The GROMOS96 molecular-dynamics (MD) program and force field was used to calculate the conformations at 298 K in CHCl 3 solution of two hexakis(3-hydroxyalkanoic acids). One consists of (R)-3-hydroxybutanoate (HB) residues only: HÀ(OCH(Me)ÀCH 2 ÀCO) 6 ÀOH (1). The other one carries the side chains of valine, alanine, and leucine: HÀ(OCH(CHMe 2 )CH 2 ÀCOÀOÀCH(Me)ÀCH 2 ÀCOÀOÀCH(CH 2 CHMe 2 )ÀCH 2 ÀCO) 2 ÀOH (2), with homochiral 3-hydroxyalkanoate (HA) moieties. In both cases, the conformational equilibria were sampled 2500 times for 25 ns. Other than clusters of arrangements with interresidual hydrogen bonding (between the O-and C-terminal OH and COOH groups, and with chain-bound ester carbonyl O-atoms; Fig. 6), there are no preferred backbone conformations in which the molecules 1 and 2 spend more than 5% of the time. Specifically, neither the 2 1 -nor the 3 1 -helical conformation of the oligoester backbone (found in stretched fibers, in lamellar crystallites, and in single crystals of polymers PHB and of oligomers OHB) is sampled to any significant extent ( Fig. 8 and 9), in spite of the high population, in both oligomers, of the (À)-synclinal conformation around the C(2)ÀC (3) bond (angle f 2 in Fig. 2). In contrast to b-oligopeptides, for which strongly preferred secondary structures are found after a few ns, and for which the number of conformations levels off with time, the number of conformational clusters of the corresponding oligoesters found by our force-field MD calculations increases steadily over the observation time of 25 ns (Fig. 5). Thus, the conclusion from biological and physical-chemical studies, according to which the PHB chain is extremely flexible, is confirmed by our computational investigation: in CHCl 3 solution, the hexakis(3-hydroxyalkanoate) chain samples its conformational space randomly! 1. Introduction. ± Associated with the biological role of the short-chain poly[(R)-3-hydroxybutanoate] (PHB) [1], which has been shown to allow the passage of ions across phospholipid bilayer membranes under voltage-driven and concentration-driven conditions [2], or to function as a transmembrane ion-channel when associated with Ca polyphosphate [1 ± 3], is the question of its secondary structure. From the investigation of PHB or PHB derivatives in the solid state, two different folding patterns were recognized: a 2 1 helix in stretched fibers [4] and in lamellar crystallites of the polymer