## BACKGROUND: The purpose of this study was to explore further the functions of konjac glucomannan (KGM) in starch-based foods. Experiments were carried out using the mixed amylose/amylopectin/KGM system as a model. High-speed differential scanning calorimetry (hyper-DSC) with the support of high
Molecular weight effects on gelation and rheological properties of konjac glucomannan–xanthan mixtures
✍ Scribed by Dan Shen; Chao Wan; Shanjun Gao
- Publisher
- John Wiley and Sons
- Year
- 2010
- Tongue
- English
- Weight
- 211 KB
- Volume
- 48
- Category
- Article
- ISSN
- 0887-6266
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✦ Synopsis
Abstract
Fractions of konjac glucomannan (KGM) with various viscosity‐average molecular weights (M~v~) ranging from 4.00 × 10^5^ to 2.50 × 10^6^ were prepared by hydrolysis degradation in hydrochloride acid/ethanol. Effect of M~v~ of KGM on the critical gelation temperature (T~gel~) determined by Winter–Chambon criterion and the elasticity of KGM/xanthan mixed gels, a kind of binary gel formed by synergistic gelation, were investigated by dynamic viscoelastic measurements. It was shown that the value of T~gel~ of the gel was shifted to a higher temperature and the gel strength was enhanced when M~v~ of KGM was increased. The critical M~v~ (1.91 × 10^6^) was observed, above which the T~gel~ and elasticity of the mixed gels showed no or slight increase. It was suggested that T~gel~ and elasticity of KGM/xanthan mixed gels mainly depend on the structure of junction zones driven by the strong interaction between KGM and xanthan, which was gradually improved with increasing M~v~ of KGM. It was found that the critical strain and yield stress of the mixed gels increased monotonically with the increasing M~v~ of KGM. © 2009 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 48: 313–321, 2010
📜 SIMILAR VOLUMES
Weight-average molecular weight ðM w Þ and intrinsic viscosity ½h of six fractions for benzyl konjac glucomannan (B-KGM) were determined by laser light scattering and viscometry, and the Mark-Houwink equation was established to be ½h ¼ 2:08 £ 10 23 M 0:87 w ðcm 3 g 21 Þ in the M w range of from 4.42