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Thermal current

Where a cupboard is fitted with a bypass, it should be designed with an air velocity that is sufficiently high to prevent the escape of contaminants. This is particularly important where the cupboard is likely to be subjected to high heat loads, which could cause strong thermal currents in the upper part of the cupboard. However, the velocity should not be high enough to disturb the flow inside the cupboard and cause loss of containment. [Pg.891]

Thermal currents Natural convection currents set up in a fluid due to density differences. [Pg.1482]

Convection requires a fluid, either liquid or gaseous, which is free to move between the hot and cold bodies. This mode of heat transfer is very complex and depends firstly on whether the flow of fluid is natural , i.e. caused by thermal currents set up in the fluid as it expands, or forced by fans or pumps. Other parameters are the density, specific heat capacity and viscosity of the fluid and the shape of the interacting surface. [Pg.7]

Increased sensitivity arising from a longer residence time within the beam of radiation from the lamp. Residence times in flames are low because of strong vertical thermal currents (p. 315). [Pg.328]

Fig. 19. The scheme of bands explaining the voltage-current curve of a tunnel diode, a. The p-region b, the n-region c, the forbidden energy gap. Arrows show the directions of electron transfer. 0, The case of the zero shift of the Fermi levels 1, 2, tunneling through the forbidden energy gap 3, the position of bands corresponding to the minimum of the voltage current curve for a diode 4, thermal currents. Fig. 19. The scheme of bands explaining the voltage-current curve of a tunnel diode, a. The p-region b, the n-region c, the forbidden energy gap. Arrows show the directions of electron transfer. 0, The case of the zero shift of the Fermi levels 1, 2, tunneling through the forbidden energy gap 3, the position of bands corresponding to the minimum of the voltage current curve for a diode 4, thermal currents.
Here N(sQ is the electron density of states on the Fermi surface for one direction of spin, is the effective volume of phonon generation, is the point contact form factor, averaged over the Fermi surface. It should be noted that point contacts of sizes d > l, d l can work also in diffusive or thermal current regimes [5] and are used for the study of EPI, phase transitions, superconductivity and other interesting physical phenomena. [Pg.291]

The conduit could be a heat conductor carrying a thermal current, Ig. Whatever the commodity might be, energy is transported concurrently with it- The rate IE, at which energy flows is proportional to the commodity current. Thus, with charge current, Ig, the electric flow rate of energy past a cross-section of the conduit is... [Pg.5]

The driving force which causes a thermal current is a temperature difference, and the flow rate of energy with thermal current is given by... [Pg.6]

In undoped conducting polymers [cr(300 K) < 10-6 S/cm], S (300 K) 1 mVK-1. This value decreases upon doping, and in fully doped systems S (300 K) 10 pV K-1. Although conducting polymers are intrinsically quasi-ID and highly disordered, a remarkable linear S(T) has been observed in high quality metallic samples down to 10 K [16,21]. This indicates that the thermal current carried by phonons is less impeded by insulating barriers... [Pg.113]

The electroactive species can also reach the electrode surface by convection, giving rise to a convection current that is, again, non-concentration-dependent. Convection effects are attributable to stirring of the solution or, less frequently, to thermal currents. Thus, polarography and voltammetry are carried out in quiet (unstirred) solutions. [Pg.1492]

Thermal Transport of Energy and Available-Energy. The energy and available-energy currents associated with a thermal current are IE = Tig and Pft = [t - T0]lg. Therefore, the available-energy current may be written in terms of the energy current as PA =... [Pg.10]

The thermal current Ig leaving the composite in Figure 2 is the rate at which "heat" is being produced inside the composite. [Pg.13]


See other pages where Thermal current is mentioned: [Pg.314]    [Pg.315]    [Pg.1001]    [Pg.453]    [Pg.173]    [Pg.288]    [Pg.61]    [Pg.137]    [Pg.358]    [Pg.471]    [Pg.471]    [Pg.174]    [Pg.156]    [Pg.42]    [Pg.90]    [Pg.288]    [Pg.214]    [Pg.167]    [Pg.258]    [Pg.10]    [Pg.252]    [Pg.286]    [Pg.310]    [Pg.147]    [Pg.4]    [Pg.315]    [Pg.12]    [Pg.20]    [Pg.445]    [Pg.149]    [Pg.144]    [Pg.277]    [Pg.981]   
See also in sourсe #XX -- [ Pg.1479 ]




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