1919
DOI: 10.1080/14786440808635943
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XVII. Notes on electric and magnetic field constants and their expression in terms of Bessel functions and elliptic integrals

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“…By substituting (B 2) and (B 4) into (5.17a) and (5.17 6), respectively, the results are The functions J m and J are Bessel functions of the respectively. The integrals in (5.19) are the L ip sch itz-H an k el ty p e involving products of Bessel functions (Gary 1919), and th eir properties have been considered in detail by E ason et al (1955), Salam on & D undurs (1971), and Salam on & W alter (1979. F or isotropic solids, the result (5.18a) and (5.186) are the same as those obtained by Yu & Sanday 1991 d).…”
Section: (D) Circular 'Prismatic Dislocation Loops With Burgers Vector Perpendicular To the Interfacementioning
confidence: 99%
“…By substituting (B 2) and (B 4) into (5.17a) and (5.17 6), respectively, the results are The functions J m and J are Bessel functions of the respectively. The integrals in (5.19) are the L ip sch itz-H an k el ty p e involving products of Bessel functions (Gary 1919), and th eir properties have been considered in detail by E ason et al (1955), Salam on & D undurs (1971), and Salam on & W alter (1979. F or isotropic solids, the result (5.18a) and (5.186) are the same as those obtained by Yu & Sanday 1991 d).…”
Section: (D) Circular 'Prismatic Dislocation Loops With Burgers Vector Perpendicular To the Interfacementioning
confidence: 99%