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B THERMOPHYSICAL PROPERTIES

Vargaftik, N. B., Thermophysical Properties of Liquids and Gases, 2nd ed., John Wiley, New York, 1975. [Pg.1048]

N. B. Vargafdk, Tables on the Thermophysical Properties of Eiquids and Gases,]ohxi Wiley Sons, Inc., New York, 1975. [Pg.45]

R. D. McCarty and R. B. Stuart, in S. Gratch, ed.,Mdvances In Thermophysical Properties atTxtreme Temperatures and Pressures, American Society of Mechanical Engineers, New York, 1965, pp. 84—97. [Pg.18]

Maranzana G, Perry I, Maillet D (2004) Mini and Micro-channels Influence of axial conduction in the wads. Int J Heat Mass Transfer 47 3993 004 Platzer B, Plot A, Maurer G (1990) Thermophysical properties of refrigerants. Springer, Berlin Heidelberg New York... [Pg.343]

Figure 4. Continued. Neutral stability diagrams from linear analysis for values of the thermophysical properties considered in this paper, (b) Diagram for properties given as Case III in Table I. Figure 4. Continued. Neutral stability diagrams from linear analysis for values of the thermophysical properties considered in this paper, (b) Diagram for properties given as Case III in Table I.
Kho, Y.W., Conrad, D.C. and Knutson, B.L. (2003) Phase equilibria and thermophysical properties of carbon dioxide-expanded fluorinated solvents. Fluid Phase Equilibria, 206 (1-2), 179-193. [Pg.56]

DIPPR, Project 801, Data Compilation (July 1990) and earlier references cited therein R D. Goodwin, NBSIR 79-1621, Thermophysical Properties Division, National Engineering Laboratory, National Bureau of Standards, Boulder, Colo. 1979 G. B. Kistiakowsky, J. R. Ruhoff, H. A. Smith,... [Pg.374]

Example 2.7 Nonisothermal Parallel Plate Drag Flow with Constant Thermophysical Properties Consider an incompressible Newtonian fluid between two infinite parallel plates at temperatures T(0) = T and T(H) — T2, in relative motion at a steady state, as shown in Fig. E2.7 The upper plate moves at velocity Vo (a) Derive the temperature profile between the plates, and (b) determine the heat fluxes at the plates. [Pg.57]

As pointed out in the previous section, melting can often be modeled in terms of simple geometries. Here we analyze the transient conduction problem in a semi-infinite solid. We compare the solutions of this problem, assuming first (a) constant thermophysical properties, then (b) variable thermophysical properties and finally, and (c) a phase transition with constant thermophysical properties in each phase. These solutions, though useful by themselves, also help demonstrate the profound effect of the material properties on the mathematical complexities of the solution. [Pg.186]

Janssens, M., In thermal model for piloted ignition of wood including variable thermophysical properties, Third International Symposium on Fire Safety Science, Edinburgh, Scotland, Cox, G., Langford, B. (Eds.), Elsevier Applied Science New York, 1991, pp. 167-176. [Pg.383]


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Thermophysical properties

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