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Original Article

Application of high-intensity ultrasound to modify the rheological properties of a guamuchil Pithecellobium dulce (Roxb.) seed protein isolate

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Pages 739-751 | Received 07 Dec 2022, Accepted 16 Feb 2023, Published online: 24 Feb 2023

Figures & data

Figure 1. Impact of high-intensity ultrasound on the moduli of storage G’ (A) and loss G” (B) of guamuchil protein isolate in function of strain sweep. For each treatment the numerator and denominator represent the power and time of exposure to ultrasound, respectively.

Figure 1. Impact of high-intensity ultrasound on the moduli of storage G’ (A) and loss G” (B) of guamuchil protein isolate in function of strain sweep. For each treatment the numerator and denominator represent the power and time of exposure to ultrasound, respectively.

Figure 2. Impact of high-intensity ultrasound on the moduli of storage G’ (A) and loss G” (B) of guamuchil protein isolate as function of frequency sweep. For each treatment the numerator and denominator represent the power and time of exposure to ultrasound, respectively.

Figure 2. Impact of high-intensity ultrasound on the moduli of storage G’ (A) and loss G” (B) of guamuchil protein isolate as function of frequency sweep. For each treatment the numerator and denominator represent the power and time of exposure to ultrasound, respectively.

Figure 3. Impact of high-intensity ultrasound on the moduli of storage G’ (A) and loss G” (B), and loss tangent of guamuchil protein isolate as function of temperature sweep. For each treatment the numerator and denominator represent the power and time of exposure to ultrasound, respectively.

Figure 3. Impact of high-intensity ultrasound on the moduli of storage G’ (A) and loss G” (B), and loss tangent of guamuchil protein isolate as function of temperature sweep. For each treatment the numerator and denominator represent the power and time of exposure to ultrasound, respectively.

Figure 4. Effect of ultrasound on the apparent viscosity (ηapp) of guamuchil protein isolate as function of shear rate (γ).

Figure 4. Effect of ultrasound on the apparent viscosity (ηapp) of guamuchil protein isolate as function of shear rate (γ).

Table 1. Impact of high-intensity ultrasound on η0 (zero viscosity), η (infinity viscosity), m* (rate constant), and 1/C (critical shear rate) parameters of guamuchil protein isolate generated by Cross model.