Magnetic actuators can be divided into two types: those in which motio
n changes the gap separation (type I) and those in which motion change
s the gap overlap area but not the gap separation (type II). In conven
tional magnetic actuators of both types, it is assumed that most of th
e magnetic energy is stored in the gap due to the large reluctance of
the gap compared with the negligibly small reluctance of the magnetic
core. However, in magnetic microactuators, the fabrication limitations
on the achievable cross-sectional area of the magnetic core as well a
s the finite core permeability increase the core reluctance to the poi
nt that this assumption may no longer be valid. in this case, the magn
etic energy is distributed in both the gap and the magnetic core, in w
hich the energy distribution is in proportion to the reluctance of the
gap (R(gap)) and the reluctance of the core (R(core)) respectively. U
sing an elementary structure of a magnetic actuator, it is shown that
for type 1 microactuators, when the initial gap of the actuator is fix
ed (e.g., determining the stroke of the actuator), the generated magne
tic force has maximum Value when the gap overlap area is designed such
that the reluctance of the gap is equal to the reluctance of the magn
etic core (i.e., R(gap) = R(core)). For type II actuators, the initial
overlap area of the actuator is fixed (determining the stroke); there
fore the generated magnetic force has a maximum value when the gap sep
aration is designed such that the above equality holds. This paper det
ails both analytical and finite element method (FEM) analysis confirma
tion for type I actuators. Extension to type II actuators is straightf
orward.