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JUNGRO YOON RICHARD W. HARTEL YEN-CHUN WANG 《Journal of Food Processing and Preservation》1993,17(6):471-484
A flow through extraction reactor was used to study supercritical fraction-ation of butterfat. the rate of extraction of butterfat was constant for an initial period followed by a decreasing rate of extraction. DSC and GC analyses showed that more soluble triglycerides extracted preferentially in the initial stages exhibited lower melting behavior. the chemical and physical properties of the fractions changed with extraction time. Residual butterfat concentration in the bed was obtained as a function of distance from the bed entrance. the breakthrough curves had a sigmoidal shape, with the ascent-portion of the curves advancing through the bed with the degree of extraction. At the highest extents of extraction, the lower acyl carbon number triglycerides were totally depleted from the lowest portions of the bed, where fresh CO2 was introduced. 相似文献
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YEN-CHUN WANG RICHARD W. HARTEL JUNGRO YOON R. SELWYN JEBSON 《Journal of Food Processing and Preservation》1995,19(6):409-425
Extraction of milk fat in several high pressure solvents was compared. Solubility of milk fat in supercritical (SC) ethylene and liquid propane was compared to previous results in SC CO2 . At the same operating conditions (temperature and pressure), solubility of milk fat was higher in SC ethylene than in CO2 , although levels generally remained below 5% (w/w). This resulted in significantly higher solubility in SC ethylene when compared at equivalent solvent density. Very little fractionation of milk fat occurred in liquid propane over the range of pressures (3.45 to 5.52 MPa) and temperatures (30 to 90C) studied. Below 77.5C and 2.76 MPa, liquid propane and milk fat were miscible, while a slight fractionation was observed above these conditions. A high pressure sight-gage apparatus was used to visually confirm these conditions for separation. 相似文献
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Drying behavior of a single baking biscuit was modeled using unsteady state, anisotropic, two dimensional, simultaneous heat and mass balances. Solutions of these equations agreed well with the experimentally determined temperature and the moisture data. Modeling revealed that in the outer sections of the baking biscuit conduction and diffusion were the dominant heat and mass transfer mechanisms, respectively. In the central section of the biscuit the gas cells cracked with the increased vapor pressure and the upward volume expansion, then air/vapor enclaves were formed among the horizontal dough layers in the radial direction. the dominant heat and mass transfer mechanisms in the central section of the biscuit were convection. Presence of two different regime zones in a baking biscuit may have important consequences concerning the strength of the commercial products against crumbling during marketing and consumption. 相似文献
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Temperature and heat distribution studies were carried out in a single basket horizontal water cascading retort at two temperatures and two air over-pressure levels under fully loaded operating conditions. Various heat transfer parameters (heating and cooling rate indices, fh and fc), lag factors (jch and jcc) and process lethality (Fo) were used as indicators of the retort performance. Time-temperature data gathered from 24 LexanTM transducers were used for calculation of the heating and cooling rate indices as well as lethality. There were significant variations in the temperature distribution and heat transfer parameters at the different tray levels; however, these variations did not contribute to large variations in the accumulated overall process lethality. 相似文献
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The convective heat transfer coefficient (hfp) between fluid and particle in continuous tube flow was estimated using a temperature pill, a remote electronic temperature sensor which uses a quartz crystal as the temperature sensing element. the temperature history of a particle (with temperature pill mounted within) was monitored as it moved through a test section. A finite element algorithm was then used to back calculate hfp from the time-temperature data. the value of hfp ranged from 134 W/m2K to 669 W/m2K (Nu=3.6 to 17.3) over a fluid generalized Reynolds number range (restricted by experimental constraints) from 19 to 196.8. As expected, hfp decreased with increasing carrier medium viscosity and increased with increasing flow rates. Even with several conservative factors at play, the lowest Nusselt number was greater than the 2.0 expected for a spherical particle in a stagnant fluid. Potential applications of the technique include noninvasive measurement of the temperature (and hfp values) of the particles moving within a fluid stream in otherwise inaccessible locations. 相似文献
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The residence time and the residence time distributions of cylindrical particles (density 1130 kg/m3 and particle concentration 20% v/v) in a U-bend of 22 cm radius of curvature were studied. All experiments were conducted at room temperature and with an aqueous solution of sodium carboxymethylcellulose (0.5% CMC) as the carrier medium. Two levels of particle size (11 and 20 mm) and three levels of product flow rates (0.66 × 10?3, 0.81 × 10?3, and 0.97 × 10?3 m3/s) were used. the results obtained from this study showed that the mean and the standard deviation of the normalized residence time of particles decreased as either particle size or flow rate was increased. the E(θ) and F(θ) curves indicated that flow profile of particles approached the plug flow profile as the particle size or the flow rate was increased. Results obtained from regression analyses revealed that the mean and the standard deviation of the normalized residence time were significantly influenced by particle Froude number and most strongly by particle-to-tube diameter ratio. 相似文献