Laser‐excited raman spectroscopy of biomolecules. XII. Thermally induced conformational changes in poly(L‐glutamic acid)

Abstract

AbstractThe α‐helical from of poly(L‐glutamic acid) [α‐poly(Glu)] gives rise to the same amide I and III lines as α‐poly(γ‐benzyl‐L‐glutamate) at 1652 and 1296 cm−1, respectively. The latter is a superposition of the amide III line near 1290 cm−1 and a line deu to vibrational made of CH2 groups of the side chain near 1300 cm−1. A line at 924 cm−1 is tentatively identified as characteristics of α‐poly(Glu). Both the β1‐ and β2‐ forms of poly(Glu) give rise to characteristic of β‐amide. III frequencies that are similar because of their similar backbone structures. Differences in the conformations of their side chains and in the environments of the backbone are reflected in the region 800–1200 cm−1 and in the amide I. A line at 1042 cm−1 and a pair at 1021 and 1059 cm−1 are tentatively assigned as characteristic of β1‐poly(Glu) and β2‐poly(Glu), respectively. The α‐β2 transition in poly(L‐Glu78L‐Val22) is shown by the appearance of all the β2‐characteristic lines in the thermally transformed sample. The same features observed in poly(L‐Glu95L‐Val5) also indicate that the α‐β2 transition of poly(Glu) is facilitated by the presence of L‐valine and that the content of L‐valine is not critical for this purpose. Investigation of the Raman spectra of the calcium, strontium, barium and sodium slats of poly(Glu) shows that these salts, under the conditions of preparation used, all the have random‐coil conformations.