"Low-order longitudinal modes of single-component plasmas" Physics of Plasmas 2 (1995), pp. 2880-2894. M. D. Tinkle, R. G. Greaves, and C. M. Surko (PDF)
... For the special case of the center-of-massmode, the assumption that odd-l coefficients vanish is not valid, because the plasma has a time-varying dipole moment. A treatment similar to that just describedfor the quadrupoleimage charge field inducedby the monopole moment of the plasmamay be used to c ...
... For the special case of the center-of-massmode, the assumption that odd-l coefficients vanish is not valid, because the plasma has a time-varying dipole moment. A treatment similar to that just describedfor the quadrupoleimage charge field inducedby the monopole moment of the plasmamay be used to c ...
Elmer non-GUI Tutorials
... General Public License as published by the Free Software Foundation; either version 2 of the License, or (at your option) any later version. Elmer software is distributed in the hope that it will be useful, but without any warranty. See the GNU General Public License for more details. Elmer includes ...
... General Public License as published by the Free Software Foundation; either version 2 of the License, or (at your option) any later version. Elmer software is distributed in the hope that it will be useful, but without any warranty. See the GNU General Public License for more details. Elmer includes ...
The Gravitational Spacecraft
... There is an electromagnetic factor of correlation between gravitational mass and inertial mass, which in specific electromagnetic conditions, can be reduced, made negative and increased in numerical value. This means that gravitational forces can be reduced, inverted and intensified by means of elec ...
... There is an electromagnetic factor of correlation between gravitational mass and inertial mass, which in specific electromagnetic conditions, can be reduced, made negative and increased in numerical value. This means that gravitational forces can be reduced, inverted and intensified by means of elec ...
chapter 12
... As mentioned in the preceding chapter, a transmission line can be used to guide EM energy from one point (generator) to another (load). A waveguide is another means of achieving the same goal. However, a waveguide differs from a transmission line in some respects, although we may regard the latter a ...
... As mentioned in the preceding chapter, a transmission line can be used to guide EM energy from one point (generator) to another (load). A waveguide is another means of achieving the same goal. However, a waveguide differs from a transmission line in some respects, although we may regard the latter a ...
Computer Simulation of the Stockmayer Fluid
... each other at close range. Based on this concept, the first microscopic theory of phase change, i.e. gas-liquid transition, was developed by van der Waals. This simple picture of molecular interaction may be extended to complex phenomenological force fields which, if properly parametrized, yield pre ...
... each other at close range. Based on this concept, the first microscopic theory of phase change, i.e. gas-liquid transition, was developed by van der Waals. This simple picture of molecular interaction may be extended to complex phenomenological force fields which, if properly parametrized, yield pre ...
Extremely Low Frequency (ELF) Radio Wave Propagation: A review
... Earth‟s radius of ~6366 km. This non-conducting layer forms a spherical cavity resonator, with two sets of eigen-values. One of them corresponds to the global electromagnetic resonance predicted by Schumann [1952], which is often regarded as SR. Its peak frequencies (frequencies of maxima in the pow ...
... Earth‟s radius of ~6366 km. This non-conducting layer forms a spherical cavity resonator, with two sets of eigen-values. One of them corresponds to the global electromagnetic resonance predicted by Schumann [1952], which is often regarded as SR. Its peak frequencies (frequencies of maxima in the pow ...
Long-term unsteadiness and large-scale structures in Rayleigh-Bénard convection
... Boundary layers in Rayleigh-Bénard convection The second part of this thesis comprises a study of the boundary layer behaviour of RB convection in the aspect-ratio-4 cell. For a wide range of Rayleigh (Ra) numbers varying between 7.0 × 104 and 2.4 × 109 , the results of LDA measurements and direct ...
... Boundary layers in Rayleigh-Bénard convection The second part of this thesis comprises a study of the boundary layer behaviour of RB convection in the aspect-ratio-4 cell. For a wide range of Rayleigh (Ra) numbers varying between 7.0 × 104 and 2.4 × 109 , the results of LDA measurements and direct ...
Superconducting qubits coupled to nanoelectromechanical resonators: An architecture
... builds on the interesting recent theoretical work by Armour et al. 关33,34兴 and Irish et al. 关35兴 on the entanglement of a nanoelectromechanical resonator with a single Cooper-pair box. In fact, there is currently a big effort to push a variety of nanomechanical systems to the quantum limit 关53–55兴. ...
... builds on the interesting recent theoretical work by Armour et al. 关33,34兴 and Irish et al. 关35兴 on the entanglement of a nanoelectromechanical resonator with a single Cooper-pair box. In fact, there is currently a big effort to push a variety of nanomechanical systems to the quantum limit 关53–55兴. ...
Time in physics
Time in physics is defined by its measurement: time is what a clock reads. In classical, non-relativistic physics it is a scalar quantity and, like length, mass, and charge, is usually described as a fundamental quantity. Time can be combined mathematically with other physical quantities to derive other concepts such as motion, kinetic energy and time-dependent fields. Timekeeping is a complex of technological and scientific issues, and part of the foundation of recordkeeping.