ASHRAE REFRIGERATION SI CH 19-2010 THERMAL PROPERTIES OF FOODS《食物的热特性》.pdf
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1、19.1CHAPTER 19THERMAL PROPERTIES OF FOODSThermal Properties of Food Constituents 19.1Thermal Properties of Foods 19.1Water Content 19.2Initial Freezing Point 19.2Ice Fraction 19.2Density . 19.6Specific Heat 19.6Enthalpy . 19.7Thermal Conductivity. 19.9Thermal Diffusivity. 19.17Heat of Respiration 19
2、.17Transpiration of Fresh Fruits and Vegetables 19.19Surface Heat Transfer Coefficient 19.24Symbols 19.27HERMAL properties of foods and beverages must be knownTto perform the various heat transfer calculations involved in de-signing storage and refrigeration equipment and estimating processtimes for
3、 refrigerating, freezing, heating, or drying of foods and bev-erages. Because the thermal properties of foods and beveragesstrongly depend on chemical composition and temperature, and be-cause many types of food are available, it is nearly impossible to ex-perimentally determine and tabulate the the
4、rmal properties of foodsand beverages for all possible conditions and compositions. How-ever, composition data for foods and beverages are readily availablefrom sources such as Holland et al. (1991) and USDA (1975). Thesedata consist of the mass fractions of the major components found infoods. Therm
5、al properties of foods can be predicted by using thesecomposition data in conjunction with temperature-dependent math-ematical models of thermal properties of the individual food constit-uents.Thermophysical properties often required for heat transfer calcu-lations include density, specific heat, en
6、thalpy, thermal conductivity,and thermal diffusivity. In addition, if the food is a living organism,such as a fresh fruit or vegetable, it generates heat through respirationand loses moisture through transpiration. Both of these processesshould be included in heat transfer calculations. This chapter
7、 summa-rizes prediction methods for estimating these thermophysical proper-ties and includes examples on the use of these prediction methods.Tables of measured thermophysical property data for various foodsand beverages are also provided.THERMAL PROPERTIES OF FOOD CONSTITUENTSConstituents commonly f
8、ound in foods include water, protein,fat, carbohydrate, fiber, and ash. Choi and Okos (1986) developedmathematical models for predicting the thermal properties of thesecomponents as functions of temperature in the range of 40 to150C (Table 1); they also developed models for predicting thethermal pro
9、perties of water and ice (Table 2). Table 3 lists the com-position of various foods, including the mass percentage of mois-ture, protein, fat, carbohydrate, fiber, and ash (USDA 1996).THERMAL PROPERTIES OF FOODSIn general, thermophysical properties of a food or beverage arewell behaved when its temp
10、erature is above its initial freezing point.However, below the initial freezing point, the thermophysical prop-erties vary greatly because of the complex processes involved dur-ing freezing.The preparation of this chapter is assigned to TC 10.9, Refrigeration Appli-cation for Foods and Beverages.Tab
11、le 1 Thermal Property Models for Food Components (40 t 150C)Thermal Property Food Component Thermal Property ModelThermal conductivity, W/(m K) Protein k = 1.7881 101+ 1.1958 103t 2.7178 106t2Fat k = 1.8071 101 2.7604 104t 1.7749 107t2Carbohydrate k = 2.0141 101+ 1.3874 103t 4.3312 106t2Fiber k = 1.
12、8331 101+ 1.2497 103t 3.1683 106t2Ash k = 3.2962 101+ 1.4011 103t 2.9069 106t2Thermal diffusivity, m2/s Protein = 6.8714 108+ 4.7578 1010t 1.4646 1012t2Fat = 9.8777 108 1.2569 1011t 3.8286 1014t2Carbohydrate = 8.0842 108+ 5.3052 1010t 2.3218 1012t2Fiber = 7.3976 108+ 5.1902 1010t 2.2202 1012t2Ash =
13、1.2461 107+ 3.7321 1010t 1.2244 1012t2Density, kg/m3Protein = 1.3299 103 5.1840 101tFat = 9.2559 102 4.1757 101tCarbohydrate = 1.5991 103 3.1046 101tFiber = 1.3115 103 3.6589 101tAsh = 2.4238 103 2.8063 101tSpecific heat, kJ/(kgK) Protein cp= 2.0082 + 1.2089 103t 1.3129 106t2Fat cp= 1.9842 + 1.4733
14、103t 4.8008 106t2Carbohydrate cp= 1.5488 + 1.9625 103t 5.9399 106t2Fiber cp= 1.8459 + 1.8306 103t 4.6509 106t2Ash cp= 1.0926 + 1.8896 103t 3.6817 106t2Source: Choi and Okos (1986)19.2 2010 ASHRAE HandbookRefrigeration (SI)The initial freezing point of a food is somewhat lower than thefreezing point
15、of pure water because of dissolved substances in themoisture in the food. At the initial freezing point, some of the waterin the food crystallizes, and the remaining solution becomes moreconcentrated. Thus, the freezing point of the unfrozen portion of thefood is further reduced. The temperature con
16、tinues to decrease asseparation of ice crystals increases the concentration of solutes insolution and depresses the freezing point further. Thus, the ice andwater fractions in the frozen food depend on temperature. Becausethe thermophysical properties of ice and water are quite different,thermophysi
17、cal properties of frozen foods vary dramatically withtemperature. In addition, the thermophysical properties of the foodabove and below the freezing point are drastically different.WATER CONTENTBecause water is the predominant constituent in most foods,water content significantly influences the ther
18、mophysical propertiesof foods. Average values of moisture content (percent by mass) aregiven in Table 3. For fruits and vegetables, water content varies withthe cultivar as well as with the stage of development or maturitywhen harvested, growing conditions, and amount of moisture lostafter harvest.
19、In general, values given in Table 3 apply to matureproducts shortly after harvest. For fresh meat, the water contentvalues in Table 3 are at the time of slaughter or after the usual agingperiod. For cured or processed products, the water content dependson the particular process or product.INITIAL FR
20、EEZING POINTFoods and beverages do not freeze completely at a single tem-perature, but rather over a range of temperatures. In fact, foods highin sugar content or packed in high syrup concentrations may neverbe completely frozen, even at typical frozen food storage tempera-tures. Thus, there is not
21、a distinct freezing point for foods and bev-erages, but an initial freezing point at which crystallization begins.The initial freezing point of a food or beverage is important notonly for determining the foods proper storage conditions, but alsofor calculating thermophysical properties. During stora
22、ge of freshfruits and vegetables, for example, the commodity temperature mustbe kept above its initial freezing point to avoid freezing damage. Inaddition, because there are drastic changes in the thermophysicalproperties of foods as they freeze, a foods initial freezing point mustbe known to model
23、its thermophysical properties accurately. Exper-imentally determined values of the initial freezing point of foods andbeverages are given in Table 3.ICE FRACTIONTo predict the thermophysical properties of frozen foods, whichdepend strongly on the fraction of ice in the food, the mass fractionof wate
24、r that has crystallized must be determined. Below the initialfreezing point, the mass fraction of water that has crystallized in afood is a function of temperature.In general, foods consist of water, dissolved solids, and undis-solved solids. During freezing, as some of the liquid water crystal-lize
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