Each of the structures generated by the NMR study was used as the starting structure for an independent simulation. The N-acetyl galactosylated peptides were each run twice, with different random number sets to ensure they sampled different conformational spaces. Thus, there were 2x16 GalNAc runs, 36 Man runs and 48 for the unglycosylated peptide, for a total of 116. Each initial structure was treated in the manner described below. Some runs were not completed when the data presented here were extracted for analysis (27 December, 2012). AMBER prmtop and inpcrd input files were generated using the tleap utility in AmberTools12. Each PDB file provided by the NMR software was used as initial input. To it were added sufficient chloride counter ions to ensure neutrality. The neutralized system was solvated using small, pre-equilibrated boxes of TIP3P water to form a solvent buffer of at least 10 Angstroms from each atom in the system. To ensure free movement, the box was increased so that it was approximately cubic, using the longest initial dimension as the target for all dimensions. The peptide portions of the molecule were modeled using the ff12SB force field, the ions were modeled using the ions08 parameters, and the monosaccharides were modeled using GLYCAM_06h-1 with GLYCAM_06h-12SB amino acid atom types. The complete set of parameters and setup files are available upon request from author Foley. Each simulation was begun with a steepest-descent minimization for 10,000 steps. The time step for all subsequent phases was 0.002 ps, and bonds involving hydrogen were constrained according to the SHAKE algorithm. The systems were run in the NTP ensemble using Particle Mesh Ewald to treat electrostatics. Next, the system was heated gently in 20,000 steps (40 ps) from 5 to 300 K at 1 atm using the weak-coupling algorithm. In the equilibration and production phases, the temperature was maintained at 300 K using Langevin dynamics. After heating, the systems were allowed to equilibrate for 2 ns before beginning a 100 ns production phase. Due to simulation restarts, a few systems ran slightly longer. System coordinates were saved every 5000 steps (10 ps) during the production phase. The results presented here are from the final, production phases, and unless otherwise noted represent the collected data from each set of runs.