<i>Electricity and Magnetism</i>

Winch, Ralph P.; Park, David A.

doi:10.1063/1.3061830

Cited by 4 publications

(3 citation statements)

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“…[46,48,56]). The time constant in such circuits is defined as the time at which the electric current or charge reaches 1 À 1/e (=0.632) of its final value.…”

Section: Time To Equilibrium and Time Constantmentioning

confidence: 99%

A similarity approach to determine response times to steady-state saturation in landscapes

Aryal

O’Loughlin²,

Mein³

2005

Advances in Water Resources

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“…[46,48,56]). The time constant in such circuits is defined as the time at which the electric current or charge reaches 1 À 1/e (=0.632) of its final value.…”

Section: Time To Equilibrium and Time Constantmentioning

confidence: 99%

A similarity approach to determine response times to steady-state saturation in landscapes

Aryal

O’Loughlin²,

Mein³

2005

Advances in Water Resources

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“…3 variants of simplified electrical and magnetical boundary conditions are investigated for a crack in a homogeneous magnetoelectroelastic material. Taking into account that according to the physical datum [26] the magnetic permeability of some materials can be lower than the vacuum one even we consider further the case of electrically permeable and magnetically impermeable boundary conditions. Moreover, it will be assumed further that the crack faces are free from concentrated loading, i.e., P = 0.…”

Section: Electrically Permeable and Magnetically Impermeable Interfacmentioning

confidence: 99%

An interface crack with contact zones in a piezoelectric/piezomagnetic bimaterial

2009

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An interface crack with a frictionless contact zone at the right crack tip between two semi-infinite piezoelectric/piezomagnetic spaces under the action of a remote mechanical loading, magnetic and electric fluxes as well as concentrated forces at the crack faces is considered. Assuming that all fields are independent on the coordinate x 2 co-directed with the crack front, the stresses, the electrical and the magnetic fluxes as well as the derivatives of the jumps of the displacements, the electrical and magnetic potentials are presented via a set of analytic functions in the (x 1 , x 3 )-plane with a cut along the crack region. Two cases of magneto-electric conditions at the crack faces are considered. The first case assumes that the crack is electrically and magnetically permeable, and in the second case the crack is assumed electrically permeable while the open part of the crack is magnetically impermeable. For both these cases due to the above-mentioned representation the combined Dirichlet-Riemann boundary value problems have been formulated and solved exactly. Stress, electric and magnetic induction intensity factors are found in a simple analytical form. Transcendental equations and a closed form analytical formula for the determination of the real contact zone length have been derived for both cases of magnetic conditions in the crack region. For a numerical illustration of the obtained results a bimaterial BaTiO 3 -CoFe 2 O 4 with different volume fractions of BaTiO 3 has been used, and the influence of the mechanical loading and the intensity of the magnetic flux upon the contact zone length and the associated intensity factors as well as the energy release rate has been shown.

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“…[29][30][31][32][33] Table 2 shows the behavior of an electromagnetic field near a metal. [34][35][36] In a radiated electromagnetic field near a metal, we can observe a high-frequency discharge, a spark discharge, a field reflection, and a secondary field radiation field such as an antenna. In an induction field, we can observe electromagnetic induction and an eddy current.…”

Section: Near-field Intrabody Communicationmentioning

confidence: 99%

Electrooptic sensor module fabrication for near-field intrabody communication

Furuya¹,

Sasaki²,

Morimura³

et al. 2014

OPT REV

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In this paper, we describe how to obtain a low cost electrooptic (EO) sensor module for the mass production of nearfield intrabody communication devices. In our previous study, we used a bulk cleavage technique to fabricate EO modulators without the need for any optical polishing or washing processes. In this study, we fabricated EO modulators as a miniaturized chip sensor without a base portion, and clarified the feasibility of assembling optical components by only a passive alignment technique with a compact housing. #

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Electricity and Magnetism

Cited by 4 publications

References 0 publications

A similarity approach to determine response times to steady-state saturation in landscapes

A similarity approach to determine response times to steady-state saturation in landscapes

An interface crack with contact zones in a piezoelectric/piezomagnetic bimaterial

Electrooptic sensor module fabrication for near-field intrabody communication

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