I. Introduction
Superconducting cable terminals are the important part of high temperature superconducting (HTS) cable system, in which the stress cone connects the superconducting conductor and current lead. Nonuniform electric field is one of the key issues for the stress cone of superconducting cable terminals, which leads to the partial discharge, accelerates the insulation degradation and even failure [1], [2]. More importantly, it is unavoidable to experience transient overvoltage caused by the switch of thyristors and the polarity reversal in HVDC converters, which aggravates the concentration of local electric field in terminal insulation [3], [4]. It is infeasible to uniform electric field in stress cone simply by designing its structure in cable terminals, due to the resistance-dependent field distribution in polymeric insulation, which is completely different from the capacity-dependence under ac field [5].