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Superconducting Magnet Systems

Specificaties
Paperback, blz. | Engels
Springer Berlin Heidelberg | 0e druk, 2011
ISBN13: 9783642807237
Rubricering
Springer Berlin Heidelberg 0e druk, 2011 9783642807237
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Samenvatting

The renaissance of magnet technology started in the early 1950s with the establishment of high-energy accelerators. About a decade later in 1961, or fifty years after the discovery of superconductivity, high-field superconducting laboratory magnets became a reality. Conventional still the major beam-handling and experimen­ electromagnets, which are tal devices used in laboratories, operate at zero efficiency. To generate high magnetic fields in a useful volume, considerable amounts of power are needed. Superconducting d. c. magnets do not require any power at all. It is somewhat depressing to note that, sixty years after the first superconductor was tested, the experimental d. c. superconducting mag­ net is still the only large-scale equipment operated in laboratories. Al­ though there has been considerable activity in the area of superconduc­ tivity, superconductors are used on quite a modest scale in electronic and quantum devices, in medicine and biology, and in physical experi­ ments where high magnetic fields are essential. It is only recently that Type II superconductors have been introduced in power engineering (power generation, storage and transport) to replace pulsed accelerator magnets; for fast and economical transportation vehicles (levitated trains) where superconductors may ultimately replace the wheel; to make new means of en~rgy generation economically feasible, such as in magneto­ hydrodynamics and in fusion reactors; and for high-efficiency electric motors. High-field superconducting magnets are being proposed for de­ salination of seawater, for magnetic separation in the mining industry, for cleaning polluted water, and for sewage treatment.

Specificaties

ISBN13:9783642807237
Taal:Engels
Bindwijze:paperback
Uitgever:Springer Berlin Heidelberg
Druk:0

Inhoudsopgave

1. Methods of Magnetic Field Generation.- 1.1 High Magnetic Field Laboratories.- 1.2 Conventional Continuous Duty Magnets with and without Iron.- 1.3 Pulsed Magnets.- 1.4 Cryogenic Magnets.- 1.5 Superconducting Coils.- References.- 2. Magnetic Field Calculations.- 2.1 Magnets without Ferromagnetic Yokes.- 2.2 Magnetic Fields due to Coils in Proximity to Ferromagnetic-Materials.- 2.3 Field Calculation of Iron-Bound Air-Core Magnets.- 2.4 Calculation of Forces.- 2.5 Calculation of Heating.- References.- 3. Phenomena and Theory of Superconductivity.- 3.1 Theory.- 3.2 Critical Fields of Type II Superconductors.- 3.3 Critical Currents of Type II Superconductors.- References.- 4. Superconducting Alternating Current Magnets.- 4.1 Alternating Current Losses.- 4.2 Additional Effects in Twisted Multifilamentary Conductors.- 4.3 Eddy Current Losses in Metallic Parts.- 4.4 Multifilamentary Conductors.- 4.5 Comparison of Loss-Calculation with Experiments.- 4.6 Methods of Loss Measurement.- 4.7 Magnetic and Thermal Instabilities.- 4.8 A.C. Magnet Fabrication Techniques.- 4.9 Irradiation Effects in Superconducting Magnets.- References.- 5. Cryogenics.- 5.1 General Properties of Cryogenic Fluids.- 5.2 Low Temperature Processes.- 5.3 Liquefaction and Refrigeration.- 5.4 Handling and Storage of Cryogenic Fluids.- 5.5 Physical Properties of Cryogenic Fluids.- 5.6 Physical Properties of Solids.- 5.7 Heat Losses.- References.- 6. Economic Consideration in the Design of Water-Cooled, Cryogenic and Superconducting Magnets.- 6.1 Introduction.- 6.2 Cost Comparison for Specific Magnet Systems.- 6.3 Cost Comparison in General.- References.- 7. Examples of Superconducting Magnet Systems.- 7.1 The Argonne National Laboratory 3.7-m Hydrogen Bubble-Chamber Magnet.- 7.2 The CERN Liquid Hydrogen Bubble-Chamber Magnet.- 7.3 Composite Magnet System, the McGill and MIT Hybrid Magnets.- 7.4 The Oak-Ridge -IMP -Superconducting Coil System.- 7.5 The SLAC 7 T, 30-cm Bore, Helmholtz Magnet.- References.

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        Superconducting Magnet Systems