Refolding of SDS-Unfolded Proteins by Nonionic Surfactants

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Presentation transcript:

Refolding of SDS-Unfolded Proteins by Nonionic Surfactants Jørn Døvling Kaspersen, Anne Søndergaard, Daniel Jhaf Madsen, Daniel E. Otzen, Jan Skov Pedersen  Biophysical Journal  Volume 112, Issue 8, Pages 1609-1620 (April 2017) DOI: 10.1016/j.bpj.2017.03.013 Copyright © 2017 Biophysical Society Terms and Conditions

Figure 1 Fits of βLG and different χSDS in C12E8. Data were fit with a linear combination of folded protein in presence of mixed micelles and SDS-unfolded protein in presence of pure NIS micelles, as described in Materials and Methods. Decreasing mole fraction from top to bottom with values given in the figure. To see this figure in color, go online. Biophysical Journal 2017 112, 1609-1620DOI: (10.1016/j.bpj.2017.03.013) Copyright © 2017 Biophysical Society Terms and Conditions

Figure 2 Results for βLG and SDS samples mixed with C12E8. (a) Part of the protein that is either folded (upper data points at low mole fractions) or unfolded around SDS micelles (lower data points at low mole fractions) is shown. (b) Near-UV CD data at 293 nm of βLG in micelles (data as a function of mole fraction) buffer (upper point at zero mole fraction), and in 25 mM C12E8 (lower point at zero mole fraction) are shown. (c) Shown here are CD spectra for pure βLG (black), βLG mixed with SDS and C12E8 at SDS mole fractions of 0.8 (curve with deepest minimum) and 0.37 (nearly coinciding with black curve), respectively. (d) The fraction of β-sheet (points going to zero at a mole fraction of 0.8), and λ222/λ208 ratio (upper points at high mole fractions) is given. Background shading in (a), (b), and (d) indicates whether the protein is mainly free in solution (right part) or bound to micelles (left part). To see this figure in color, go online. Biophysical Journal 2017 112, 1609-1620DOI: (10.1016/j.bpj.2017.03.013) Copyright © 2017 Biophysical Society Terms and Conditions

Figure 3 Results for βLG and SDS samples mixed with DDM. (a) Part of the protein that is either folded (upper data points at low mole fractions) or unfolded around SDS micelles (lower data points at low mole fractions) is shown. (b) Near-UV CD data at 293 nm of βLG in micelles (data as a function of mole fraction), buffer (lowest point at zero mole fraction), and in 25 mM DDM (upper data point at zero mole fraction) are shown. (c) Shown here are CD spectra for pure βLG (black), βLG mixed SDS, and DDM with SDS mole fraction of 0.5 (curve with deepest minimum) and 0.1 (nearly coinciding with black curve), respectively. (d) The fraction of β-sheet (points going to zero at a mole fraction of 0.6), and λ222/λ208 ratio (upper points at high mole fractions) is given. To see this figure in color, go online. Biophysical Journal 2017 112, 1609-1620DOI: (10.1016/j.bpj.2017.03.013) Copyright © 2017 Biophysical Society Terms and Conditions

Figure 4 Results for αLA and SDS samples mixed with C12E8. (a) Part of the protein that is either folded (data with highest data point at low mole fraction) or unfolded around SDS micelles (goes to unity at high mole fraction) from SAXS analysis is shown. (b) Near-UV CD data at 296 nm of αLA in micelles (data as a function of mole fraction) and buffer (point at zero mole fraction) are shown. (c) Shown here are CD spectra for pure αLA (black), and αLA mixed SDS and C12E8 with SDS mole fractions of 0.5 (curve with deepest minimum) and 0.1 (nearly coinciding with black curve), respectively. (d) λ222/λ208 ratio. To see this figure in color, go online. Biophysical Journal 2017 112, 1609-1620DOI: (10.1016/j.bpj.2017.03.013) Copyright © 2017 Biophysical Society Terms and Conditions

Figure 5 Results for αLA and SDS samples mixed with DDM. (a) Part of the protein that is either folded (highest data points at low mole fraction) or unfolded around SDS micelles (goes to unity at high mole fraction) from SAXS analysis is shown. (b) Near-UV CD data at 296 nm of αLA in micelles (data as a function of mole fraction), buffer (lowest point at zero mole fraction), and in DDM (highest point at zero mole fraction) are given. (c) Shown here are CD spectra for pure αLA (black), αLA mixed with DDM (second curve from top at 207 nm), and αLA mixed with SDS and DDM to SDS mole fractions of 0.5 (deepest minimum) and 0.1 (second curve from below at 207 nm), respectively. (d) λ222/λ208 ratio. To see this figure in color, go online. Biophysical Journal 2017 112, 1609-1620DOI: (10.1016/j.bpj.2017.03.013) Copyright © 2017 Biophysical Society Terms and Conditions

Figure 6 Results for LYZ and SDS samples mixed with C12E8. (a) Part of the protein that is either folded (upper data points at low mole fraction) or unfolded around SDS micelles (unity at high mole fraction) from SAXS analysis is shown. (b) Near-UV CD data at 296 nm of LYZ in micelles (data as function of mole fraction), buffer (lowest point, nearly covered, at zero mole fraction), and in C12E8 (upper point at zero mole fraction) are shown. (c) CD spectra for pure LYZ (black), LYZ-mixed SDS, and C12E8 with SDS mole fractions of 1 (with deepest minimum) and 0.1 (nearly coinciding with black curve above 202 nm), respectively, are given. (d) λ222/λ208 ratio. To see this figure in color, go online. Biophysical Journal 2017 112, 1609-1620DOI: (10.1016/j.bpj.2017.03.013) Copyright © 2017 Biophysical Society Terms and Conditions

Figure 7 Results from measurements and analysis of BSA and SDS samples mixed with C12E8. (a) Part of the protein that is either folded (data at unity at low mole fraction) or unfolded around SDS micelles (data at zero at low mole fraction) from SAXS analysis is shown. (b) Estimate of maximum particle diameter determined using IFT is given. (c) CD spectra for pure BSA (black) and BSA in mixed SDS-C12E8 micelles with an SDS mole fraction of 0.8 (upper curve near the minima) and 0.51 (middle curve), respectively, are given. (d) λ222/λ208 ratio. To see this figure in color, go online. Biophysical Journal 2017 112, 1609-1620DOI: (10.1016/j.bpj.2017.03.013) Copyright © 2017 Biophysical Society Terms and Conditions