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Magnetic drug targeting  205


                   intense, MD transfer through the endothelial membrane and tissue are described
                   by, respectively,
                                          @
                                            c M 1 v mg Ur c M 5 rU D M rc M Þ;
                                         @t                    ð                         ð6:30Þ

                                          @
                                            c T 1 v mg Ur c T 5 rU D T rc T Þ;
                                          @t                   ð                         ð6:31Þ

                   where c M and c T denote the species (MNPs) in the membrane and tissue, respectively,
                   D M and D T are the diffusivities of MNPs through the membrane and tissue, respec-
                   tively. The recommended magnetic velocity, v mg ,is (Grief and Richardson, 2005;
                   Nacev et al., 2011)

                                                             a μ χ
                                                              2
                                                    2
                                            v r 5 krH ; k 5      0    ;
                                                            9η 1 1  χ                    ð6:32Þ
                                                                   3
                   where k is the magnetic drift coefficient, which depends on: a—MNP radius,
                   χ—MNPs susceptibility, and η the dynamic viscosity of blood.
                      In fact, the suggested approach to calculate the magnetic velocity, v r , that is used as
                   a macroscopic quantity, is a homogenization technique that raises the physical model
                   scale from the MNP nanometric level to a macroscopic, continuous, magnetizable
                   medium, superparamagnetic like, which is characterized by an apparent susceptibility,
                   χ app , that depends on the (constant) viscosity of a Newtonian fluid—the coefficient k
                   in Eq. (6.32), which is proportional with the susceptivity of the MNP and the
                   dynamic viscosity of the solute fluid. In view of Eq. (6.32), for constant χ (same mate-
                   rial for the MNP), η - 0 yields k - N, consequently less viscous the fluid is the
                   higher the magnetic velocity is.
                      The bidimensional model in Fig. 6.28 refers to the membrane of a blood vessel
                   and the surrounding tissue: a longitudinal section through a cylindrical blood vessel
                   (R1) with a diameter d 5 5 mm. The vessel is bounded by an endothelial layer
                   (R2) of thickness g 5 0.5 mm, and embedded into the target tissue (R5), 50 mm
                   thick. The PM (R4, NdFeB, B rem 5 1T, of size 10mm 3 30 mm) is outside the
                   target tissue, and its magnetization is set to favor the transendothelial transfer of
                   MNPs. MNPs may cross through the wall with a diffusion coefficient D M .The
                   magnetic field problem is closed by free space (R3). The membrane face inside the
                                         3
                   vessel has C b 5 4mol/m , and all other parts of the species transfer boundary are
                                                                     2
                                                                                           2
                   impermeable. The properties are D M 5 1.5 3 10 212  m /s, D T 5 1.2 3 10 214  m /s,
                              23   2           217  4   2
                   a 5 2.5 3 10  m , k 5 5 3 10   m /(A s), and χ 5 0.003 (Swabb et al., 1974;
                   Nacev et al., 2011; Soltani and Chen, 2013; Winner et al., 2016; Zhan et al., 2019).
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