Permanent Magnet and Electromechanical Devices: Materials, Analysis, and Applications

By E. Furlani. 2001

687 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/81b9b7d97829027f5a551013cad4fc642a9b18ca

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Citations in the corpus

Permanent Magnets for MEMS (2009, background): “supply the most magnetic energy to an air gap, which is particularly important for actuator applications [13].”
Design and modeling of a magnetic shock absorber based on eddy current damping effect (2008, methodology): “Furlani [16] has shown that a cylindrical magnet can be replaced by an equivalent magnetic volume current density Jm 1⁄4X M and an equivalent surface current density jm 1⁄4 M n̂ that circulates around the body of the cylinder.”
Three-Dimensional Magnetic Manipulation of Micro- and Nanostructures for Applications in Life Sciences (2013, background): “where is the volumemagnetization in [A/m] of the object of a certain volume [27].”
Microrobots for minimally invasive medicine. (2010, methodology): “For a circular loop of radius r and current i, the dipole moment is simply | D| = π ir2, with the direction of D pointed along the axis of the loop and defined by the direction of current flow using the right-hand rule (80).”
Magnetic Actuation Systems for Miniature Robots: A Review (2020, background): “Note that the governing equations (Equation (2) and (3)) abstract the magnetic miniature robots into a dipole, which is reasonable due to the sufficient distances relative to their sizes.([40]) Supposing that the magnetic field is fully flexible, only maximal 5-DOF actuation is possible under this d”
Analysis of particle transport in a magnetophoretic microsystem (2006, background): “ ∂∂ ax ax mx ax ay Hxy H xy xy f H xy H xy xy (15) and 0p (, ) (, ) F(,) V (H) (,) (,) ,µ ∂∂ =+ ∂∂ ay ay my a ax ay Hxy H xy xy f H xy H xy xy (16) where H =H(,) H (,)ˆˆ aax ayx yxyx+ y. (17) To evaluate ( , )Fm x y we need an expression for the field distribution ( , )Ha x y . This is a superpo”