The aim of this study is to analyze the nonlinear stability of two viscoelastic electrified superimposed liquids immersed in porous media. Two limitless horizontal semi-infinite electrified fluids make up the present structure. The impacts of an unchanged oblique electric field (EF) and surface tension (ST) are applied. The increasing attraction of atmospheric and oceanic dynamics is fundamental to understanding this issue. The viscous potential flow (VPF) is employed to make mathematical usage easier. The concern mainly relies on combining the essential hydrodynamic equations with Maxwell's equations in an approximately quasi-static style. The linearized controlling equations are addressed to achieve the nonlinear expression under the appropriate boundary conditions (BCs). Subsequently, the influences of viscoelasticity are ignored, while solving the equations of motion. Therefore, the flat axis and the interface disturbance are interacting horizontally. The Rayleigh Helmholtz-Duffing oscillator (RHDO) describes how the two liquids in the interface spread out. He's frequency formula (HFF) converts the traditional nonlinear differential equation (NDE) into a linear one, which is analyzed through the non-perturbative approach (NPA). As shown through a non-dimensional analysis, there are diverse dimensionless physical numerals. Likewise well-known, the non-dimensional physical characteristics could be employed to investigate the fundamental aspects of a liquid structure. Additionally, they applied to degeneration the number of characteristics needed to understand the construction. A brief description of the NPA is likewise provided. The real/complex features of the NDEs are revealed via the stability research. According to the numerical simulations, the entire system is stabilized by different situations of the oblique EF versus the horizontal wavenumber. For both real and complex components, diverse sorts of polar plots are exhibited by graphs to elucidate the impacts of diverse elements and ensure the stability of the solutions. It should be noticed that all circumstances of the EFs are portrayed. It is observed that, when the EF is tangent to the interface, the Darcy and Bond numbers have a stabilized influence on the stability configuration. Supplementary, when the EF is normal to the interface, it is recognized that dynamic viscosity stabilizes the stability distribution. The density parameter has a destabilized effect on the stability zone. Finally, when the EF is inclined to the interface, it is observed that the Bond number and the viscoelastic parameter have a stabilizing influence on the stability region.