1993
DOI: 10.1016/0009-2509(93)80366-x
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Holdup and dispersion: tracer residence times, moments and inventory measurements

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Cited by 32 publications
(11 citation statements)
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“…One way to test robustness is to examine the sensitivity of fitted parameter values to perturbations in system conditions. For laboratory miscible-displacement experiments, this could involve, for example, changing the pore-water velocity or magnitude of the input pulse (e.g., De Lasa et al, 1986; Brusseau et al, 1989; Buffham and Mason, 1993; Young and Ball, 2000; Schnaar and Brusseau, 2013). The potential experiment-condition dependency of the continuous-distribution rate model has received minimal investigation to date.…”
Section: Introductionmentioning
confidence: 99%
“…One way to test robustness is to examine the sensitivity of fitted parameter values to perturbations in system conditions. For laboratory miscible-displacement experiments, this could involve, for example, changing the pore-water velocity or magnitude of the input pulse (e.g., De Lasa et al, 1986; Brusseau et al, 1989; Buffham and Mason, 1993; Young and Ball, 2000; Schnaar and Brusseau, 2013). The potential experiment-condition dependency of the continuous-distribution rate model has received minimal investigation to date.…”
Section: Introductionmentioning
confidence: 99%
“…When the Bo number tends to infinity, the mixing conditions are similar to those of a plug-flow reactor, and the reactor can be considered as well mixed for low Bo numbers. The alternative approach of Buffham and Mason (165) states that the mixing characteristics of a piece of equipment should be expressed as the variance σ 2 of the distribution obtained by injection of a pulse of tracer without adopting any mechanistic model (165). The relationship between Bo and σ 2 depends on the reactor configuration (166).…”
Section: Liquid Mixingmentioning
confidence: 99%
“…For pulse inputs (Valocchi, 1985) μ1i=0tFtCgidt0tFCgidttp2where μ ′ 1 is the mean travel time of the conservative ( i = c ) or partitioning ( i = p ) tracer, t F is the time the tracer measurements were terminated, and t p is the duration of the input pulse. For pulse inputs, the concentration of the tracer at t = t F was designated as the tracer detection limit, c d g For step inputs (Buffham and Mason, 1993), μ1i=0tFtrue(1Cgitrue)dtThe retardation factor and the water saturation were then calculated by R=μ1pμ1c Sw=11+1KHtrue(R1true)Spreading of the conservative tracer was influenced only by the Peclet number, since R = 1 and the second and third moments are only affected by Pe (Eq. [13] and [14]) Because of this and our focus on the influence of mass transfer limitations on measurement error, in the computational experiments discussed below we assumed the mean travel time of the conservative tracer was determined exactly, while the mean travel time of the partitioning tracer was computed using Eq.…”
Section: Mathematical Modelingmentioning
confidence: 99%