Superhelical structure of apoA-I within nascent HDL revealed by SANS and HD-MS/MS. A, comparison of experimental SANS intensity from deuterated apoA-I-nascent HDL in 12% D2O buffer (black dotted line) with calculated intensity of the double superhelix model (blue line), solar flares model (green line), and belt model (red line). B, SANS low resolution structure of apoA-I reconstructed from the experimentally obtained scattering curve of nascent HDL (left) and the all-atom double superhelix model of apoA-I within nascent HDL (right). C, 12% D2O SANS shape (black), apoA-I in the double superhelix model (red-blue), and their overlap from a viewing angle that emphasizes the helical conformation of the protein; N termini are colored in dark red/blue and C termini in light red/blue. D, map of “patch” hydrophobicity of apoA-I within nascent HDL in the double superhelix model. Like the hydrophobic index, the patch hydrophobicity is in the range [0,1] and is determined for each amino acid residue by averaging the hydrophobic indices of neighboring residues (e.g. within 15 Å) located on the same side of protein, i.e. either inside (facing lipid) or outside (facing solvent) (79). E, correlation (R) between the experimentally measured deuterium incorporation factors (D0) for apoA-I peptic peptides from nascent HDL versus the predicted (calculated) D0 values for both the belt (open circle) and double superhelix (open triangle) models of nascent HDL. F, “goodness of fit” of the double superhelix, solar flares, and the belt models at the individual residue level. The probability correction factor (PCF) plotted on the y axis represents the multiplier needed to adjust the exchange probability of individual residues within the model to match that determined by hydrogen/deuterium exchange mass spectrometry studies. The dashed line at unity represents the probability correction factor of a given amino acid within the model that possesses a conformation with the same H/D exchange as observed by experimental measurement.