The correlative potential function and a new method for solving Maxwell equations

1984 
This paper is a continuation of Paper [1]. 1. A new potential ψ which is defined as the correlative potential is developed in this paper. The potential ψ is different from the classical scalar potential ϕ and the vector potential\(A\) developed by Helmholtz. The new formulae of the solution of eqs.\(\nabla \times \mathop f\limits^ \to = \mathop \infty \limits^ \to .\nabla \cdot \mathop f\limits^ \to = p\) are given in terms of ψ. 2. In the time-varying electromagnetic field, two new retarded potentials, the electric type retarded correlative potential ψe and the magnetic type retarded correlative potential ψe, which are distinct from the classical retarded potentials\(A\) and ϕ, are used to solve Maxwell equations. The new formulae of solution of Maxwell equation are given in terms of ψe and ψm. 3. The methods for constructing a rotational field with given curl function (vorticity) is proposed.
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