'Applied field' presentation slideshows

11.1 Band Theory of Solids 11.2 Semiconductor Theory 11.3 Semiconductor Devices 11.4 Nanotechnology

CHAPTER 11 Semiconductor Theory and Devices. 11.1 Band Theory of Solids 11.2 Semiconductor Theory 11.3 Semiconductor Devices 11.4 Nanotechnology.

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Introduction to NMR Physics

Introduction to NMR Physics. Terry M. Button, Ph.D. Tiny Magnets. Nucleons behave as small current carrying loops. Such current carrying loops give rise to a small magnetic field. Tiny Magnets. Like nucleons pair such their net magnetic fields cancel.

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MHD induction & dynamo

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Limits in a RF cavity

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Collision Cross Section:

Collision Cross Section:. Ideal elastic hard sphere collision:. Where W is the collision cross-section. Where d is the collision distance. These equations negate potential interactions between the two molecules (atoms), attractive and repulsive, and assume spherical geometry. r 2. r 1.

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MHD in the Spherical Tokamak

Office of Science. Supported by. 21 st IAEA Fusion Energy Conference, Chengdu, China, 2006. MHD in the Spherical Tokamak. EX/7-2Ra.

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Magnetism on the verge of breakdown

Magnetism on the verge of breakdown. H. Aourag Laboratory for Study and Prediction of Materials URMER; University of Tlemcen. ? What is magnetism? ? Examples of collective behaviour ? Itinerant magnetism ? Disappearance of magnetism ? Quantum critical points ? Metamagnetism.

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Liquid Crystal Elastomer Dielectric Constant Measurements

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Bruce Mayer, PE Registered Electrical & Mechanical Engineer BMayer@ChabotCollege

Engineering 45. Electrical Properties-3. Bruce Mayer, PE Registered Electrical & Mechanical Engineer BMayer@ChabotCollege.edu. Learning Goals – Dielectrics. Understand the fundamentals of Electrical Capacitance How Certain Materials can Dramatically Increase the Electrical Capacity

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Smolenice, 25. a 26.9.2006

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Smolenice, 25. a 26.9.2006

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Lecture 7b Magnetism

Lecture 7b Magnetism. Contents 7.5 Magnetic properties of materials 7.6 Soft ferromagnetic materials 7.7 Hard ferromagnetic materials 7.8 Paramagnetism and diamagnetism. 7.5 Magnetic properties of materials.

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Chamber Clearing by Electrostatic Fields

Chamber Clearing by Electrostatic Fields. L. Bromberg ARIES Meeting UCSD January 10, 2002. Motivation. Aerosols are created in chamber due to large heating flux on surface of liquid Aerosols are charged, due to presence of plasma afterglow following the pulse

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Wave phenomena in radar meteorology

Wave phenomena in radar meteorology. Chris Westbrook. Rayleigh (small size compared to wavelength). Reflectivity, Z - Measure of intensity reflected back to radar:. Almost no phase difference (uniform E - field) across particle: wave blind to details, scatters

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Lecture 5

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Capillary Electrophoresis

Capillary Electrophoresis. Separation of analyte ions via differential migration in an electric field, coupled with electro-osmotic flow of mobile phase. Advantages Only needs nL sample High speed and resolution, virtually no band broadening Instrumentation

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Nice, round particle

Silica-Polypeptide Composite Particles (and Worms) Paul S. Russo, Louisiana State University, DMR 1005707.

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ABSTRACT

Magnetically Inhomogeneous Plasmas & Space Charge Robert Sheldon NASA/MSFC/NSSTC. R STAG 1.4 10.4 1.25 65 20 20 25. B 0 (nT) 330 31,000 < 6 430,000 21,000 23,000 14,000. E RAD 4 keV 5 MeV < 1.5 eV 150 MeV 1.2 MeV 1.4 MeV

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YBCO: Tape, || Tape-plane, SuperPower. 1,000,000. (Used in NHMFL tested Insert Coil 2007). At 4.2 K Unless. YBCO: Tape, |_ Tape Plane, SuperPower. (Used in NHMFL tested Insert Coil 2007). Otherwise Stated. YBCO B||c. Bi-2212: non-Ag J c , 427 fil. round wire,. YBCO B||ab.

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