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Fourier numbers

Fig. 5.23 show the solution to Fourier s equation in terms of the temperature gradient at the centre line of section considered and the Fourier Number for... [Pg.391]

The above analysis illustrates how to estimate the cooling time using the relationship between the temperature gradient AT and the Fouriers Number... [Pg.394]

From Fig. S.23 it may be seen that the centre line temperature gradient at this Fourier Number is almost 1. [Pg.396]

This equation is the first term of an infinite series which appears in the rigorous solution of the quasi-diffusion. This equation describes the regular process of quasi-diffusion. For the low values of the Fourier number (irregular quasi-diffusion) it is necessary to use Eq. (5.1) or Boyd-Barrer approximation [105, 106] for the first term in Eq. (5.1)... [Pg.39]

Figures 9.14-9.16 enable the temperature 9C at the centre of the solid (centre-plane, centre-line or centre-point) to be obtained as a function of the Fourier number, and hence of time, with the reciprocal of the Biot number (Bil) as parameter. Figures 9.14-9.16 enable the temperature 9C at the centre of the solid (centre-plane, centre-line or centre-point) to be obtained as a function of the Fourier number, and hence of time, with the reciprocal of the Biot number (Bil) as parameter.
Figures 9.17-9.19 clearly show that, as the Biot number approaches zero, the temperature becomes uniform within the solid, and the lumped capacity method may be used for calculating the unsteady-state heating of the particles, as discussed in section (2). The charts are applicable for Fourier numbers greater than about 0.2. Figures 9.17-9.19 clearly show that, as the Biot number approaches zero, the temperature becomes uniform within the solid, and the lumped capacity method may be used for calculating the unsteady-state heating of the particles, as discussed in section (2). The charts are applicable for Fourier numbers greater than about 0.2.
Kato et al. have used electric stepwise heating of a thin metal layer to measure thermal diffusivity of molten salts. The ratio of the temperatures with time and 2/i at distance x below tlie heating plate was evaluated as a function of the Fourier number ... [Pg.185]

In addihon to the CFD results, estimates of the mixing length based on the Fourier number ... [Pg.201]

For heat transfer the Fourier number is cct/a. The heat transfer analogs of the mass transfer dimensionless groups can be found by making the substitutions described in Chapter 1. [Pg.52]

Fo being the Fourier number and d the diameter of the disk. The mass transfer coefficient k can be considered as interpolating between the steady-state convective diffusion at large times (t - oo) and unsteady-state diffusion at short times (t — 0 and v = 0). The constants A and B of Eq. (147) follow from the solutions for these two limiting cases. For these two limiting cases... [Pg.43]

In the theory of heat transfer, 112 is known as the Fourier number. Therefore, the baking procedure can be presented in a two-dimensional frame ... [Pg.6]

The dimensionless temperature profile is described as a function of the Biot number and Fourier numbers [3, 5]. [Pg.343]

A conservative estimate of the disc s mass transfer performance may be obtained from the Nusselt model, assuming that there is no film mixing as it proceeds to the edge of the disc. For unsteady diffusion into a finite stagnant slab, the plot shown in Figure 8 from (8) gives the relative concentration distribution within the slab at various times, with a zero initial concentration and a surface concentration C0 imposed at time t = 0. The parameter on the curves is the Fourier number, Fo, where... [Pg.98]


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