July 15, 2017

Download Applied Superconductivity. Volume II by Vernon L. Newhouse PDF

By Vernon L. Newhouse

Utilized Superconductivity, quantity II, is a part of a two-volume sequence on utilized superconductivity. the 1st quantity handled digital purposes and radiation detection, and includes a bankruptcy on liquid helium refrigeration. the current quantity discusses magnets, electromechanical functions, accelerators, and microwave and rf units.
The publication opens with a bankruptcy on high-field superconducting magnets, masking purposes and magnet layout. next chapters talk about superconductive equipment akin to superconductive bearings and automobiles; rf superconducting units; and destiny customers in utilized superconductivity.
Each bankruptcy within the volumes might be learn independently, and so much suppose little or no or no heritage within the physics of superconductivity. the subjects handled don't require using complex quantum mechanics; hence the books might be available to scholars or study employees in any department of engineering or physics. they're meant to serve either as a resource of reference fabric to latest ideas and as a advisor to destiny learn.

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Example text

We discuss here only the circular-aperture case, neglecting end effects but including the the effects of an iron shield (Iwasa and Weggel, 1972). In a region where no current exists, the magnetic field H is the gradient of a potential φ which satisfies Laplace's equation, namely, H = -νφ (25) 2 (26) νφ = 0 In two-dimensional polar coordinates, shown in Fig. 16, one class of φ is φη = cos nB/rn n φη = r cos ηθ r > R (27) r

707 in percent deviation from the central field. Also shown are lines of constant F (a, ß) and minimum-volume curve. FIG. 13b. The uniformity of the central field as in Fig. 13a for the higher ranges of ß. 6. HIGH-FIELD SUPERCONDUCTING MAGNETS 409 20 15 10 FIG. 14. The amount of superconducting material necessary versus the space factor λ for three solenoids with bore diameters of 1, 10, and 100 cm. 5 superconducting material alone can seldom be used to make a reliable con­ ductor; it must generally be embedded in a matrix of copper or other normal conductor, and, depending on the amount of normal conductor, the overall current density of the conductor, \jc, varies considerably.

Although idealized, two such winding schemes for the dipole and quadrupole are discussed, and solutions are presented. We begin first with a general approach in solving the magnetic field in a multipole magnet (Asner, 1969; Green, 1971). This is essential because idealized schemes are useful only as an overall design approach—several compromising factors must be taken into account, and it becomes necessary eventually to compute the magnetic field for a current distribution which differs from any idealized case.

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