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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

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

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In order to have a better understanding of platelet activation, we employed convectiondiffusion-reaction<br />

(CDR) equations for the distribution of coagulant factors. These<br />

coagulant factors, in the vicinity of platelets and over a critical amount, can result in<br />

activation of platelets. Here, in this model, we are concerned in thrombin concentration<br />

([T] in unit/ml) and neglected other factors; as previously shown in [12], thrombin is the<br />

most predominant factor in platelet activation. The CDR equation in 2D for thrombin<br />

can be written as (10). In (10), the last term includes the reaction which results in<br />

inactivation of thrombin. The reaction coefficient, Γ, is derived from the relation that<br />

Sorenson et al. proposed in [2], where we assumed uniform concentration of heparin<br />

and anti-thrombin (ATIII). Here, D, the diffusion coefficient for thrombin is assumed to<br />

be constant with the value of 4.16×10 -17 cm 2 /s. We used alternating direction implicit<br />

(ADI) scheme to solve the equation on a structured grid over the whole domain, which<br />

overlay the cells and fluid. The fluid velocity is averaged from the DPD solution and<br />

thrombin concentration on the grid points, which overlaid platelets, are set to zero.

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