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Thermal conductivity from

Figure 7. Ion source and reaction chamber for the study of ion-molecule reactions at different temperatures. Notation used is same as in Figure 4 except CB = copper block, EL = electrode attached to pressure reducing capillary, TC = thermocouple, TS = thermal shield, ISP = evacuated space reduces thermal conductivity from CB to flange. From Klassen, J. S. Blades, A. T. Kebarle, P. ). Am. Chem. Soc. 1996, with permission. Figure 7. Ion source and reaction chamber for the study of ion-molecule reactions at different temperatures. Notation used is same as in Figure 4 except CB = copper block, EL = electrode attached to pressure reducing capillary, TC = thermocouple, TS = thermal shield, ISP = evacuated space reduces thermal conductivity from CB to flange. From Klassen, J. S. Blades, A. T. Kebarle, P. ). Am. Chem. Soc. 1996, with permission.
The last equation has been used by numerous investigators to evaluate effective thermal conductivities from experimental data. Figure 12.18 reproduced from Froment (94) indicates the... [Pg.498]

P. J. S. Vie and S. Kjelstrup. Thermal conductivities from temperature profiles in the polymer electrolyte fuel cell. Electrochimica Acta 49 (2004) 1069-1077. [Pg.301]

Early results (67) for YBa2Cu307 showed an increase in k (thermal conductivity) from lower temperatures to about 60 K, a slight decrease to near Tc and a nearly constant value between 100-150 K. The low temperature thermal conductivity in single crystal Bi-Sr-Ca-Cu-O (2212 phase) has been measured by Zhu et al. (68) and at temperatures less than 1 K they obtain a fit k = 0.15 T2 W/mK which they note is similar in temperature dependence to Y-Ba-Cu-O and... [Pg.656]

Salamone and Newman (SI) recently studied heat transfer to suspensions of copper, carbon, silica, and chalk in water over the concentration range of 2.75 to 11.0% solids by weight. These authors calculated effective thermal conductivities from the heat transfer data and reached conclusions which not only contradicted Eqs. (35) and (36), but also indicated a large effect of particle size. However, if one compares the conductivities of their suspensions at a constant volume fraction of solids, the assumed importance of particle size is no longer present. It should also be noted that their calculational procedure was a difficult one in that it placed all undefined errors present in the heat transfer data into the thermal conductivity term. For example, six of the seven-... [Pg.123]

Figure 3.4-5. Reduced thermal conductivity from Brunner [12] with permission of Steinkopff Verlag... Figure 3.4-5. Reduced thermal conductivity from Brunner [12] with permission of Steinkopff Verlag...
Jobst has measured the liquid thermal conductivities from - I00X to ckisc to the boiling point of ethyl, propyl, and butyl ether Mawn has determined the thermal conductivity from OT to 30T for ethyl ether 51 A tabulation of some of the literature data for ethyl, propyl, and butyl ether Is available.2 The thermal conductivity of methyl ether was estimated by the method of Robbins and Kingrea. 0... [Pg.53]

Figure 9.1 Cylindrical geometry for calculation of thermal conductivity from radial heat flow. Figure 9.1 Cylindrical geometry for calculation of thermal conductivity from radial heat flow.
During primary drying, the temperature of the product is dependent on shelf temperature and on chamber pressure. The higher the temperature of the shelf, the higher the temperature of the product will be. An increase in chamber pressure favors the thermal exchanges at the gas-product interface and the thermal conductivity from the shelf to the tray. More heat is transported to the product and this results in a rise of product temperature. [Pg.382]

This inaccuracy stems from their calculation of molecular transport effects, such as viscous dissipation and thermal conduction, from bulk flow quantities, such as mean flow velocity and temperature. This approximation of microscale phenomena with macroscale information fails as the characteristic length of the (gaseous) flow gradients approaches the average distance travelled by molecules between collisions - the mean path. The ratio of these quantities is referred to as Knudsen number. [Pg.3]

The strength of the thermal lens, 0, is related to wavelength (X) and power of the laser (P), the sample absorbance (A) and dn/dT and thermal conductivity k values of the solvent as (In this section, k, not Z as in the previous 2.1 section, is used for thermal conductivity. This was done in order to differentiate the thermal conductivity from the wavelength of the laser, which is X in this section.)... [Pg.101]

VPS FeSi2 does not exhibit such a large change in thermal conductivity. From the beginning, the material is more dense and k quite large. Table 1 lists /c-values of SPS and VPS FeSi2 which were measured after a 2 h heat treatment at 800°C (i.e. the time required to induce the a to /3 transition) and after a certain temper time at 800° C. It can be seen that in both cases the thermal conductivity of hot pressed FeSi2 is approached. [Pg.565]

For a uniform energy generation and constant thermal conductivity, from Eq. (2.92) with Ar = 2jtrL or from twice integration of Eq. (2.89) with A, = 2nrL,... [Pg.71]

For air, the change in thermal conductivity from the bulk to the gas at the wall is probably the major factor to consider. [Pg.174]

Average errors are 5 percent when this equation is used. For pressures greater than 3.4 M Pa, the thermal conductivity from Eq. (2-135) may be corrected by the technique suggested by Lenoir. The correction factor is the ratio of conductivityfactors F/F, where F is at the desired temperature and higher pressure, and F is at the same temperature and lower pressure (usually atmospheric). The conductivity factors are calculated from ... [Pg.416]

We turn first to computation of thermal transport coefficients, which provides a description of heat flow in the linear response regime. We compute the coefficient of thermal conductivity, from which we obtain the thermal diffusivity that appears in Fourier s heat law. Starting with the kinetic theory of gases, the main focus of the computation of the thermal conductivity is the frequency-dependent energy diffusion coefficient, or mode diffusivity. In previous woik, we computed this quantity by propagating wave packets filtered to contain only vibrational modes around a particular mode frequency [26]. This approach has the advantage that one can place the wave packets in a particular region of interest, for instance the core of the protein to avoid surface effects. Another approach, which we apply in this chapter, is via the heat current operator [27], and this method is detailed in Section 11.2. [Pg.249]

There is a close relationship between electrical and thermal conductivity. From the simple jBree-electron model for metals, the ratio of the thermal conductivity and the electrical conductivity (reciprocal of resistivity) for metals is directly proportional to the temperature. This is called the Wiedemann-Franz-Lorenz (WFL) relation and the constant of proportionality yields the theoretical (Sommerfeld) Lorenz number, L = 7 l3- kjef = 2.45 x lO" W ft K [67], which was predicted to be independent of temperature (for temperatures significantly larger than the Debye temperature) and of the material. Assuming a known uid/or constant value of Z, the WFL relation can be used to obtain the thermal conductivity from pulse-heating data. [Pg.315]

In general, film adhesives are best suited as insulation to isolate circuitry or to attach large devices or substrates. Insulative films have volume resistivities from 10 to 10 " ohm-cm, thermal conductivities from 0.8 to 1 W/mK, and lap shear strengths ranging from 1200 to 3000 psi. They are available in thicknesses from 2 to 8 mils. ° ... [Pg.133]

When the thermal conductivity attains the high-pressure asymptotic value, the mean free path of the gas molecules within the void spaces of the dried layer has become substantially less than the dimensions of the void spaces. During the transition in thermal conductivity from the low-pressure asymptote to the high-pressure asymptote, the mean free path of the gas molecules rivals the void space dimensions in magnitude, but once the mean free path is reduced to the point at which the gas phase within the solid matrix obeys simple kinetic theory, the thermal conductivity stops rising. [Pg.275]


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