推廣的赫姆霍茲定理及其在電磁理論中的應(yīng)用
EXTENDED HELMHOLTZ THEOREM AND ITS APPLICATION IN ELECTROMAGNETIC THEORY
-
摘要: 本文證明了在直角、畫柱和球坐標(biāo)系的規(guī)則邊界的系統(tǒng)內(nèi),一個(gè)任意的矢量一定可以分解為無(wú)旋場(chǎng)、橫電模場(chǎng)和橫磁模場(chǎng)三個(gè)相互正交的分量,每一個(gè)分量都可用一個(gè)標(biāo)量函數(shù)來(lái)描述。并在此基礎(chǔ)上證明了這些系統(tǒng)內(nèi)的{L、M和N}矢量波函數(shù)系的完備性。由此說(shuō)明了一個(gè)矢量函數(shù)空間不僅可以通過(guò)它在歐氏空間中的射影分解為三個(gè)不相交的子空間,同樣可以通過(guò)它在矢量波函數(shù)系上的射影分解為三個(gè)不相交的子空間。
-
關(guān)鍵詞:
- 電磁理論; 赫姆霍茲定理; 無(wú)旋場(chǎng)
Abstract: It is proved that in a regular boundary system of rectangular, cylindrical or spherical coordinate, an arbrtrary Vector function can be separated into three orthogonal parts: TE mode field, TM mode field and irro tational field. Each of these components can be determined fully by a scalas function. On the basis of this theorem, the compltenesa of vector wave function system {L, M, and N} is proved, also. Thus it is explained that a vector furction space can be proiected into three uncrossed subspaces not only in Euclidean space but also in the subspace of vector wave function space. -
P. M. Morse, F. Feshback, Math. of Theoretical Phys., Pt. I, McGraw-Hill Book Company,New York.(1953).[2]宋文森,微波,1986年,第3期,第23-28頁(yè).[3]林為干,微波理論和技術(shù),科學(xué)出版社,(1979), p.671.[4]Wang Jianying, Song Wenmiao, Helmholtz's Theorem and Expansions of Eigentunctions of EM Field in Resonant Cavity, APMC88, The Second Asia-Pacitic Microwave Conference, Beijing,(1988), p. 85.[5]J. D.杰克遜著,朱培予譯,經(jīng)典電動(dòng)力學(xué),上冊(cè),人民教育出版社,(1980),p.244.[6]O. L. Brill, H. Grodman, Am. J. Phys., 35(1967), 832.[7]宋文森,電子科學(xué)學(xué)刊,8(1986)3, 188-195.[8]K. Kurokawa, IRE Trans. on MTT, MTT-6 (1958), 178-187.[9]龔書喜,電磁理論中廣義本征函數(shù)展開(kāi)間題,西安交通大學(xué)博士論文,1987年.[10]宋文森,微波學(xué)報(bào),1989年,第3期,第21-28頁(yè).[11]R. E. Collin, Rodio Science, 21(1986), 883-890.[12]宋文森,王建英,電子科學(xué)學(xué)刊, 11(1989)5, 518-527. -
計(jì)量
- 文章訪問(wèn)數(shù): 2418
- HTML全文瀏覽量: 137
- PDF下載量: 633
- 被引次數(shù): 0