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Thermal Conductivity K Factor

Thermal Conductivity (K Factor) Depending on the type of insulation, the thermal conductivity K factor) can vary with age, manufacturer, moisture content, and temperature. Typical published values are shown in Fig. 11-65. Mean temperature is equal to the arithmetic average of me temperatures on both sides of the insulating material. [Pg.1098]

Values of thermal conductivity (K factor) depend on density, closed cell content, composition of the gas. Cell size and orientation also affect the K factor, which decreases with the decrease of temperatnre independent on the nature of foaming agent [39]. [Pg.247]

Notes. Thermal conductivity (k-factor) dimensions, Btu/h-ft °F/in. Erosion loss per ASTM C704. [Pg.396]

Liquid 4He, above 2.2 K (He I), because of its low density, shows transport properties similar to those of a classic gas (Fig. 2.12). The same happens for 3He above 0.1 K. Above the A-point, 4He has a low thermal conductivity (a factor of 10-4 compared to Cu and a factor of 10-1 compared to stainless steel) and boils with strong bubbling. [Pg.66]

Since the results of zone refining depend on the interaction of momentum, heat and mass transfer in the system, all the basic factors affecting these three processes, both molecular and convective, have to be taken into consideration. These basic factors are concentration W, Density f, viscosity /i, heat capacity Cp, temperature den-sification coefficient, thermal conductivity k, molecular dif-fusivity D, zone diameter d, zone length L, zone travel speed u, temperature difference in zone A T and acceleration g. The concentration W may affect, JJi, Cp,, k, and D as well as the properties of the P.S.Z. (mushy region). Aside from the concentration W, all... [Pg.231]

Table 1.1. Abundance of the metal in the earths s crust, optical band gap Es (d direct i indirect) [23,24], crystal structure and lattice parameters a and c [23,24], density, thermal conductivity k, thermal expansion coefficient at room temperature a [25-27], piezoelectric stress ea, e3i, eis and strain d33, dn, dig coefficients [28], electromechanical coupling factors IC33, ksi, fcis [29], static e(0) and optical e(oo) dielectric constants [23,30,31] (see also Sect. 3.3, Table 3.3), melting temperature of the compound Tm and of the metal Tm(metal), temperature Tvp at which the metal has a vapor pressure of 10 3 Pa, heat of formation AH per formula unit [32] of zinc oxide in comparison to other TCOs and to silicon... Table 1.1. Abundance of the metal in the earths s crust, optical band gap Es (d direct i indirect) [23,24], crystal structure and lattice parameters a and c [23,24], density, thermal conductivity k, thermal expansion coefficient at room temperature a [25-27], piezoelectric stress ea, e3i, eis and strain d33, dn, dig coefficients [28], electromechanical coupling factors IC33, ksi, fcis [29], static e(0) and optical e(oo) dielectric constants [23,30,31] (see also Sect. 3.3, Table 3.3), melting temperature of the compound Tm and of the metal Tm(metal), temperature Tvp at which the metal has a vapor pressure of 10 3 Pa, heat of formation AH per formula unit [32] of zinc oxide in comparison to other TCOs and to silicon...
The heat transfer-coefficients and fouling factors are listed in Table 7.2.1. Because of the acetic acid, select SS316 as the material of constraction. The thermal conductivity, k, of SS316 and the wall thickness of the reactor, Xw, are given in Table 7.2.1. [Pg.400]

Conduction shape factors Sfor several configurations for use in Q = frS(T, - T2) to determine the steady rate of heat transfer through a medium of thermal conductivity k between the surfaces at temperatures Ti and... [Pg.194]

Die thermal conductivity k for use in the Nu relations above should be evaluated at the bulk mean fluid temperature, which is the arithmetic average of the mean fluid temperatures at the inlet and the exit of the tube. For laminar flow, the effect of suiface roughness on the friction factor and the heat transfer coefficient is negligible. [Pg.487]

Figure 7 presents the numerical results, obtained for k dependent thermal conductivity k) by combining the MD simulations and GCM approach for KrAr and LiF. The difference between these two cases is seen on the qualitative level. For a mixture of neutral particles (right) the expected behavior, described by the Lorentzian-like function, is observed. Otherwise, we found the increase in A(k) when k becomes larger for molten LiF, and a well pronounced peak is seen at wavenumber kp where the first peak of static structure factor Sxx(k) is located (see Fig. 1). [Pg.137]

Few measurements rely on a single factor velocity, for example, is a product of time and distance—two factors. The volumetric flow rate through an orifice depends on the pressure drop, fluid density, and geometry, which adds up to three factors or more. Thermal conductivity, k, is the ratio of heat flux to temperature gradient— this measurement could have as many as six factors. All factors have an associated uncertainty that contributes to the overall uncertainty of the measurand. [Pg.36]

Material K Factor or Thermal Conductivity R Factor, 1-in. Thicknesses Thickness in Inches Required for Equivalent Insulating Value... [Pg.249]

Tables 4.4-3-4.4-21 are arranged according to piezoelectric classes in order of decreasing symmetry (see Table 4.4-2), and alphabetically within each class. They contain a number of columns placed on two pages, even and odd. The following properties are presented for each dielectric material density q, Mohs hardness, thermal conductivity k, static dielectric constant Sij, dissipation factor tanS at various temperatures and frequencies, elastic stiffness Cmn, elastic compliance s n (for isotropic and cubic materials only), piezoelectric strain tensor di , elastooptic tensor electrooptic coefficients r k (the lat-... Tables 4.4-3-4.4-21 are arranged according to piezoelectric classes in order of decreasing symmetry (see Table 4.4-2), and alphabetically within each class. They contain a number of columns placed on two pages, even and odd. The following properties are presented for each dielectric material density q, Mohs hardness, thermal conductivity k, static dielectric constant Sij, dissipation factor tanS at various temperatures and frequencies, elastic stiffness Cmn, elastic compliance s n (for isotropic and cubic materials only), piezoelectric strain tensor di , elastooptic tensor electrooptic coefficients r k (the lat-...

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