Abstract:Abstract. Doughs from three flours were sheared between a cone and plate at constant rates in the range 6 times 10‐4‐2 times 10‐2 s‐1.
At temperatures between 25 and 40d̀C, the apparent viscosity decreased with increasing temperature and with increasing rate of shear. The effects of the temperature and of the rate of shear were independent one of another, and can be described by an Arrhenius type equation and a power equation, respectively. At temperatures between 45 and 60d̀C, the apparent viscosity increased… Show more
“…Law established from data acquired on crumb of gas fraction 0.7-0.8 and at ambient temperature (Rask, 1989;Zanoni et al, 1995) m g Kinematic viscosity of gas m 2 s À1 3 Â 10 À5 g Bulk dough viscosity Pa s g o = 450 g f = 4.5 Â 10 6 Bloksma and Nieman (1975) q dm Z Density of dry matter kg m À3 1800 Rask (1989) q w.liq Z Density of liquid water kg m À3 1000 Perry and Chilton (1973) s Tortuosity of liquid phase due to presence of bubbles p/2 Heat transfer is characterized by a global heat transfer coefficient, h bot, and the air temperature under the plate of the oven, T bot .…”
“…Law established from data acquired on crumb of gas fraction 0.7-0.8 and at ambient temperature (Rask, 1989;Zanoni et al, 1995) m g Kinematic viscosity of gas m 2 s À1 3 Â 10 À5 g Bulk dough viscosity Pa s g o = 450 g f = 4.5 Â 10 6 Bloksma and Nieman (1975) q dm Z Density of dry matter kg m À3 1800 Rask (1989) q w.liq Z Density of liquid water kg m À3 1000 Perry and Chilton (1973) s Tortuosity of liquid phase due to presence of bubbles p/2 Heat transfer is characterized by a global heat transfer coefficient, h bot, and the air temperature under the plate of the oven, T bot .…”
“…A Weissenberg R 18 Rheogoniometer was used, (a brief description is given here; a more detailed description is given by Bloksma and Nieman [27]). The apparatus consisted of a cone (top) and a plate (bottom), both having a radius of 37.52 ram.…”
A b s t r a c # The rheological properties of rennet-induced skim milk gels were determined by two methods, i.e., via stress relaxation and dynamic tests. The stress relaxation modulus Gc(t ) was calculated from the dynamic moduli G' and G" by using a simple approximation formula and by means of a more complex procedure, via calculation of the relaxation spectrum. Either calculation method gave the same results for Go(t). The magnitude of the relaxation modulus obtained from the stress relaxation experiments was 10% to 20% lower than that calculated from the dynamic tests.Rennet-induced skim milk gels did not show an equilibrium modulus. An increase in temperature in the range from 20 ° to 35 °C resulted in lower moduli at a given time scale and faster relaxation. Dynamic measurements were also performed on acid-induced skim milk gels at various temperatures and Gc(t) was calculated. The moduli of the acid-induced gels were higher than those of the rennet-induced gels and a kind of "permanent" network seemed to exist, also at higher temperatures.
“…The fact that two apparently equivalent doughs, proofed to the same height, can produce loaves of significantly different volumes suggests that the temperature-dependent changes that occur during baking may define or determine flour quality. Despite the fact that there is, a priori, no reason to presume that only those changes occurring prior to baking are relevant, little data exist on the fundamental rheological properties of doughs during heating (Bloksma and Nieman, 1975;LeGrys et aI., 1980;Dreese et aI., 1988aDreese et aI., , 1988c. This lack of data may be because of the inherent difficulty in heating a dough mass uniformly while at the same time testing it.…”
It should be evident that cereal scientists need to be able to measure and understand the fundamental mechanical properties of wheat flour doughs. Restated more precisely, the goal is to understand the relationships between the forces acting on dough, its subsequent deformation, and time. This goal has been the impetus for a great deal of research over the past 60 years. Several recent reviews (Hlynka, 1970;Hibberd and Parker, 1975b;Baird, 1983;Faubion et al. 1985; Faubion and Faridi, 1986) present the rationale for applying fundamental rheological tests to investigate the mechanical properties of dough. Bushuk (1985) sums up this rationale concisely:In breadmaking, the dough undergoes some type of deformation in every phase of the process. During mixing, dough undergoes extreme deformations beyond the rupture limits; during fermentation the deformations are much smaller; during sheeting and shaping, deformations are of an intermediate level; and finally during proofing and baking, dough is subjected to more deformations. Accordingly. the application of rheological concepts to the behavior of doughs seems a natural requirement of research on the interrelationships among flour composition. added ingredients, process parameters and the characteristics of the loaf of bread.The process of generating the data necessary to characterize the rheology of dough is far from complete, because of the difficulty of determining the material properties of systems as complex as wheat flour doughs. If determining the material properties were simple, most (if not all) of the required information would now be in hand. Of the large body of research that exists on the rheological properties of wheat flour doughs, the great portion is empirical rather than fundamental in nature. It is important to bear in mind, however, Contribution No. 89-32S-B from the Kansas Agricultural Experiment Station. 29 H. Faridi et al. (eds.), Dough Rheology and Baked Product Texture
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