17,139 research outputs found

    Spin current induced magnetization oscillations in a paramagnetic disc

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    When electron spins are injected uniformly into a paramagnetic disc, they can precess along the demagnetizing field induced by the resulting magnetic moment. Normally this precession damps out by virtue of the spin relaxation which is present in paramagnetic materials. We propose a new mechanism to excite a steady-state form of this dynamics by injecting a constant spin current into this paramagnetic disc. We show that the rotating magnetic field generated by the eddy currents provide a torque which makes this possible. Unlike the ferromagnetic equivalent, the spin-torque-oscillator, the oscillation frequency is fixed and determined by the dimensions and intrinsic parameters of the paramagnet. The system possesses an intrinsic threshold for spin injection which needs to be overcome before steady-state precession is possible. The additional application of a magnetic field lowers this threshold. We discuss the feasibility of this effect in modern materials. Transient analysis using pump-probe techniques should give insight in the physical processes which accompany this effect

    Ferromagnetic resonance study of polycrystalline Fe_{1-x}V_x alloy thin films

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    Ferromagnetic resonance has been used to study the magnetic properties and magnetization dynamics of polycrystalline Fe1x_{1-x}Vx_{x} alloy films with 0x<0.70\leq x < 0.7. Films were produced by co-sputtering from separate Fe and V targets, leading to a composition gradient across a Si substrate. FMR studies were conducted at room temperature with a broadband coplanar waveguide at frequencies up to 50 GHz using the flip-chip method. The effective demagnetization field 4πMeff4 \pi M_{\mathrm{eff}} and the Gilbert damping parameter α\alpha have been determined as a function of V concentration. The results are compared to those of epitaxial FeV films

    Synchronization Of Video Kinematic And Analog Biomechanical Data Using The Motion Analysis System

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    A significant advantage of using integrated biomechanical data collection systems to study human movement is the simultaneous storage in a single computer of video-derived kinematic data and digitized records of analog data such as force and electromyographic signals. However care must be taken to assure that these records are properly synchronized by the respective data-logging parts of the hardware and software. This is particularly important when the data are combined to calculate dynamic values such as net joint moments. We have studied data synchronization using the Motion Analysis Corporation's Expertvision 60Hz video system (VP320) and have identified three important issues: 1) sampling rate; 2) video sampling initiation; and 3) intra-frame video/analog initiation synchronization. The first issue, sampling rate, arises since each data collection process assigns time values throughout the data based on a nominal sampling rate. Errors in this assumed rate will cause increasing cumulative synchronization error throughout the sampling interval unless appropriate corrections are appplied. We have found the analog data collection rates to be sufficiently accurate (within the lOO-2KHz range), but the video sampling rate deviates from the nominal 60Hz by 1-2.5%, depending on the hardware version. This error requires a software adjustment to the packaged calculation of video frame times. The second issue, video sampling initiation, occurs because the video collection triggering process starts by storing (as "Frame 1") the second video field to occur after the detection of the trigger signal. Since the A/D conversion of analog signals uses the same algorithm but (usually) a much faster sample rate, the analog sample begins nearly one video frame interval ahead of the video sample. This constant initiation time offset must be corrected before post-hoc data analysis. The third issue compounds the initiation correction procedure, as the trigger signal (and subsequent analog data collection) may occur at any point between two video frames, introducing an additional random offset ranging from 0-1 7ms. In many applications this amount of error is unacceptable, and correction in the form of external video synchronization is required. One simple way to accomplish this is to lead the video synch pulse into an unused A/D channel; another is to use a pulsed light in the video record which is also sampled by the A/D system. Synchronization errors are system-specific, and may be constant or variable. Collection of accurately synchronized video kinematic and analog data requires careful attention and post processing to correct these three sources of potential error

    Noncentral extensions as anomalies in classical dynamical systems

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    A two cocycle is associated to any action of a Lie group on a symplectic manifold. This allows to enlarge the concept of anomaly in classical dynamical systems considered by F. Toppan [in J. Nonlinear Math. Phys. 8, no.3 (2001) 518-533] so as to encompass some extensions of Lie algebras related to noncanonical actions.Comment: arxiv version is already officia

    A kinetic model of radiating electrons

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    A kinetic theory is developed to describe radiating electrons whose motion is governed by the Lorentz-Dirac equation. This gives rise to a generalized Vlasov equation coupled to an equation for the evolution of the physical submanifold of phase space. The pathological solutions of the 1-particle theory may be removed by expanding the latter equation in powers of τ ≔ q 2/6πm. The radiation-induced change in entropy is explored and its physical origin is discussed. As a simple demonstration of the theory, the radiative damping rate of longitudinal plasma waves is calculated

    Feasibility of reduced gravity experiments involving quiescent, uniform particle cloud combustion

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    The study of combustible particle clouds is of fundamental scientific interest as well as a practical concern. The principal scientific interests are the characteristic combustion properties, especially flame structure, propagation rates, stability limits, and the effects of stoichiometry, particle type, transport phenomena, and nonadiabatic processes on these properties. The feasibility tests for the particle cloud combustion experiment (PCCE) were performed in reduced gravity in the following stages: (1) fuel particles were mixed into cloud form inside a flammability tube; (2) when the concentration of particles in the cloud was sufficiently uniform, the particle motion was allowed to decay toward quiescence; (3) an igniter was energized which both opened one end of the tube and ignited the suspended particle cloud; and (4) the flame proceeded down the tube length, with its position and characteristic features being photographed by high-speed cameras. Gravitational settling and buoyancy effects were minimized because of the reduced gravity enviroment in the NASA Lewis drop towers and aircraft. Feasibility was shown as quasi-steady flame propagation which was observed for fuel-rich mixtures. Of greatest scientific interest is the finding that for near-stoichiometric mixtures, a new mode of flame propagation was observed, now called a chattering flame. These flames did not propagate steadily through the tube. Chattering modes of flame propagation are not expected to display extinction limits that are the same as those for acoustically undisturbed, uniform, quiescent clouds. A low concentration of fuel particles, uniformly distributed in a volume, may not be flammable but may be made flammable, as was observed, through induced segregation processes. A theory was developed which showed that chattering flame propagation was controlled by radiation from combustion products which heated the successive discrete laminae sufficiently to cause autoignition

    The impact of lightning on tropospheric ozone chemistry using a new global lightning parametrisation

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    A lightning parametrisation based on upward cloud ice flux is implemented in a chemistry–climate model (CCM) for the first time. The UK Chemistry and Aerosols model is used to study the impact of these lightning nitric oxide (NO) emissions on ozone. Comparisons are then made between the new ice flux parametrisation and the commonly used, cloud-top height parametrisation. The ice flux approach improves the simulation of lightning and the temporal correlations with ozone sonde measurements in the middle and upper troposphere. Peak values of ozone in these regions are attributed to high lightning NO emissions. The ice flux approach reduces the overestimation of tropical lightning apparent in this CCM when using the cloud-top approach. This results in less NO emission in the tropical upper troposphere and more in the extratropics when using the ice flux scheme. In the tropical upper troposphere the reduction in ozone concentration is around 5–10 %. Surprisingly, there is only a small reduction in tropospheric ozone burden when using the ice flux approach. The greatest absolute change in ozone burden is found in the lower stratosphere, suggesting that much of the ozone produced in the upper troposphere is transported to higher altitudes. Major differences in the frequency distribution of flash rates for the two approaches are found. The cloud-top height scheme has lower maximum flash rates and more mid-range flash rates than the ice flux scheme. The initial Ox (odd oxygen species) production associated with the frequency distribution of continental lightning is analysed to show that higher flash rates are less efficient at producing Ox; low flash rates initially produce around 10 times more Ox per flash than high-end flash rates. We find that the newly implemented lightning scheme performs favourably compared to the cloud-top scheme with respect to simulation of lightning and tropospheric ozone. This alternative lightning scheme shows spatial and temporal differences in ozone chemistry which may have implications for comparison between models and observations, as well as for simulation of future changes in tropospheric ozone

    The free rigid body dynamics: generalized versus classic

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    In this paper we analyze the normal forms of a general quadratic Hamiltonian system defined on the dual of the Lie algebra o(K)\mathfrak{o}(K) of real KK - skew - symmetric matrices, where KK is an arbitrary 3×33\times 3 real symmetric matrix. A consequence of the main results is that any first-order autonomous three-dimensional differential equation possessing two independent quadratic constants of motion which admits a positive/negative definite linear combination, is affinely equivalent to the classical "relaxed" free rigid body dynamics with linear controls.Comment: 12 page

    A Rigorous Derivation of Electromagnetic Self-force

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    During the past century, there has been considerable discussion and analysis of the motion of a point charge, taking into account "self-force" effects due to the particle's own electromagnetic field. We analyze the issue of "particle motion" in classical electromagnetism in a rigorous and systematic way by considering a one-parameter family of solutions to the coupled Maxwell and matter equations corresponding to having a body whose charge-current density Ja(λ)J^a(\lambda) and stress-energy tensor Tab(λ)T_{ab} (\lambda) scale to zero size in an asymptotically self-similar manner about a worldline γ\gamma as λ0\lambda \to 0. In this limit, the charge, qq, and total mass, mm, of the body go to zero, and q/mq/m goes to a well defined limit. The Maxwell field Fab(λ)F_{ab}(\lambda) is assumed to be the retarded solution associated with Ja(λ)J^a(\lambda) plus a homogeneous solution (the "external field") that varies smoothly with λ\lambda. We prove that the worldline γ\gamma must be a solution to the Lorentz force equations of motion in the external field Fab(λ=0)F_{ab}(\lambda=0). We then obtain self-force, dipole forces, and spin force as first order perturbative corrections to the center of mass motion of the body. We believe that this is the first rigorous derivation of the complete first order correction to Lorentz force motion. We also address the issue of obtaining a self-consistent perturbative equation of motion associated with our perturbative result, and argue that the self-force equations of motion that have previously been written down in conjunction with the "reduction of order" procedure should provide accurate equations of motion for a sufficiently small charged body with negligible dipole moments and spin. There is no corresponding justification for the non-reduced-order equations.Comment: 52 pages, minor correction
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