PulseExploreJournal ClubDebatesTrendingResearchersJournals
Instagram
HomeExploreJournal ClubTrending
Synapse
⌘+K
Synapse
April 22, 2026Materials0 citationsOpen Access

Dielectric and Magnetic Spherical Hollow Shells Subjected to a dc or Low-Frequency ac Field of Any Spatial Form: Complete Theoretical Survey of All Scalar and Vector Physical Entities, Including the Depolarization Effect

PMPetros MoraitisKTKosmas TsakmakidisNNNorbert M. Nemes

Key Points

  • This work aims to analyze the behaviors of dielectric and magnetic spherical hollow shells when subjected to external DC or AC electromagnetic fields.
  • Applied method-of-linear-recursive-solution (MLRS) to the Laplace equation.
  • Calculated internal and total potentials in relation to external potentials.
  • Derived scalar and vector physical entities, including depolarization factors and susceptibilities.
  • Identified two depolarization factors, Nl and Nl+1, which depend on degree l.
  • Demonstrated that Nl + Nl+1 = 1, maintaining mathematical consistency.
  • Provided a flexible analytical framework applicable to various dielectric and magnetic geometries.

Abstract

Dielectric and magnetic spherical hollow shells are employed in many applications as standard building units. These structures are commonly subjected to size reduction to obtain a high surface area/volume ratio, a property that is in favor of specific applications. However, the size reduction enhances the importance of physical mechanisms that originate from surfaces, such as the depolarization effect. Here we tackle the problem of dielectric and magnetic spherical hollow shells, consisting of a linear, homogeneous and isotropic parent material, subjected to an external potential, Uextr, of any spatial form (either dc (static) or ac of low-frequency (quasistatic limit)). By applying the method-of-linear-recursive-solution (MLRS) to the Laplace equation, we calculate analytically the internal, Uintr, and total, Utotr, potentials in respect to the external one, Uextr. From Uintr and Utotr we calculate all relevant scalar and vector physical entities of interest. The MLRS unveils straightforwardly the existence of two distinct depolarization factors, Nl=l/(2l+1) and Nl+1=(l+1)/(2l+1), both depending on the degree, l, however not on the order, m, of the mode of the external potential, Uext(l,m)r. These depolarization factors, Nl and Nl+1, originate from the outer, r=b, and inner, r=a, surfaces and are accompanied by two extrinsic susceptibilities, χe,lext=χe /(1+Nlχe ) and χe,l+1ext=χe /(1+Nl+1χe ), respectively. Importantly, Nl+Nl+1=1, irrespective of the degree, l, as it should. The properties of spherical hollow shells are investigated through analytical modeling and detailed simulations, with emphasis on application-relevant scenarios including resonance phenomena in scattering, quantitative materials characterization, and shielding/distortion. The generic MLRS strategy provides a flexible and reliable route for analyzing depolarization processes in other dielectric and magnetic building-unit geometries encountered in practice.

Ask AI
Helpful
Bookmark
Share
View Full Paper

Cite This Study

Moraitis et al. (2026) studied this question.

synapsesocial.com/papers/69e866ad6e0dea528ddeafb9https://doi.org/10.3390/ma19081638
Ask AI
Helpful
Bookmark
Share
View Full Paper