PDB 2iwv) of the open OmpG conformation. Loop-6 (arrowhead L6) stands out of the image plane towards the viewer. Loop-2 (L2) forms a beta strand pointing away from the β-barrel, well detected by HS-AFM in the open state (b). f OmpG at pH 5.0 (Supplementary movie 1, right; frame rate: 200 ms per frame). A OmpG dimer is highlighted with dashed outline in all frames. g Correlation average (n = 2472) of the HS-AFM movie frames (309 frames recorded over 61.8 s, full color scale: 0.0 nm < height < 0.7 nm, where the membrane level was set to 0.0 nm). h Correlation average of OmpG dimers. For comparison, the topography outline of the open state (e) is shown (the position of loop-6 is indicated by the asterisk). i Standard deviation (std) map (n = 2472) from the averaging process in (g) (full color scale from blue to red: 0.04 nm < std < 0.07 nm) and topography outlines as in (h). j X-ray structure (PDB 2iww) of the closed OmpG conformation shown in the same orientation as in (e). Loop-6 (L6) folds over the β-barrel lumen in a lid-like manner. Loop-2 (L2) does not form a β-strand in the closed state, in agreement with absence of topography in this region in (h). Black dashed line: outline based on (e) for comparison. NanoWorld USC-F1.2-k0.15 AFM probes were used for the HS-AFM.
Figure 1 from “Correlation of membrane protein conformational and functional dynamics” by R.R. Sanganna Gari et al:
HS-AFM imaging of OmpG in lipid bilayers at pH 7.6 and pH 5.0.
a OmpG at pH 7.6 (Supplementary movie 1, left; frame rate: 200 ms per frame). A OmpG dimer is highlighted with dashed outline in all frames. Arrowheads in t = 11.6 s: Loop-6 fluctuating over the lumen. Arrowhead in t = 12.0 s: Fully open state. b Correlation average (n = 2752) of the HS-AFM movie frames (344 frames recorded over 68.8 s, full color scale: 0.0 nm < height < 1.25 nm, where the membrane level was set to 0.0 nm). c Correlation average of OmpG dimers. The topography outline (based on the molecular structure in 1e), serves as a visual guide to locate loop-6 and loop-2 in the topography and is highlighted by the dashed outline (the position of loop-6 is indicated by the asterisk based on its location in the structure (e)). Inner dashed outline show barrel lumen. d Standard deviation (std) map (n = 2752) from the averaging process in (b) (full color scale from blue to red: 0.05 nm < std < 0.19 nm) and topography outlines as in (c). e X-ray structure (PDB 2iwv) of the open OmpG conformation. Loop-6 (arrowhead L6) stands out of the image plane towards the viewer. Loop-2 (L2) forms a beta strand pointing away from the β-barrel, well detected by HS-AFM in the open state (b). f OmpG at pH 5.0 (Supplementary movie 1, right; frame rate: 200 ms per frame). A OmpG dimer is highlighted with dashed outline in all frames. g Correlation average (n = 2472) of the HS-AFM movie frames (309 frames recorded over 61.8 s, full color scale: 0.0 nm < height < 0.7 nm, where the membrane level was set to 0.0 nm). h Correlation average of OmpG dimers. For comparison, the topography outline of the open state (e) is shown (the position of loop-6 is indicated by the asterisk). i Standard deviation (std) map (n = 2472) from the averaging process in (g) (full color scale from blue to red: 0.04 nm < std < 0.07 nm) and topography outlines as in (h). j X-ray structure (PDB 2iww) of the closed OmpG conformation shown in the same orientation as in (e). Loop-6 (L6) folds over the β-barrel lumen in a lid-like manner. Loop-2 (L2) does not form a β-strand in the closed state, in agreement with absence of topography in this region in (h). Black dashed line: outline based on (e) for comparison.
Figure 2 from “Correlation of membrane protein conformational and functional dynamics” by R.R. Sanganna Gari et al: Single channel electrophysiology and HS-AFM height spectroscopy recordings of OmpG in lipid bilayers. Representative 60-ms segments of OmpG single channel recordings at pH 7.6 (a) and pH 5.0 (b) at +40 mV membrane potential (longer traces in Supplementary Figs. 2 and 3). Cartoon representation of single channel recording experimental setup is shown in inset of (a). OmpG (yellow) in open state (PDB:2IWV) is placed in a lipid bilayer (green) surrounded by buffer (light blue shade) and potassium and chloride ions are shown as red and blue spheres. Red arrow indicates ion flow through OmpG in response to voltage application. Dwell time histograms of open and closed states at pH 7.6 (c) and pH 5.0 (d) from single-channel recordings (see Supplementary Table 1). Representative 60-ms segments of OmpG HS-AFM-HS recordings at pH 7.6 (e) and pH 5.0 (f) (longer traces in Supplementary Fig. 4). Cartoon representation of HS-AFM height spectroscopy experimental setup is shown in inset of (e). An oscillating AFM tip (orange) detects conformational changes of loop motion. Dwell time histograms of open and closed states at pH 7.6 (g) and pH 5.0 (h) from HS-AFM-HS recordings (Supplementary Table 2). In HS-AFM-HS the low state represents the open state, where the HS-AFM tip can descend into the β-barrel, and the high state represents the closed state, where loop-6 covers the beta barrel barring access of the HS-AFM tip to the cavity. All current-time and height-time traces were filtered at 20 kHz during analysis. The state dwell-time histograms are shown using log binning for better visualization of the components49. Red traces in (a) and (b) represent idealized current-time traces using clampfit software. Red traces in (e) and (f) represent idealized height-time traces using the STaSI algorithm (see Methods). NanoWorld USC-F1.2-k0.15 AFM probes were used for the HS-AFM-HS.
Figure 2 from “Correlation of membrane protein conformational and functional dynamics” by R.R. Sanganna Gari et al:
Single channel electrophysiology and HS-AFM height spectroscopy recordings of OmpG in lipid bilayers.
Representative 60-ms segments of OmpG single channel recordings at pH 7.6 (a) and pH 5.0 (b) at +40 mV membrane potential (longer traces in Supplementary Figs. 2 and 3). Cartoon representation of single channel recording experimental setup is shown in inset of (a). OmpG (yellow) in open state (PDB:2IWV) is placed in a lipid bilayer (green) surrounded by buffer (light blue shade) and potassium and chloride ions are shown as red and blue spheres. Red arrow indicates ion flow through OmpG in response to voltage application. Dwell time histograms of open and closed states at pH 7.6 (c) and pH 5.0 (d) from single-channel recordings (see Supplementary Table 1). Representative 60-ms segments of OmpG HS-AFM-HS recordings at pH 7.6 (e) and pH 5.0 (f) (longer traces in Supplementary Fig. 4). Cartoon representation of HS-AFM height spectroscopy experimental setup is shown in inset of (e). An oscillating AFM tip (orange) detects conformational changes of loop motion. Dwell time histograms of open and closed states at pH 7.6 (g) and pH 5.0 (h) from HS-AFM-HS recordings (Supplementary Table 2). In HS-AFM-HS the low state represents the open state, where the HS-AFM tip can descend into the β-barrel, and the high state represents the closed state, where loop-6 covers the beta barrel barring access of the HS-AFM tip to the cavity. All current-time and height-time traces were filtered at 20 kHz during analysis. The state dwell-time histograms are shown using log binning for better visualization of the components49. Red traces in (a) and (b) represent idealized current-time traces using clampfit software. Red traces in (e) and (f) represent idealized height-time traces using the STaSI algorithm (see Methods).

*Raghavendar Reddy Sanganna Gari, Joel José Montalvo-Acosta, George R. Heath, Yining Jiang, Xiaolong Gao, Crina M. Nimigean, Christophe Chipot and Simon Scheuring
Correlation of membrane protein conformational and functional dynamics
Nature Communications volume 12, Article number: 4363 (2021)
DOI: https://doi.org/10.1038/s41467-021-24660-1

Please follow this external link to read the full article: https://rdcu.be/cAE2S

Open Access : The article “Correlation of membrane protein conformational and functional dynamics” by Raghavendar Reddy Sanganna Gari, Joel José Montalvo-Acosta, George R. Heath, Yining Jiang, Xiaolong Gao, Crina M. Nimigean, Christophe Chipot and Simon Scheuring is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit https://creativecommons.org/licenses/by/4.0/.

High-speed AFM height spectroscopy reveals microsecond-dynamics of unlabeled biomolecules

In their recent publication “High-speed AFM height spectroscopy reveals μs-dynamics of unlabeled biomolecules” in Nature Communications George R. Heath and Simon Sheuring develop and apply HS-AFM height spectroscopy (HS-AFM-HS, a technique inspired by fluorescence spectroscopy), a technique whereby the AFM tip is held at a fixed x–y position and  the height fluctuations under the tip in z-direction with Angstrom spatial and 10µs temporal resolution are monitored.

They demonstrate “how this technique can be used to simultaneously measure surface concentrations, diffusion rates and oligomer sizes of highly mobile annexin-V molecules during membrane-binding and self-assembly at model membranes and derive its kinetic and energetic terms. Additionally, HS-AFM-HS at specific positions in the annexin lattice where the freedom of movement is restricted to rotation allowed determination of the interaction free energies of protein-protein contacts.”* The applicability of this technique is wide and is discussed at the end of the publication.

NanoWorld Ultra-Short Cantilevers (USC) for Fast-/High-Speed AFM  ( USC-F1.2-k0.15 ) were used.

Congratulations to the authors to this publication which pushes the speed limits of AFM even further!

Increasing the temporal resolution of HS-AFM by reducing the dimensionality of data acquisition. a HS-AFM image of a DOPC/DOPS (8:2) membrane in the presence of annexin-V and NP-EGTA-caged Ca2+. Blue arrows illustrate the slow- (vertical) and the fast-scan axis (horizontal). Images can be captured at up to 10–20 frames s−1. b HS-AFM movie frames of A5 membrane-binding, self-assembly and formation of p6 2D-crystals upon UV-illumination induced Ca2+-release. c Average height/time trace of the membrane area in b. d Averaged HS-AFM image of an A5 p6-lattice overlaid with the subsequent line scanning kymograph, obtained by scanning repeatedly the central x-direction line as illustrated by the blue arrow with a maximum rate of 1000–2000 lines s−1. e Line scanning kymograph across one protomer of the non-p6 trimer, marked by * in d and e at a rate of 417 lines s−1 (2.4 ms per line). f Histogram of state dwell-times of the molecule in e. g HS-AFM image of an A5 p6-lattice partially covering a DOPC/DOPS (8:2) SLB surface during self-assembly. HS-AFM height spectroscopy (HS-AFM-HS) is performed following halting the x- and y-piezos to capture height information at a fixed position at the center of the image (illustrated by the target). h Schematic showing the principle of HS-AFM-HS. The AFM tip is oscillated in z at a fixed x,y-position, detecting single molecule dynamics such as diffusion under the tip. i Height/time trace obtained by HS-AFM-HS with the tip positioned at the center of image (g). The height/time trace allows determination of the local A5 concentration analyzing the time fraction of the occurrence of height peaks. j Dwell-time analysis of each height peak of diffusing A5 from 60 s height/time data and subsequent fitting of the distribution to multiple Gaussians (possible molecular aggregates corresponding to the fits with distinct dwell-times (τD) are shown above the graph). All scale bars: 20 nm, NanoWorld Ultra-Short Cantilevers (USC) for Fast-/High-Speed AFM ( USC-F1.2-k0.15 ) were used.
Figure 1 from “High-speed AFM height spectroscopy reveals μs-dynamics of unlabeled biomolecules”: Increasing the temporal resolution of HS-AFM by reducing the dimensionality of data acquisition. a HS-AFM image of a DOPC/DOPS (8:2) membrane in the presence of annexin-V and NP-EGTA-caged Ca2+. Blue arrows illustrate the slow- (vertical) and the fast-scan axis (horizontal). Images can be captured at up to 10–20 frames s−1. b HS-AFM movie frames of A5 membrane-binding, self-assembly and formation of p6 2D-crystals upon UV-illumination induced Ca2+-release. c Average height/time trace of the membrane area in b. d Averaged HS-AFM image of an A5 p6-lattice overlaid with the subsequent line scanning kymograph, obtained by scanning repeatedly the central x-direction line as illustrated by the blue arrow with a maximum rate of 1000–2000 lines s−1. e Line scanning kymograph across one protomer of the non-p6 trimer, marked by * in d and e at a rate of 417 lines s−1 (2.4 ms per line). f Histogram of state dwell-times of the molecule in e. g HS-AFM image of an A5 p6-lattice partially covering a DOPC/DOPS (8:2) SLB surface during self-assembly. HS-AFM height spectroscopy (HS-AFM-HS) is performed following halting the x- and y-piezos to capture height information at a fixed position at the center of the image (illustrated by the target). h Schematic showing the principle of HS-AFM-HS. The AFM tip is oscillated in z at a fixed x,y-position, detecting single molecule dynamics such as diffusion under the tip. i Height/time trace obtained by HS-AFM-HS with the tip positioned at the center of image (g). The height/time trace allows determination of the local A5 concentration analyzing the time fraction of the occurrence of height peaks. j Dwell-time analysis of each height peak of diffusing A5 from 60 s height/time data and subsequent fitting of the distribution to multiple Gaussians (possible molecular aggregates corresponding to the fits with distinct dwell-times (τD) are shown above the graph). All scale bars: 20 nm

*George R. Heath & Simon Scheuring
High-speed AFM height spectroscopy reveals μs-dynamics of unlabeled biomolecules
Nature Communicationsvolume 9, Article number: 4983 (2018)
DOI: https://doi.org/10.1038/s41467-018-07512-3

Please follow this external link for the full article: https://rdcu.be/bdaKU

Open Access The article “High-speed AFM height spectroscopy reveals μ s-dynamics of unlabeled biomolecules” by George R. Heath & Simon Scheuring is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.