Diffraction of a Dipole Field by a Perfectly Conducting Half Plane
dc.contributor.author | Bowman, J. J. | en_US |
dc.contributor.author | Senior, T. B. A. | en_US |
dc.date.accessioned | 2015-12-03T15:04:12Z | |
dc.date.available | 2015-12-03T15:04:12Z | |
dc.date.issued | 1967-11 | en_US |
dc.identifier.citation | Bowman, J. J.; Senior, T. B. A. (1967). "Diffraction of a Dipole Field by a Perfectly Conducting Half Plane." Radio Science 2(11): 1339-1345. | en_US |
dc.identifier.issn | 0048-6604 | en_US |
dc.identifier.issn | 1944-799X | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/116080 | |
dc.publisher | The Macmillan Co. | en_US |
dc.publisher | Wiley Periodicals, Inc. | en_US |
dc.title | Diffraction of a Dipole Field by a Perfectly Conducting Half Plane | en_US |
dc.type | Article | en_US |
dc.rights.robots | IndexNoFollow | en_US |
dc.subject.hlbsecondlevel | Electrical Engineering | en_US |
dc.subject.hlbtoplevel | Engineering | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Radiation Laboratory, Department of Electrical Engineering, University of Michigan, Ann Arbor, Mich. 48108, U.S.A. | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/116080/1/rds19672111339.pdf | |
dc.identifier.doi | 10.1002/rds19672111339 | en_US |
dc.identifier.source | Radio Science | en_US |
dc.identifier.citedreference | Bromwich, T. J. I'A. ( 1915 ), Diffraction of waves by a wedge, Proc. London Math. Soc. 14, 450 – 463. | en_US |
dc.identifier.citedreference | Carslaw, H. S. ( 1899 ), Some multiform solutions of the partial differential equations of physical mathematics and their applications, Proc. London Math. Soc. 30, 121 – 161. | en_US |
dc.identifier.citedreference | Felsen, L. B. ( 1957 ), Alternative field representations in regions bounded by spheres, cones and planes, IRE Trans. Ant. Prop. AP‐ 5, No. 1, 109 – 121. Note that in eq (54) the componets and must be evaluated at the source point. | en_US |
dc.identifier.citedreference | Jones, D. S. ( 1964 ), The Theory of Electromagnetism ( The Macmillan Co., New York, N.Y. ). The scalar point‐source solutions on pp. 592 and 593 are in error by a factor k. This error carries over to the dipole solutions on p. 594. The “additional” terms in the expression for B are also in error by a factor 4π. | en_US |
dc.identifier.citedreference | Macdonald, H. M. ( 1915 ), A class of diffraction problems, Proc. London Math. Soc. 14, 410 ‐ 427. | en_US |
dc.identifier.citedreference | Malyuzhinets, G. D., and A. A. Tuzhilin ( 1963 ), The electromagnetic field excited by an electric dipole in a wedge‐shaped region, Soviet Phys. Doklady 7, No. 10, 879–882. English translation of Dokl. Akad. Nauk SSSR 146, No. 5, 1039 – 1042 (1962).In eq (8), replace − 2Ψ by 2Ψ. | en_US |
dc.identifier.citedreference | Senior, T. B. A. ( 1953 ), The diffraction of a dipole field by a perfectly conducting half plane, Quart. J. Mech. Appl. Math. 6, 101 – 114. | en_US |
dc.identifier.citedreference | Stratton, J. A. ( 1941 ), Electromagnetic Theory ( McGraw‐Hill Book Co., Inc., New York, N.Y. ). | en_US |
dc.identifier.citedreference | Tai, C. T. ( 1954 ), Radiation from current elements and apertures in the presence of a perfectly conducting half‐plane sheet, Stanford Univ. Res. Inst. Tech. Rept. No. 45, Stanford Univ., Stanford, Calif. | en_US |
dc.identifier.citedreference | Tilston, W. V. (Oct. 1952 ), Contributions to the theory of antennas, Tech. Rept., Antenna Lab., Dept. Elec. Eng., Univ. of Toronto, Toronto, Ontario. Due to normalization errors in both the θ and ϕ integrations, a factor 2π/ ϕ 0 is omitted and should bereplaced by throughout. Further, mB sin. should read whenever it appears (pp. 32,33, 37). On the same pages replace C by − C and on pp. 36, 37 replace A, B, C, by −A, −B, −C, respectively. In eq (3.48),multiply the right‐hand side by −1, and in eq (3.59) divide the summand by n !. | en_US |
dc.identifier.citedreference | Tuzhilin, A. A. ( 1964 ), Short‐wave asymptotic representation of electromagnetic diffraction fields produced by arbitrarilyoriented dipoles in a wedge‐shaped region with ideally conducting sides, Annotation of reports of Third All‐Union Symp. on Wave Diffraction, Acad. Sci. USSR, 93‐95 (in Russian). In the line following eq (8), replace ϕ by θ. The integral in eq (10) should be multiplied by sgn ( β −4 n Φ). In eq (14) replace ϕ n by 4 n, and in the line following, the first should read. | en_US |
dc.identifier.citedreference | Williams, W. E. ( 1957 ), A note on the diffraction of a dipole field by a half plane, Quart. J. Mech. Appl. Math. 10, 210 – 213. | en_US |
dc.identifier.citedreference | Woods, B. D. ( 1957 ), The diffraction of a dipole field by a half plane, Quart. J. Mech. Appl. Math. 10, 90 – 100. | en_US |
dc.identifier.citedreference | The solutions given are correct if the scalar point sources are defined in terms of a Hertz potential ( kR ) −1 e −ikR, not R −1 e −ikR as indicated. | en_US |
dc.identifier.citedreference | Vandakurov, Y. V. ( 1954 ), Diffraction of electromagnetic waves by an arbitrarily‐oriented electric or magnetic dipole on a perfectly conducting half plane, Zh. Eksp. Teor. Fiz. 26, 3 − 18 (in Russian). | en_US |
dc.owningcollname | Interdisciplinary and Peer-Reviewed |
Files in this item
Remediation of Harmful Language
The University of Michigan Library aims to describe library materials in a way that respects the people and communities who create, use, and are represented in our collections. Report harmful or offensive language in catalog records, finding aids, or elsewhere in our collections anonymously through our metadata feedback form. More information at Remediation of Harmful Language.
Accessibility
If you are unable to use this file in its current format, please select the Contact Us link and we can modify it to make it more accessible to you.