Four-Vector Potential for Point Charge Moving Arbitrarily in Cylindrical Drift Tube

Author(s):  
K. Ilyenko ◽  
G. Gorbik
2015 ◽  
Vol 66 (6) ◽  
pp. 317-322
Author(s):  
L’ubomír Šumichrast

Abstract Scalar and vector potential as well as the electromagnetic field of a moving point charge is a nice example how the application of symbolic functions (distributions) in electromagnetics makes it easier to obtain and interpret solutions of otherwise hardly solvable problems.


The following paper is occupied by an attempt to investigate the distribution of the electric and magnetic forces which are called into play when certain electro­magnetic systems are made to move with uniform velocity through the ether. Maxwell’s theory will be employed throughout, and will be applied to th e exact solution of several problems, and to the establishment of some results of a general nature. Professor J. J. Thomson was, I believe, the first to consider a problem of this sort, his paper giving the solution for the motion of a single electrical point-charge at a speed small compared with that of light. Mr. Oliver Heaviside next considered the question, and in his paper obtained an exact solution for the motion of a point-charge. He got the solution by means of the “vector potential” of the convection current formed by the moving charge. The mathematical analysis is of the symbolical kind, but it is shown that the result obtained by means of it satisfies all the necessary conditions. By integrations Mr. Heaviside obtains solutions for the motion of some simple cases of electrical distribution.


Author(s):  
J. Pierrus

This chapter expresses the fields E ( r, t) and B ( r, t) in terms of the electromagnetic potentials Ф( r, t) and A ( r, t), and shows that these potentials are defined only up to a gauge transformation. This leads the reader naturally to the Coulomb and Lorenz gauges which are usually encountered in textbooks. The inhomogeneous wave equations whose solutions are the retarded electromagnetic potentials are also considered, as well as the Lienard–Wiechert potentials for an arbitrarily moving point charge. A few questions are included in which the Lagrangian and Hamiltonian of a point charge are expressed in terms of Ф and A. The chapter concludes by deriving a multipole expansion for the dynamic vector potential which will provide the starting point in our treatment of electromagnetic radiation later on in Chapter 11


2018 ◽  
Vol 69 (3) ◽  
pp. 259-260
Author(s):  
L’ubomír Šumichrast ◽  
Rastislav Dosoudil

Abstract In the recently published short paper author deals with the derivation of the scalar potential pertaining to the point charge as well as of the vector potential pertaining to the point current. He shows his alternative approach and compares it to the ”traditional” methods commonly used in textbooks. Here we want to show that use of the generalised functions (symbolic functions, distributions) in the domain of electromagnetic field theory provides more straightforward and more rigorous approach to the problem.


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