The effective capture radius

is shown to be estimated from the single wire buildup study through the next equation.

, where

is the effective density of as-captured particles, dS/dt is the rate of increase of the particle retention cross section, C
inand v
oare the concentration and the velocity of the feed slurry, respectively, and a is the wire radius. Using α-Fe
2O
3particles, it is found that

, where S is the buildup cross section,

, and τ is the characteristic time depending on v
oand the applied field H
o. From these two equations, it is found that

, where

. This relation can adequately be explained by the existing theory. Another finding is

or

. The dependence of τ or

on H
ocan be explained by considering the weak ferromagnetic nature of α-Fe
2O
3. However, to explain the dependence of τ or

on v
o, the introduction of the sticking factor, namely the probability that a particle arrived at the wire surface is actually captured, seems to be required.