Drug Targeting Ferrofluidics磁性药物靶向治疗磁流体课件.pptVIP

Magnetic Drug Targeting, Ferrofluidics Magnetic Drug Targeting: Ferrofluidics Magnetic Drug Targeting Ferrofluids (magnetic liquids) as drug carriers Drug targeting applications Localized chemotherapy Less damage to healthy cells Multiphysics: Magntostatics Fluid Flow This model was provided by Daniel J. Strauss, The Institute for New Materials, Inc., www.inm-gmbh.de Geometry – 2D Approximation The Math behind the Magnetostatics Maxwells law for the magnetic field and current (static) Gauss’ theorem for the magnetic flux density (B-field) Definition of a magnetic vector potential A Constitutive relation to tie B-H (M is magnetization) Combining the above equations gives, for zero currents The Math behind the Fluid Flow Incompressible Navier Stoke’s equations The Math behind the Fluid Flow Incompressible Navier Stoke’s equations Magnetic Volume Force for a Ferrofluid: M = magnetization H = magnetic field The Math behind the Fluid Flow Magnetic Volume Force for a Ferrofluid x,y, components Boundary Conditions Magnetostatics Reasonably far away from the magnet, magnetic insulation is applied: Az=0 Navier Stokes A pulsating inlet velocity simulates the heart beat. No-slip on walls Pressure on outlet Az=0 Results – magnetic field The magnetic flux density has a maximum near the sharp corners. White areas are excluced from the plot range for clarity. The interesting area is the blood vessel. Results – Velocity Field at max blood throughput (heat beat), t=0.25. The flow field is clearly distorted by the magnet Results – Velocity Field at zero throughput, t=1 Even though the net flow is zero, we can see agitation in eddies generated by the magnetic field. Results – movie Results - Conclusions Certain points near the magnetic disturbances will be exposed to a larger flow rate per unit area, (close to the reddish areas) whereas some parts will get less exposed (blue areas near vessel wall). COMSOL Multiphysics is a good tool to test different flowrates and geomet