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P ptd 200 air

Manufactured by Anton Paar
Sourced in Austria

The P-PTD 200/AIR is a laboratory instrument designed for the determination of the phase transition temperature (PTT) of materials. It operates using the air pressure method and can measure PTT values in the range of -20 °C to 200 °C.

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3 protocols using p ptd 200 air

1

Viscosity Measurement of Fermented Samples

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An Anton Paar MCR 72 rheometer (Anton Paar, Graz, Austria), equipped with a Peltier plate-plate system (P-PTD 200/Air), was used to measure the viscosity of the samples both before and after fermentation. The samples were positioned between the two plates, the lower plate having a temperature control system set at 25 °C with a gap of 1 mm, and the upper plate having smooth parallel plate geometry of 50 mm diameter. To ensure thermal equilibrium before measurements, the sample surplus was taken out and permitted to rest for 10 min. With a linearly increasing shear rate from 5 to 300 1/s, each measurement was carried out twice.
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2

Rheological Characterization of Formulations

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The formulations’ rheological properties were studied using an MCR 92 modular compact rheometer (Anton Paar, Graz, Austria), equipped with a CP35-2 cone-plate sensor system (angle 2°, diameter 35 mm) and a P-PTD 200/AIR Peltier plate to keep the measurement temperature constant at 25 °C. Dynamic viscosity measurements were performed at shear rates between 0.01 and 1000 s−1. Frequency sweep analysis was performed at frequencies ranging from 0.01 to 10 Hz, for a constant strain of 0.1–1.0% that was well within the linear viscoelastic limit evaluated through preliminary amplitude sweep tests [14 (link)].
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3

Rheological Characterization of Emulsions

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The emulsions’ rheological properties were studied using an MCR 92 modular compact rheometer (Anton Paar, Graz, Austria), equipped with a PP50/S parallel plate geometry (diameter 50 mm) and a P-PTD 200/AIR Peltier plate to keep the measurement temperature constant at 25 °C. A steady-state flow ramp was used to determine flow curves for shear rates between 0.01 and 1000 s−1. The flow curves were fitted to the Cross model [16 (link),26 (link)]: η=η01+τγ˙m
where η is the apparent viscosity (Pa.s), η0 is the viscosity at zero shear rate (Pa.s), τ (s) is the relaxation time (s), and m is a dimensionless constant, related to the exponent of pow-er law (n) by m = 1 − n [13 (link),16 (link)]. Frequency sweep tests were performed with frequencies ranging from 0.01 to 16 Hz for a constant strain of 0.5% that was well within the linear viscoelastic limit (LVE) evaluated through preliminary amplitude sweep tests.
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