THESIS
THESIS
THESIS
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calorimetry (DSC) (Russell, 1983; Mua and Jackson, 1995), Fourier transform<br />
infrared spectroscopy (FT-IR) (Van et al. 1994) or Raman spectroscopy (Bulkin et al.<br />
1987) and rheological techniques (Doublier and Choplin, 1989; Mita, 1992).<br />
1) Retrogradation measured by X-ray diffraction<br />
Early X-ray diffraction studied on aged starch gels showed that<br />
the B-type diffraction pattern developed slowly (Zobel, 1973). Crystal growth, as<br />
detected by X-ray diffraction, is slower than formation of the gel network and has<br />
been proposed as occurring in the polymer-rich regions of the gel (Miles et al.,<br />
1985a). For both amylose and starch gel, the initial development of crystallinity<br />
occurred at similar rate. However, the crystallization of amylose effectively reached a<br />
limit rates. However, the crystallization of amylose effectively reached a limit after 2<br />
days whereas the crystallinity of the starch gel continued to increase (Miles et al.<br />
1985b). The amylopectin gels show only a slow increase in crystallinity with time and<br />
approach a limiting value after 30-40 days (Ring et al. 1987). Isolated gelatinized<br />
starch granules that have been washed free from all exudates amylose gave no X-ray<br />
diffraction pattern immediately after cooling. After two weeks of storage, the B-type<br />
pattern is obtained. Amylose gels are firm, white and opaque. They can withstand<br />
autoclave at 130 o C. Retrograded amylose gives the B-type starch X-ray diffraction<br />
pattern. Early X-ray diffraction analysis of stretched amylose film in the B-type<br />
structure was interpreted in terms of a six fold single helix structure with a repeat<br />
distance of 10.4 °A. On this basis it could be postulated that the mechanism of cross<br />
linking amylose gels was via junction zones of aggregated single helices. From<br />
studies on Naegeli amylodextrins, however, Kainuma and French (1972) proposed a<br />
model for B-type starch comprising intertwined double helices. This proposal has<br />
recently been confirmed by X-ray diffraction studies (Wu and Sarko, 1978) as showed<br />
in Figure 11. This most recent crystal structure of the B-polymorph of amylose is<br />
based on double stranded helices. The individual strands are in a six fold helical<br />
conformation repeating in 20.8 Å, and are wound parallel around each other. In the<br />
case, however, the X-ray data cannot reliably distinguish between right and lefthanded<br />
models (Cheetham and Tao (1998).<br />
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