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ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

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dimensionless frequency . With the above definitions, the dimensionless advectiondiffusion-reaction<br />

equation at constant temperature and low density of ligands can be<br />

written [12]:<br />

At the cells surface (0 < x < 1, y = 0), we considered a first order two ways reaction for<br />

ligands binding the receptors on the cell membrane [13]:<br />

where B is the surface concentration of bound receptors normalized by total number of<br />

receptors (RT), is the dimensionless association rate, K is the dimensionless binding<br />

affinity.<br />

We considered ligands as autologous and secreted at a constant rate. Therefore,<br />

boundary conditions on the reactive surface were defined as:<br />

where is the dimensionless secretion rate.<br />

(2)<br />

(3)<br />

, for (4)<br />

The boundary conditions at the chamber entrance, downstream end and channel ceiling,<br />

were respectively given by [14]:<br />

, , (5)<br />

This model was implemented in COMSOL 4.2a (COMSOL Inc, Palo Alto, USA).<br />

Physiological constant values were used as input data [9, 15, 16]:<br />

(L = 6.1mm, h = 0.25 mm), (V = 4.9 mm/s), D = 100 µm 2 /s, , =<br />

20 nM (K = 100), = 3 10 4 M -1 s -1 ( 3.75 10 -3 ), CT = 2 10 -7 mol/m 3 , = 15.7 10 -3 .<br />

The stationary no-flow (Pe = 0) solution for infinite epithelia (L = ∞) was taken as<br />

initial condition and set as reference state:<br />

For the oscillatory flow, four values of frequency were considered: 0.1, 0.5, 1 and 2 Hz.<br />

(6)<br />

(7)<br />

(8)

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