Special Theory of Relativity through the Doppler EffectWe present the special theory of relativity taking the Doppler effect as the starting point, and derive several of its main effects, such as time dilation, length contraction, addition of velocities,…M. Moriconi·May 24, 2006SaveLearn
Coherent thermodynamical modelling of geomaterial reinforced by wiresThe TexSol is a composite geomaterial : a sand matrix and a wire network reinforcement. For small strains a thermodynamical continuous model of the TexSol including the unilaterality of the wire…Romain Laniel, Pierre Alart, Stéphane Pagano·May 23, 2006SaveLearn
Three methods for the description of the temporal response to a SH plane impulsive seismic wave in a soft elastic layer overlying a hard elastic substratumWe treat the case of a flat stress-free surface (i.e., the ground in seismological applications) separating air from a homogeneous, isotropic, solid substratum overlain by a homogeneous, isotropic,…Armand Wirgin·May 15, 2006SaveLearn
Nonequilibrium Approach to Bloch-Peierls-Berry DynamicsWe examine the Bloch-Peierls-Berry dynamics under a classical nonequilibrium dynamical formulation. In this formulation all coordinates in phase space formed by the position and crystal momentum…John Olson, Ping Ao·May 12, 2006SaveLearn
Poincare's relativistic Doppler-Fizeau formulaWe deduce from Poincare's ellipsoidal wavefronts a relativistic Doppler-Fizeau formula that is not the same as 1905 Einstein's one. Longitudinally, Einstein's formula and Poincare's…Yves Pierseaux·May 8, 2006SaveLearn
Radiation enhancement and radiation suppression by a left-handed metamaterialThe perfect lens property of a dispersive and lossy left-handed metamaterial (LHM) disk is exploited to superimpose a source of electromagnetic radiation onto its mirror image, formed as a result of…A. D. Boardman, K. Marinov·May 6, 2006SaveLearn
Wave Equation for Fractal Solid StringWe use the fractional integrals to describe fractal solid. We suggest to consider the fractal solid as special (fractional) continuous medium. We replace the fractal solid with fractal mass dimension…Vasily E. Tarasov·Apr 29, 2006SaveLearn
Connecting Blackbody Radiation, Relativity, and Discrete Charge in Classical ElectrodynamicsIt is suggested that an understanding of blackbody radiation within classical physics requires the presence of classical electromagnetic zero-point radiation, the restriction to relativistic…Timothy H. Boyer·Apr 28, 2006SaveLearn
Excitation of surface dipole and solenoidal modes on toroidal structuresThe time dependent Schrodinger equation inclusive of curvature effects is developed for a spinless electron constrained to motion on a toroidal surface and subjected to circularly polarized and…M. Encinosa, M. Jack·Apr 27, 2006SaveLearn
Chaotic Emission from Electromagnetic Systems Considering Self-InteractionThe emission of electromagnetic waves from a system described by the Hénon-Heiles potential is studied in this work. The main aim being to analyze the behavior of the system when the damping term is…Fernando Kokubun, Vilson T. Zanchin·Apr 25, 2006SaveLearn
Vibrational dynamics of confined granular materialBy means of two-dimensional contact dynamics simulations, we analyze the vibrational dynamics of a confined granular layer in response to harmonic forcing. We use irregular polygonal grains allowing…Emilien Azema, Farhang Radjaï, Robert Peyroux et al.·Apr 21, 2006SaveLearn
Comment on "Gauge transformations are Canonical transformations"We comment on the work of Tai L Chow, Eur. J. Phys. 18, 467 (1997). By considering the Lagrangians which are uniquely defined only to within an additive total time derivative of a function of…Pathikrit Bhattacharya, Bhabani Prasad Mandal·Apr 21, 2006SaveLearn
Stationary solutions and Neumann boundary conditions in the Sivashinsky equationNew stationary solutions of the (Michelson) Sivashinsky equation of premixed flames are obtained numerically in this paper. Some of these solutions, of the bicoalescent type recently described by…Bruno Denet·Apr 17, 2006SaveLearn
Delayed Choice Between Purely Classical StatesIt is argued that Wheeler's insightful idea of delayed choice experiments may be explored at a classical level, arising naturally from number-theoretical conjugacies always necessarily present in…Jason A. C. Gallas·Apr 11, 2006SaveLearn
On the vector solutions of Maxwell equations with the spin-weighted spherical harmonicsThe discussion of our recent work concerning the vector solution of boundary-value problems in electromagnetism is extended to the case of no azimuthal symmetry by means of the spin-weighted…E. A. Matute·Apr 11, 2006SaveLearn
On the Solution of Maxwell's First Order EquationsIn an attempt to solve Maxwell's first order system of equations, starting from a given initial state, it is found that a consistent solution depending on the temporal evolution of the sources…Wolfgang Engelhardt·Apr 5, 2006SaveLearn
The clock paradox in a static homogeneous gravitational fieldThe gedanken experiment of the clock paradox is solved exactly using the general relativistic equations for a static homogeneous gravitational field. We demonstrate that the general and special…Preston Jones, Lucas F. Wanex·Apr 4, 2006SaveLearn
From Maxwell Stresses to Nonlinear Field EquationsThis paper aims to show that making use of Newton's view on equations of motion of a physical system and of the Maxwell stress tensor we come to a natural nonlinearization of Maxwell equations in…Stoil Donev, Maria Tashkova·Apr 4, 2006SaveLearn
Electromagnetic braking: a simple quantitative modelA calculation is presented which quantitatively accounts for the terminal velocity of a cylindrical magnet falling through a long copper or aluminum pipe. The experiment and the theory are a dramatic…Yan Levin, Fernando L. da Silveira, Felipe B. Rizzato·Mar 31, 2006SaveLearn
The motion of two masses coupled to a massive springWe discuss the classical motion of a spring of arbitrary mass coupled to two arbitrary massive blocks attached at its ends. A general approach to the problem is presented and some general results are…F C Santos, Y A Coutinho, L Ribeiro-Pinto et al.·Mar 29, 2006SaveLearn
Efficiency of Carnot Cycle with Arbitrary Gas Equation of StateThe derivation of the efficiency of Carnot cycle is usually done by calculating the heats involved in two isothermal processes and making use of the associated adiabatic relation for a given working…Paulus C. Tjiang, Sylvia H. Sutanto·Mar 27, 2006SaveLearn
Electromagnetic energy in a dispersive metamaterialAn expression for the electromagnetic field energy density in a dispersive, lossy, left-handed metamaterial, consisting of an array of split-ring resonators and an array of wires is derived. An…A. D. Boardman, K. Marinov·Mar 23, 2006SaveLearn
Skopje and Sofia 2005 Earthquake and Geomagnetic data and the Geomagnetic Quake as Imminent Reliable Earthquakes PrecursorThe imminent WHEN earthquake predictions are based on the correlation between geomagnetic quakes and the incoming minimum (or maximum) of tidal gravitational potential. The probability time window…S. Cht. Mavrodiev, L. Pekevski·Mar 23, 2006SaveLearn
Mass, Time, and Clock (Twin) Paradox in Relativity TheoryThe paper is intended to clarify operational meaning of mass and time quantities as main characteristics of an atomic clock, which is considered a quantum oscillator in association with the de…Anatoli Vankov·Mar 21, 2006SaveLearn
h is classicalRegardless of number, standing wave modes are by definition noninteracting, and therefore cannot thermalize by themselves. Doppler shifts due to thermal motions of cavity walls provide necessary…V. Guruprasad·Mar 21, 2006SaveLearn