Comparison of apoA-I helical structure and stability in discoidal and spherical HDL particles by HX and mass spectrometry
Elucidation of apoA-I secondary structure in spherical plasma HDL particles is essential for understanding HDL structure and function at the molecular level. To provide this information, we have applied hydrogen exchange (HX) and mass spectrometry methods to compare apoA-I secondary structure in dis...
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doaj-c1819ae8aeb2452eb464c7ad4db5c4b12021-04-28T06:01:08ZengElsevierJournal of Lipid Research0022-22752013-06-0154615891597Comparison of apoA-I helical structure and stability in discoidal and spherical HDL particles by HX and mass spectrometryPalaniappan Sevugan Chetty0David Nguyen1Margaret Nickel2Sissel Lund-Katz3Leland Mayne4S.Walter Englander5Michael C. Phillips6Lipid Research Group, Gastroenterology, Hepatology, and Nutrition Division, Children's Hospital of Philadelphia, Philadelphia, PA 19104-4318; andLipid Research Group, Gastroenterology, Hepatology, and Nutrition Division, Children's Hospital of Philadelphia, Philadelphia, PA 19104-4318; andLipid Research Group, Gastroenterology, Hepatology, and Nutrition Division, Children's Hospital of Philadelphia, Philadelphia, PA 19104-4318; andLipid Research Group, Gastroenterology, Hepatology, and Nutrition Division, Children's Hospital of Philadelphia, Philadelphia, PA 19104-4318; andThe Johnson Research Foundation, Department of Biochemistry and Biophysics, Perelman School of Medicine at the University of Pennsylvania, Philadelphia, PA 19104-4318The Johnson Research Foundation, Department of Biochemistry and Biophysics, Perelman School of Medicine at the University of Pennsylvania, Philadelphia, PA 19104-4318To whom correspondence should be addressed; Lipid Research Group, Gastroenterology, Hepatology, and Nutrition Division, Children's Hospital of Philadelphia, Philadelphia, PA 19104-4318; and; To whom correspondence should be addressedElucidation of apoA-I secondary structure in spherical plasma HDL particles is essential for understanding HDL structure and function at the molecular level. To provide this information, we have applied hydrogen exchange (HX) and mass spectrometry methods to compare apoA-I secondary structure in discoidal (two apoA-I molecules/particle) and spherical (five apoA-I molecules/particle) HDL particles. The HX kinetics indicate that the locations of helical segments within the apoA-I molecules are the same in both discoidal and spherical HDL particles (approximately 10 nm hydrodynamic diameter). Helix stabilities in both types of particles are 3–5 kcal/mol, consistent with the apoA-I molecules being in a highly dynamic state with helical segments unfolding and refolding in seconds. For the spherical HDL, apoA-I fragments corresponding to residues 115–158 exhibit bimodal HX kinetics consistent with this segment adopting an inter-converting (on the timescale of tens of minutes) helix-loop configuration. The segment adopting this configuration in the 10 nm disc is shorter because the surface area available to each apoA-I molecule is apparently larger. Loop formation in the central region of the apoA-I molecule contributes to the ability of the protein to adapt to changes in available space on the HDL particle surface. Overall, apoA-I secondary structure is largely unaffected by a change in HDL particle shape from disc to sphere.http://www.sciencedirect.com/science/article/pii/S0022227520357151amphipathic α-helixcholesterollipoproteinphospholipidhydrogen exchange |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Palaniappan Sevugan Chetty David Nguyen Margaret Nickel Sissel Lund-Katz Leland Mayne S.Walter Englander Michael C. Phillips |
spellingShingle |
Palaniappan Sevugan Chetty David Nguyen Margaret Nickel Sissel Lund-Katz Leland Mayne S.Walter Englander Michael C. Phillips Comparison of apoA-I helical structure and stability in discoidal and spherical HDL particles by HX and mass spectrometry Journal of Lipid Research amphipathic α-helix cholesterol lipoprotein phospholipid hydrogen exchange |
author_facet |
Palaniappan Sevugan Chetty David Nguyen Margaret Nickel Sissel Lund-Katz Leland Mayne S.Walter Englander Michael C. Phillips |
author_sort |
Palaniappan Sevugan Chetty |
title |
Comparison of apoA-I helical structure and stability in discoidal and spherical HDL particles by HX and mass spectrometry |
title_short |
Comparison of apoA-I helical structure and stability in discoidal and spherical HDL particles by HX and mass spectrometry |
title_full |
Comparison of apoA-I helical structure and stability in discoidal and spherical HDL particles by HX and mass spectrometry |
title_fullStr |
Comparison of apoA-I helical structure and stability in discoidal and spherical HDL particles by HX and mass spectrometry |
title_full_unstemmed |
Comparison of apoA-I helical structure and stability in discoidal and spherical HDL particles by HX and mass spectrometry |
title_sort |
comparison of apoa-i helical structure and stability in discoidal and spherical hdl particles by hx and mass spectrometry |
publisher |
Elsevier |
series |
Journal of Lipid Research |
issn |
0022-2275 |
publishDate |
2013-06-01 |
description |
Elucidation of apoA-I secondary structure in spherical plasma HDL particles is essential for understanding HDL structure and function at the molecular level. To provide this information, we have applied hydrogen exchange (HX) and mass spectrometry methods to compare apoA-I secondary structure in discoidal (two apoA-I molecules/particle) and spherical (five apoA-I molecules/particle) HDL particles. The HX kinetics indicate that the locations of helical segments within the apoA-I molecules are the same in both discoidal and spherical HDL particles (approximately 10 nm hydrodynamic diameter). Helix stabilities in both types of particles are 3–5 kcal/mol, consistent with the apoA-I molecules being in a highly dynamic state with helical segments unfolding and refolding in seconds. For the spherical HDL, apoA-I fragments corresponding to residues 115–158 exhibit bimodal HX kinetics consistent with this segment adopting an inter-converting (on the timescale of tens of minutes) helix-loop configuration. The segment adopting this configuration in the 10 nm disc is shorter because the surface area available to each apoA-I molecule is apparently larger. Loop formation in the central region of the apoA-I molecule contributes to the ability of the protein to adapt to changes in available space on the HDL particle surface. Overall, apoA-I secondary structure is largely unaffected by a change in HDL particle shape from disc to sphere. |
topic |
amphipathic α-helix cholesterol lipoprotein phospholipid hydrogen exchange |
url |
http://www.sciencedirect.com/science/article/pii/S0022227520357151 |
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