By Vernon L. Newhouse
Utilized Superconductivity, quantity II, is a part of a two-volume sequence on utilized superconductivity. the 1st quantity handled digital functions and radiation detection, and features a bankruptcy on liquid helium refrigeration. the current quantity discusses magnets, electromechanical purposes, accelerators, and microwave and rf units.
The booklet opens with a bankruptcy on high-field superconducting magnets, masking functions and magnet layout. next chapters speak about superconductive equipment equivalent to superconductive bearings and cars; rf superconducting units; and destiny customers in utilized superconductivity.
Each bankruptcy within the volumes may be learn independently, and so much imagine little or no or no history within the physics of superconductivity. the subjects taken care of don't require using complex quantum mechanics; therefore the books could be obtainable to scholars or learn employees in any department of engineering or physics. they're meant to serve either as a resource of reference fabric to latest concepts and as a consultant to destiny study.
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Extra info for Applied Superconductivity. Volume II
3426 K=4 Ci aj/ai W*! 6798 (sin(2n -l)ak-Bin(2n-l)aii_1} the iron shield. For this scheme, it can be shown that Dn(K, n, ci) = 2 (2n - 1) (3 - 2n) (ci ny£[er-en X [sin(2n — 1)«* — sin(2n — 1)α*_ι] DniKyUyd) = d2n(2n- 2 l ) ( 2 n + 1) (ci (53) =π£[(Τ-©Π X [sin(2n — 1)αΛ — sin(2n — 1)α*_ι] (54) «A, bk, oik, Dn, and Dn are given in Table II. d. Quadrupoles. A procedure entirely similar to that used for the dipole is applicable here. Again, we examine two winding schemes analogous to those examined for the dipole and obtain appropriate expressions for the field.
81). The factor eQ(ci, bi/bB) is given for lines of constant bi/bB plotted versus d. ii. QUADRUPOLES. 2(ci «Q(CI, bi/bs) is plotted in Fig. 23. l)j\QiJ J/m (82) 428 B. Y. IWASA AND D. B. MONTGOMERY MATERIALS, CONDUCTOR CONFIGURATIONS, AND STABILITY 1. High-field, high-current superconductors The properties a material should have to be practical for the construction of superconducting magnets are (1) (2) (3) (4) (5) (6) high upper critical field, Hc2; high critical current density, Je; high critical temperature, Tc; good strength and ductility; high stability; availability in quantity.
In practice, however, such a large cross section in a single-core configuration is never used for magnets of any size. Instabilities inherent in large-size superconductors make it im possible to operate such a magnet successfully. Furthermore, the alloy, no matter how small its cross section, is rarely used alone: for stability it is always cladded with a high-conductivity normal metal. The whole question of stability will be discussed in the next section. 430 Y. I WAS A AND D. B. MONTGOMERY b.
Applied Superconductivity. Volume II by Vernon L. Newhouse