Parallel Hall effect from 3D single-component metamaterialsWe propose a class of three-dimensional metamaterial architectures composed of a single doped semiconductor (e.g., n-Si) in air or vacuum that lead to unusual effective behavior of the classical Hall…Christian Kern, Muamer Kadic, Martin Wegener·Jul 15, 2015SaveLearn
An acoustic invisible gatewayThe recently-emerged concept of "invisible gateway" with the extraordinary capability to block the waves but allow the passage of other entities has attracted great attentions due to the…Yi-Fan Zhu, Xin-Ye Zou, Bin Liang et al.·Jul 14, 2015SaveLearn
Highly asymmetric interaction forces induced by acoustic waves in coupled plate structuresMutual forces can be induced between coupled structures when illuminated by external acoustic waves. In this Letter, we propose a concept of asymmetric interaction between two coupled plate-like…Xiying Fan, Chunyin Qiu, Shenwei Zhang et al.·Jul 6, 2015SaveLearn
On equivalent resistance of electrical circuitsWhile the standard (introductory physics) way of computing the equvalent resistance of non-trivial electrical ciruits is based on Kirchhoff's rules, there is a mathematically and conceptually…Mikhail Kagan·Jun 26, 2015SaveLearn
Cylindrical lateral depth-sensing indentation testing of thin transversely isotropic elastic films: Incompressible and weakly compressible materialsAn indentation testing method, which utilizes lateral contact of a long cylindrical indenter, is developed for a thin transversely isotropic incompressible elastic film deposited onto a smooth rigid…I. Argatov, G. Mishuris·Jun 23, 2015SaveLearn
Bound states in the continuum in open acoustic resonatorsWe consider bound states in the continuum (BSC) or embedded trapped modes in two- and three-dimensional acoustic axisymmetric duct-cavity structures. We demonstrate numerically that under variation…A. A. Lyapina, D. N. Maksimov, A. S. Pilipchuk et al.·Jun 19, 2015SaveLearn
A class of auxetic three-dimensional latticesWe propose a class of auxetic three-dimensional lattice structures. The elastic microstructure can be designed in order to have omni-directional Poisson's ratio arbitrarily close to the stability…Luigi Cabras, Michele Brun·Jun 16, 2015SaveLearn
Tautochrone in the damped cycloidal pendulumThe tautochrone on a cycloid curve is usually considered without drag force. In this work, we investigate the motion of a damped cycloidal pendulum under presence of a drag force. Using the Lagrange…Paco H. Talero L, César A. Herreño-Fierro, Fernanda Santana·Jun 15, 2015SaveLearn
How to introduce physical quantities physicallyThe centuries-long practice of the teaching turned mechanics into an academic construct detached from its underlying science, the physics of macroscopic bodies. In particular, the regularities that…Serge A. Wagner·Jun 12, 2015SaveLearn
Lower Bounds on Q for Finite Size Antennas of Arbitrary ShapeThe problem of the lower bound on the radiation Q for an arbitrarily shaped finite size antenna of non-zero volume is formulated in terms of equivalent electric and magnetic currents densities…Oleksiy S. Kim·Jun 11, 2015SaveLearn
What's the Use of Bound Charge?Bound charge is a useful construct for calculating the electrostatic field of polarized material, and it represents a perfectly genuine accumulation of charge. But is such a material in every respect…David J. Griffiths, V. Hnizdo·Jun 8, 2015SaveLearn
Another derivation of generalized Langevin equationsThe formal derivation of Langevin equations (and, equivalently Fokker-Planck equations) with projection operator techniques of Mori, Zwanzig, Kawasaki and others apparently not has widely found its…R. Dengler·Jun 8, 2015SaveLearn
Experimental Evaluation of the Claimed Coulomb Rotation (Electrostatic Torque)In the year 2002 publications of A.V.M. Khachatourian and A.O. Wistrom were released, in which the existence of an electrostatic torque has been claimed. This moment of force should act in a three…D. Bojiloff, M. Tajmar·Jun 6, 2015SaveLearn
Interaction between an electric charge and a magnetic dipole of any kind (permanent, para- or dia- magnetic or superconducting)The interaction between point charge and magnetic dipole is usually considered only for the case of a rigid ferromagnetic dipole (constant-current): here the analysis of force, momentum and energy…R. Coïsson, G. Asti·Jun 4, 2015SaveLearn
Structural model for the dynamic buckling of a column under constant rate compressionDynamic buckling behavior of a column (rod, beam) under constant rate compression is considered. The buckling is caused by prescribed motion of column ends toward each other with constant velocity.…Vitaly A. Kuzkin·Jun 1, 2015SaveLearn
The Helmholtz decomposition of decreasing and weakly increasing vector fieldsHelmholtz decomposition theorem for vector fields is presented usually with too strong restrictions on the fields. Based on the work of Blumenthal of 1905 it is shown that the decomposition of vector…D. Petrascheck, R. Folk·May 31, 2015SaveLearn
Broadband non-reciprocal transmission of sound with invariant frequencyThe emergence of "acoustic diode" (AD) capable of rectifying acoustic wave like electrical diodes do to electricity has been believed to be able to offer unconventional manipulation on sound,…Zhong-ming Gu, Jie Hu, Bin Liang et al.·May 29, 2015SaveLearn
Axisymmetric scattering of an acoustical Bessel beam by a rigid fixed spheroidBased on the partial-wave series expansion (PWSE) method in spherical coordinates, a formal analytical solution for the acoustic scattering of a zeroth-order Bessel acoustic beam centered on a rigid…F. G. Mitri·May 25, 2015SaveLearn
Classical Mechanics in Hilbert Space: Path Integral Formulation, and a Quantum CorrectionWhile it is well-known that quantum mechanics can be reformulated in terms of a path integral representation, it will be shown that such a formulation is also possible in the case of classical…James Shee·May 24, 2015SaveLearn
Subtleties of the clock retardationFor a simple electromagnetic model of a clock introduced by Jefimenko (clock \# 1 in 1996 Am. J. Phys. 64 812), a change of the rate of the clock when it is set in uniform motion is…D. V. Redzic·May 23, 2015SaveLearn
Active cloaking of resonant coated inclusions for waves in membranes and Kirchhoff platesThe dynamic response of a coated inclusion is considered in the context of active cloaking. The active cloak is achieved for a coated inclusion in the presence of membrane and flexural waves. In this…J. O'Neill, O. Selsil, R. C. McPhedran et al.·May 22, 2015SaveLearn
A conserved quantity in thin body dynamicsThin, solid bodies with metric symmetries admit a restricted form of reparameterization invariance. Their dynamical equilibria include motions with both rigid and flowing aspects. On such…J. A. Hanna, H. Pendar·May 21, 2015SaveLearn
Energy Conservation Equations of MotionA conventional derivation of motion equations in mechanics and field equations in field theory is based on the principle of least action with a proper Lagrangian. With a time-independent Lagrangian,…Nikolay A. Vinokurov·May 18, 2015SaveLearn
Static interaction between electrically polarisable particles in vacuoThe static interaction of a point charge and a polarisable particle and between two polarisable particles is discussed in vacuo, and force and energy considerations are made. In particular a critical…R. Coïsson·May 18, 2015SaveLearn
Analysis of transition between different ringing schemes of the church bellIn this paper we investigate dynamics of church bells, characterize their most common working regimes and investigate how to obtain them. To simulate the behavior of the yoke-bell-clapper system we…Piotr Brzeski, Tomasz Kapitaniak, Przemyslaw Perlikowski·May 17, 2015SaveLearn