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Shields for the starship Enterprise
Shields for the starship Enterprise

Excitation of molecules in dense clouds
Excitation of molecules in dense clouds

R07 Set No. 2
R07 Set No. 2

The direction of the magnetic field B at any location
The direction of the magnetic field B at any location

Hamiltonian Mechanics and Single Particle Motion
Hamiltonian Mechanics and Single Particle Motion

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Adaptation of Ultra-Precise Atomic Mass Measurement
Adaptation of Ultra-Precise Atomic Mass Measurement



II. The induced emf in a coil in a varying magnetic field.
II. The induced emf in a coil in a varying magnetic field.

... the resistor current would be the voltage drop divided by 5.00 Ω. Thus it should be about 6 A. This is also the current through the solenoid which is in series with the resistor. 2. The Graph Tool provides a more precise reading of the current than the power supply. So we’ll always use it for our da ...
Time-Dependent Meson Melting in External Magnetic Field
Time-Dependent Meson Melting in External Magnetic Field

finite element modelling of electric currents in ac
finite element modelling of electric currents in ac

... significant horizontal dissipation, and that very little current flows near the walls. This is consistent with the results for the round furnace. The current path in the matte is concentrated near the top surface. The dominant path is between electrodes 2 and 3, and 4 and 5. The concentration of cur ...
A model of slingshot prominences in rapidly rotating stars
A model of slingshot prominences in rapidly rotating stars

i. electricity and magnetism i
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SPH4U Sample Test - Electric & Magnetic Fields

On ion gyro-harmonic structuring in the stimulated electromagnetic
On ion gyro-harmonic structuring in the stimulated electromagnetic

... A. Samimi et al.: Ion gyro-structures in the SEE spectrum field relative to the magnetic field. Our calculations show that the threshold electric field intensity required to excite the oblique IA wave is actually higher than for the neutralized IB mode. Since the oblique IA wave is excited by strong ...
XRD - Shodhganga
XRD - Shodhganga

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Magnetic Pulsations: Sources and Properties

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Electron dynamics in inhomogeneous magnetic fields
Electron dynamics in inhomogeneous magnetic fields

... random magnetic field with zero average breaks time reversal symmetry locally and randomly. The disruption of extended states by the random potential a priori provides a good reason to expect electron localization and an insulating behaviour in the random magnetic field [1–3]. Zhang and Arovas [4] h ...
Magnetic Interactions in Low-Dimensional Iron Nanostructures
Magnetic Interactions in Low-Dimensional Iron Nanostructures

... Skomski. Their knowledgeable guidance and patient tutoring carried me throughout my program. I cannot remember how many times that I approached them with questions and puzzles and left with answers and ideas. It is their supports that have led me through the most challenging time of my life. I would ...
Manipulating exciton fine-structure in quantum dots with a lateral electric field
Manipulating exciton fine-structure in quantum dots with a lateral electric field

... biases. At high excitation powers the Stark effect is strongly reduced due to space-charge accumulation in the device. At low powers Stark shifts of ~ 1.5 meV are observed for an applied bias of 10V. ...
Jonti`s first lecture (Magnetism)
Jonti`s first lecture (Magnetism)

Document
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PVT Insensitive Reference Current Generation
PVT Insensitive Reference Current Generation

- Sussex Research Online
- Sussex Research Online

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Superconductivity



Superconductivity is a phenomenon of exactly zero electrical resistance and expulsion of magnetic fields occurring in certain materials when cooled below a characteristic critical temperature. It was discovered by Dutch physicist Heike Kamerlingh Onnes on April 8, 1911 in Leiden. Like ferromagnetism and atomic spectral lines, superconductivity is a quantum mechanical phenomenon. It is characterized by the Meissner effect, the complete ejection of magnetic field lines from the interior of the superconductor as it transitions into the superconducting state. The occurrence of the Meissner effect indicates that superconductivity cannot be understood simply as the idealization of perfect conductivity in classical physics.The electrical resistivity of a metallic conductor decreases gradually as temperature is lowered. In ordinary conductors, such as copper or silver, this decrease is limited by impurities and other defects. Even near absolute zero, a real sample of a normal conductor shows some resistance. In a superconductor, the resistance drops abruptly to zero when the material is cooled below its critical temperature. An electric current flowing through a loop of superconducting wire can persist indefinitely with no power source.In 1986, it was discovered that some cuprate-perovskite ceramic materials have a critical temperature above 90 K (−183 °C). Such a high transition temperature is theoretically impossible for a conventional superconductor, leading the materials to be termed high-temperature superconductors. Liquid nitrogen boils at 77 K, and superconduction at higher temperatures than this facilitates many experiments and applications that are less practical at lower temperatures.
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