QuasiresonanceThe concept of quasiresonance was introduced in connection with inelastic collisions between one atom and a vibro-rotationally excited diatomic molecule. In its original form, the collisions induce…Antonia Ruiz, Eric J. Heller·May 19, 2005SaveLearn
Torsional waves in a bowed stringBowing a string with a non-zero radius exerts a torque, which excites torsional waves. In general, torsional standing waves have higher fundamental frequencies than do transverse standing waves, and…Eric Bavu, John Smith, Joe Wolfe·May 9, 2005SaveLearn
Rotationnal and translational waves in a bowed stringWe measure and compare the rotational and transverse velocity of a bowed string. When bowed by an experienced player, the torsional motion is phase-locked to the transverse waves, producing highly…Eric Bavu, Manfred Yew, Pierre-Yves Placais et al.·May 9, 2005SaveLearn
Shear Instabilities in Granular Flows down on Inclined PlaneInstabilities at interface of two stream granular flows have been reported in recent experiment [1] that breaking waves can form at the interface between two streams of identical grains flowing on an…Hua-Shu Dou, Boo Cheong Khoo, Nhan Phan-Thien·May 3, 2005SaveLearn
Covariant Thermodynamics of an Object with Finite VolumeA covariant way to define the relativistic entropy of a finite object has been proposed. The energy-momentum of an object with finite volume is not a covariant physical entity because of the…Tadas K. Nakamura·Apr 30, 2005SaveLearn
The Faraday induction law in relativity theoryWe analyze the transformation properties of Faraday law in an empty space and its relationship with Maxwell equations. In our analysis we express the Faraday law via the four-potential of…Alexander L Kholmetskii, Oleg V. Missevitch·Apr 29, 2005SaveLearn
The Normalization Problem of Special RelativityFor the special theory of relativity, the normalization problem is formulated as the question how observers in constant relative motion may reach an agreement on space and time scales. As the…Franz-Guenter Winkler·Apr 28, 2005SaveLearn
Field Theory reformulated without self-energy parts.Divergence-free classical electrodynamicsA manifestly gauge-invariant hamiltonian formulation of classical electrodynamics has been shown to be relativistic invariant by the construction of the adequate generators of the Poincare Lie…M. de Haan·Apr 25, 2005SaveLearn
Electromagnetic Field Particles in the Classical TheoryThis simple analysis shows that photon-like particles are not strange within the conceptual framework of the classical electromagnetic field theory. Circular polarized waves lead to photons. Thus,…Srecko Botric, Krunoslav Ljolje·Apr 20, 2005SaveLearn
On the Nature of the Relativity PrincipleWe discuss the nature and a general formulation of the relativity principle and we show that it can be justified starting from a strictly operational point of view. We give some remark on the…M. Toller·Apr 19, 2005SaveLearn
Improving antenna near-field pattern by use of artificial impedance screensAn antenna prototype utilizing artificial impedance surfaces to control the near field distribution is described. The antenna is a folded dipole placed above a finite-size artificial impedance…Stanislav Maslovski, Pekka Ikonen, Constantin Simovski et al.·Apr 18, 2005SaveLearn
Commentary on `The Three-Dimensional Current and Surface Wave Equations' by George MellorThe lowest order sigma-transformed momentum equation given by Mellor (J. Phys. Oceangr. 2003) takes into account a phase-averaged wave forcing based on Airy wave theory. This equation is shown to be…Fabrice Ardhuin, Alastair D. Jenkins, Kostas Belibassakis·Apr 14, 2005SaveLearn
Deriving relativistic momentum and energy. II. Three-dimensional caseWe generalise a recent derivation of the relativistic expressions for momentum and kinetic energy from the one-dimensional to the three-dimensional case.Sebastiano Sonego, Massimo Pin·Apr 14, 2005SaveLearn
Inside Perspectives on Classical ElectromagnetismThe concept "Classical Electromagnetism" in the title of the paper here refers to a theory built on three foundations: relativity principles, the original Maxwell's equations, and the…Leif Pettersson·Apr 13, 2005SaveLearn
Angular momentum of the electromagnetic field: the plane wave paradox resolvedThe angular momentum of a classical electromagnetic plane wave of arbitrary extent is predicted to be, on theoretical grounds, exactly zero. However, finite sections of circularly polarized plane…A. M. Stewart·Apr 13, 2005SaveLearn
Billiards, Invariant Measures, and Equilibrium ThermodynamicsThe questions of justification of the Gibbs canonical distribution for systems with elastic impacts are discussed. A special attention is paid to the description of probability measures with…V. V. Kozlov·Apr 13, 2005SaveLearn
Testing a Crucial AssumptionSimplified description of an experiment of the Michelson-Morley type being completed at the University of Western Australia with a discussion of the possible meanings of its outcome.Ll. Bel·Apr 13, 2005SaveLearn
Patch antennas with new artificial magnetic layersA new type of high-impedance surfaces (HIS) has been introduced by C.R. Simovski et al. recently. In this paper, we propose to use such layers as artificial magnetic materials in the design of patch…M. Ermutlu, C. R. Simovski, M. Karkainen et al.·Apr 11, 2005SaveLearn
Monte Carlo transient phonons transport in silicon and germanium at nanoscalesHeat transport at nanoscales in semiconductors is investigated with a statistical method. The Boltzmann Transport Equation (BTE) which characterize phonons motion and interaction within the crystal…David Lacroix, Karl Joulain·Apr 11, 2005SaveLearn
Light-Weight Base Station Antenna with Artificial Wire Medium LensIn this paper we study the possibility of utilizing a loaded wire medium as an artificial material for beam shaping element in base station antenna applications. The wires in the lattice are loaded…Pekka Ikonen, Mikko Karkkainen, Constantin Simovski et al.·Apr 11, 2005SaveLearn
Canonically Transformed Detectors Applied to the Classical Inverse Scattering ProblemThe concept of measurement in classical scattering is interpreted as an overlap of a particle packet with some area in phase space that describes the detector. Considering that usually we record the…C Jung, T H Seligman, J M Torres·Apr 8, 2005SaveLearn
Perfect electromagnetic conductorIn differential-form representation, the Maxwell equations are represented by simple differential relations between the electromagnetic two-forms and source three-forms while the electromagnetic…Ismo V. Lindell, Ari Sihvola·Mar 31, 2005SaveLearn
Modélisation des déformations de maturation de la fibreThe generation mechanism of growth strains is investigated theoretically by developing an elastic analysis of a wood cell viewed as a composite tube, with layers composed of a ligno-cellulosic…François Sassus, Tancrède Alméras, Joseph Gril et al.·Mar 26, 2005SaveLearn
Role of the Gelatinous Layer (G-Layer) on the Origin of the Physical Properties of the Tension Wood of Acer sieboldianumThe tension wood (TW) properties of a 70 year-old Acer sieboldianum Miq were analyzed by using the G-fiber model which was proposed in our previous paper. The roles of the G-layer on the origins of…Hiroyuki Yamamoto, Kentaro Abe, Yoshiharu Arakawa et al.·Mar 26, 2005SaveLearn
Reduction of wood hygroscopicity and associated dimensional response by repeated humidity cyclesThe reduction of wood response to variations of ambient humidity, described as kind of ageing, has been studied from both points of view of moisture uptake and dimensional changes. Clearwood…Luis García Esteban, Joseph Gril, Paloma De Palacios De Palacios et al.·Mar 22, 2005SaveLearn