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. 2016 Nov 9;53(11):3960–3968. doi: 10.1007/s13197-016-2388-4

Table 3.

Rheological parameters modelling of 5× HUFR samples at the pH of maximum heat stability

Samplea Bingham Herschel–Bulkley Power Law T (°C)b Viscosity (mPa.s) at 50 s−1
σ0 (Pa) η (mPa.s) R2 σ0, Pa k η (mPa.s) R2 k n R2
5× TSC (6.6) 1.183 75.59 0.973 0.941 0.203 0.774 0.999 0.965 0.434 0.949 53.1 46.4
5× DSP (6.5) 0.962 54.86 0.978 0.782 0.143 0.781 0.999 0.766 0.419 0.941 55.5 35.2
5× DSP (6.6) 0.991 51.18 0.977 0.838 0.119 0.809 0.998 0.785 0.402 0.937 50.6 46.1
5× DSP (6.7) 0.802 64.20 0.966 0.580 0.202 0.735 0.999 0.679 0.470 0.962 53.1 42.6

aValues in parentheses shows the pH at which samples exhibited maximum heat stability

bT—Temperature corresponding to minimum viscosity