Squeezing flow of semi liquid foods between parallel Teflon coated plates

Citation
Mg. Corradini et al., Squeezing flow of semi liquid foods between parallel Teflon coated plates, RHEOL ACT, 39(5), 2000, pp. 452-460
Citations number
19
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
RHEOLOGICA ACTA
ISSN journal
00354511 → ACNP
Volume
39
Issue
5
Year of publication
2000
Pages
452 - 460
Database
ISI
SICI code
0035-4511(200010)39:5<452:SFOSLF>2.0.ZU;2-S
Abstract
Samples of commercial tomato paste, low fat mayonnaise and mustard about 6- 8 mm thick were squeezed to 0.8 mm at various speeds between 5 mm min(-1) a nd 25 mm min(-1) between Teflon-coated parallel plates 127 mm in diameter u sing an Instron UTM Model 5542. All the log force vs log height relationshi ps had a clearly identified linear region. This indicated that a dominant s queezing flow regime was achieved at about 3 mm height, and that the machin e has the proper stiffness to perform the tests. The stress level at a pre- selected height in this region is a measure of consistency, sensitive enoug h to distinguish between products of different brands. The residual stress after relaxation for about 2 min was on order of 10-50% of the initial stre ss, an indication that all three foods have a considerable structural integ rity. In all three products there was a considerable discrepancy between th e observed rate effects and predictions based on a pseudoplastic (power law ) model. It could be described by the empirical relation (F-nu1 - F-R)/(F ( nu2) - F-R) = (V-1/V-2)(m) where F-nu1 and F-nu2 are the forces at the give n displacement reached at speeds nu (1) and nu (2) respectively, F-R is the residual force after relaxation (found to be practically rate independent) , and m is a constant of the order of 0.15-0.33, independent of the compres sion velocities ratio but characteristic of the food and brand. The calcula ted elongational viscosity was not a unique function of biaxial strain rate . To a certain extent, this was probably due to imperfect lubrication. But it was also a manifestation of these products considerable structural integ rity which cannot be accounted for by models developed for ideal liquids.