Stamopoulos Dimosthenis
Department of Physics, School of Science, National and Kapodistrian University of Athens, Zografou Panepistimioupolis, 15784 Athens, Greece.
Materials (Basel). 2025 May 17;18(10):2344. doi: 10.3390/ma18102344.
The multipole expansion on the basis of Spherical Harmonics is a multifaceted mathematical tool utilized in many disciplines of science and engineering. Regarding physics, in electromagnetism, the multipole expansion is exclusively focused on the scalar potential, Ur, defined only in the so-called inside, Uinr, and outside, Uoutr, spaces, separated by the middle space wherein the source resides, for both dielectric and magnetic materials. Intriguingly, though the middle space probably encloses more physics than the inside and outside spaces, it is never assessed in the literature, probably due to the rather complicated mathematics. Here, we investigate the middle space and introduce the multipole expansion of the scalar potential, Umidr, in this, until now, unsurveyed area. This is achieved through the complementary superposition of the solutions of the inside, Uinr, and outside, Uoutr, spaces when carefully adjusted at the interface of two appropriately defined subspaces of the middle space. Importantly, while the multipole expansion of Uinr and Uoutr satisfies the Laplace equation, the expression of the middle space, Umidr, introduced here satisfies the Poisson equation, as it should. Interestingly, this is mathematically proved by using the method of variation of parameters, which allows us to switch between the solution of the homogeneous Laplace equation to that of the nonhomogeneous Poisson one, thus completely bypassing the standard method in which the multipole expansion of |r-r'|-1 is used in the generalized law of Coulomb. Due to this characteristic, the notion of Umidr introduced here can be utilized on a general basis for the effective calculation of the scalar potential in spaces wherein sources reside. The proof of concept is documented for representative cases found in the literature. Though here we deal with the static and quasi-static limit of low frequencies, our concept can be easily developed to the fully dynamic case. At all instances, the exact mathematical modeling of Umidr introduced here can be very useful in applications of both homogeneous and nonhomogeneous, dielectric and magnetic materials.
基于球谐函数的多极展开是一种多方面的数学工具,在许多科学和工程学科中都有应用。在物理学方面,在电磁学中,多极展开专门关注标量势(U_r),它仅在所谓的内部空间(U_{in}(r))和外部空间(U_{out}(r))中定义,这两个空间由源所在的中间空间分隔开,适用于电介质和磁性材料。有趣的是,尽管中间空间可能包含比内部和外部空间更多的物理内容,但在文献中从未对其进行评估,这可能是由于数学相当复杂。在这里,我们研究中间空间,并在此之前未被研究的领域引入标量势(U_{mid}(r))的多极展开。这是通过在中间空间的两个适当定义的子空间的界面处仔细调整时,将内部空间(U_{in}(r))和外部空间(U_{out}(r))的解进行互补叠加来实现的。重要的是,虽然(U_{in}(r))和(U_{out}(r))的多极展开满足拉普拉斯方程,但这里引入的中间空间的表达式(U_{mid}(r))满足泊松方程,这是它应有的。有趣的是,这是通过使用参数变分法在数学上证明的,这使我们能够在齐次拉普拉斯方程的解和非齐次泊松方程的解之间切换,从而完全绕过在库仑广义定律中使用(\vert\vec{r}-\vec{r}'\vert^{-1})的多极展开的标准方法。由于这一特性,这里引入的(U_{mid}(r))的概念可以在一般基础上用于有效计算源所在空间中的标量势。针对文献中发现的代表性案例记录了概念验证。尽管这里我们处理的是低频的静态和准静态极限,但我们的概念可以很容易地扩展到完全动态的情况。在所有情况下,这里引入的(U_{mid}(r))的精确数学建模在均匀和非均匀、电介质和磁性材料的应用中都可能非常有用。