scholarly journals Transient solute transport with sorption in Poiseuille flow

2017 ◽  
Vol 828 ◽  
pp. 733-752 ◽  
Author(s):  
Li Zhang ◽  
Marc A. Hesse ◽  
Moran Wang

Previous work on solute transport with sorption in Poiseuille flow has reached contradictory conclusions. Some have concluded that sorption increases mean solute transport velocity and decreases dispersion relative to a tracer, while others have concluded the opposite. Here we resolve this contradiction by deriving a series solution for the transient evolution that recovers previous results in the appropriate limits. This solution shows a transition in solute transport behaviour from early to late time that is captured by the first- and zeroth-order terms. Mean solute transport velocity is increased at early times and reduced at late times, while solute dispersion is initially reduced, but shows a complex dependence on the partition coefficient $k$ at late times. In the equilibrium sorption model, the time scale of the early regime and the duration of the transition to the late regime both increase with $\ln k$ for large $k$. The early regime is pronounced in strongly sorbing systems ($k\gg 1$). The kinetic sorption model shows a similar transition from the early to the late transport regime and recovers the equilibrium results when adsorption and desorption rates are large. As the reaction rates slow down, the duration of the early regime increases, but the changes in transport velocity and dispersion relative to a tracer diminish. In general, if the partition coefficient $k$ is large, the early regime is well developed and the behaviour is well characterized by the analysis of the limiting case without desorption.

2015 ◽  
Vol 25 (7) ◽  
pp. 075403 ◽  
Author(s):  
A. G. Hunt ◽  
B. Ghanbarian ◽  
T. E. Skinner ◽  
R. P. Ewing

Author(s):  
Adam B. Nover ◽  
Krista M. Durney ◽  
Shashank R. Sirsi ◽  
Gerard A. Ateshian ◽  
Mark A. Borden ◽  
...  

Previously, microbubbles have been studied for a number of different medical applications including ultrasound imaging contrast and drug delivery [1]. Microbubbles are comprised of a gas enclosed in a lipid shell. Recent research has shown that the inclusion of microbubbles in tissue engineered cartilage constructs has been shown to enhance mechanical and biochemical growth [2,3]. This modification of the tissue engineering scaffold by incorporation of gas-filled microbubbles has been shown to homogenize depth-dependent mechanical properties (Fig. 1) [3], which, in standard constructs, resembles a “U-shaped” strain profile with the stiffest regions on the edges surrounding a soft center [4]. In addition, these microbubble containing constructs are described by a higher partition coefficient than standard constructs, indicating increased solute transport [3]. These results led us to propose the hypothesis that the incorporation of microbubbles: a) increases nutrient transport upon microbubble dissolution, b) creates fluid-filled pores upon gas efflux and subsequent influx of culture media [3]. In this study, the aforementioned hypothesis is interrogated through analysis of local solute diffusivity.


2000 ◽  
Vol 72 (20) ◽  
pp. 4767-4777 ◽  
Author(s):  
Stewart K. Griffiths ◽  
Robert H. Nilson

1973 ◽  
Vol 61 (1) ◽  
pp. 97-107 ◽  
Author(s):  
A. E. Gill

The properties of infinitesimal disturbances to Poiseuille flow in a circular pipe have been found for a wide range of wavenumbers through recent numerical work (Salwen & Grosch 1972; Garg & Rouleau 1972). These studies did not, however, find the least-damped disturbances. In this paper, the properties of disturbances are found in a limiting case. These disturbances are thought to have decay rates which are equal to or very close to the smallest value possible for any given large value of the Reynolds number R. For disturbances which decay in time, the limiting disturbances can be found analytically. They have the property that the axial wavenumber α tends to zero as R → ∞. The smallest decay rate -βi is given by \[ -\beta_iR = j^2_{1,1}\approx 14.7, \] where j1,1 is the first zero of the Bessel function J1. Two modes have this decay rate. One is axisymmetric with motion only in the azimuthal direction, and the other has azimuthal wavenumber n = 1. For disturbances which decay in space, the limiting solutions can be found by numerically evaluating power series. They have the property that the frequency β tends to zero as R tends to infinity. The smallest decay rate αi for these disturbances is given by αiR ≈ 21·4, corresponding to an axisymmetric mode with motion only in the azimuthal direction. A mode with azimuthal wavenumber n = 1 has a slightly larger decay rate given by αiR ≈ 28·7.


2020 ◽  
Vol 54 (8) ◽  
pp. 4912-4921
Author(s):  
Hamed Mohammadnejad ◽  
Shuchi Liao ◽  
Bonnie A. Marion ◽  
Kurt D. Pennell ◽  
Linda M. Abriola

2001 ◽  
Vol 43 (7) ◽  
pp. 247-255 ◽  
Author(s):  
S. Passone ◽  
D. B. Das ◽  
V. Nassehi

The tidal hydrodynamics and effluent distribution in estuaries involve a complicated range of solute transport phenomena modelled by partial differential equations. Therefore, the quantitative estimation of the risks of water and soil contamination of coastal areas as a result of polluted estuary flows, or effects of the effluent input on the chemical loads, involves the solution of these equations. Generally, the pollutants load in an estuary is determined by the nature of land use which by altering the watershed hydrology or chemical detention/release in the river banks affect the water quality of the estuaries. The present modelling work aims to investigate the solute transport behaviour in the Tay Estuary in Scotland. Based on this study, an attempt to devise an estuary specific discharge strategy for the Tay has been made. The numerical calculations are based on using 2D Galerkin finite element discretisation of the governing equations in an Eulerian co-ordinate system. The flexibility of the formulation allows it to be extended to moving boundary situations encountered in most tidal water systems.


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