Results 251 to 260 of about 8,817,528 (292)
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1993
Optical NMR and ESR spectroscopy - equivalent magnetic flux density and the circularly polarized laser the magnetostatic flux density of the electromagnetic field - development and classical interpretation the elementary static magnetic field of the photon the photon's magnetostatic flux quantum - symmetry and wave particle duality, fundamental ...
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Optical NMR and ESR spectroscopy - equivalent magnetic flux density and the circularly polarized laser the magnetostatic flux density of the electromagnetic field - development and classical interpretation the elementary static magnetic field of the photon the photon's magnetostatic flux quantum - symmetry and wave particle duality, fundamental ...
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Magnets and Magnetic Field Measurements
Science, 1955A L, Bloom, M E, Packard
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Physica B: Condensed Matter, 1995
Abstract After a summary of the observations of cosmic magnetic fields, I briefly discuss the status of dynamos, the use of electric circuits, the physics of magnetic explosions, the role of magnetic tension and our strongest magnet known, the radio pulsar. Finally I mention a few problem areas which may show a breakthrough in the near future.
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Abstract After a summary of the observations of cosmic magnetic fields, I briefly discuss the status of dynamos, the use of electric circuits, the physics of magnetic explosions, the role of magnetic tension and our strongest magnet known, the radio pulsar. Finally I mention a few problem areas which may show a breakthrough in the near future.
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2018
Classically, a point charge that circulates on a ring of radius r produces a current \(i = \frac{ev}{2 \pi r}\), which causes a magnetic dipole moment \(\overrightarrow{\mu }= \frac{i}{c} S \overrightarrow{n}\), \(S= \pi r^{2}\), in obvious notation; \(\overrightarrow{\mu }= \frac{e v}{2c} r \overrightarrow{n}= \frac{e}{2c} \overrightarrow{r} \wedge ...
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Classically, a point charge that circulates on a ring of radius r produces a current \(i = \frac{ev}{2 \pi r}\), which causes a magnetic dipole moment \(\overrightarrow{\mu }= \frac{i}{c} S \overrightarrow{n}\), \(S= \pi r^{2}\), in obvious notation; \(\overrightarrow{\mu }= \frac{e v}{2c} r \overrightarrow{n}= \frac{e}{2c} \overrightarrow{r} \wedge ...
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Limits of Low Magnetic Field Environments in Magnetic Shields
IEEE Transactions on Industrial Electronics, 2021Tianhao Liu, Liyi Li, Jiecai Han
exaly