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Modern Polymer Spect..

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5.4 Polvpeptida 259<br />

Figure 5-2. Antiparallelchain<br />

pleated sheet of<br />

polyi L-alanine). The CH;<br />

group is represented by<br />

the largest circle. (From<br />

[51)<br />

Figure 5-3. Antiparallelchain<br />

rippled sheet of<br />

polyglycine. (From [5])<br />

produce such a regular alternation with other side-chain-residue polypeptides.)<br />

Thus, in principle we can have antiparallel-chain pleated sheet (APPS) (Figure 5-2),<br />

antiparallel-chain rippled sheet (APRS) (Figure 5-3), parallel-chain pleated sheet<br />

(PPS), and parallel-chain rippled sheet (PRS) extended-chain structures. Their<br />

structural parameters are given in Table 5-5 [82].<br />

In describing these structures, and in the vibrational analyses, we assume the<br />

sheets to be infinite in two dimensions and therefore calculate only the in-phase unit<br />

cell modes. Although modes of only a single sheet are treated, the TDC interactions<br />

have been evaluated over a number of sheets (7-11). The effect of finiteness of a<br />

single sheet on just the TDC interactions for the amide I mode has been examined<br />

[83, 841.<br />

Extended-chain regions are a major component of protein structures. They can<br />

occui- in mixed antiparallel and parallel arrangements even within a sheet, the sheets<br />

can be twisted, and complex ‘barrel’ arrangements are also found [2]. It is therefore

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