“…[
28 ] Under a magnetic field, the magnetic particles arrange into columns aligned with the field due to dipole–dipole interactions, and these arrangements are transported as a whole and act as larger, non‐spherical objects. This phenomenon, referred to as “cooperative magnetophoresis,” [
29–31 ] leads to increased magnetophoretic velocity and facilitates further aggregation of magnetic particles. The magnetic force acting on a column of beads is assumed to be equal to the sum of the force applied to each individual particle, as this body force acts in the bulk of the material, and can be expressed as:
where N is the number of particles in the column that can be estimated experimentally, ρ p (kg m –3 ) and V p (m 3 ) are the particle density and volume, respectively, M p (emu g –1 or A m 2 kg –1 ) is the particle magnetization per mass unit, and ∇ B (T m –1 ) is the magnetic field gradient.…”