During the past decade, the electrically redox conducting polymers (CPs) have been delivering high capacitance and lower cyclic life due to their unique charge storage mechanism. Along with many advantages of CPs (their high conductivity, fast charge and discharge, and high specific capacitance), the main shortcoming of using them as the supercapacitor electrodes alone is that they are unstable over long cycle runs. Using CPs for long cycle runs during the redox reactions can not only lead to material loss but can also cause fractures or even breaking of the polymer chains during the reaction. Development of these flaws over a period can eventually breakdown the electrode.Polyaniline (PANI) is a special class of CPs that has been thoroughly examined as a good emerging supercapacitor electrode due to its large pseudo-capacitance and intrinsic redox states. [1] But as with CPs, during the process of charging/ discharging, PANI electrodes result in degradation leading to poor cycle life. [2] One solution of this inadequacy is to integrate PANI with any metal oxide material (TiO 2 , MnO 2 , NiO, Co 3 O 4 , and V 2 O 5 ) and/or carbon materials (activated carbon (AC), carbon nanotubes (CNTs), and graphene). It is seen that the electrochemical properties of PANI become more pronounced when PANI is combined with nanostructured TiO 2 (nTiO 2 ). [3] Carbon materials like AC have also established themselves as anode materials and have played crucial roles in the energy storage field because of their cost-effectiveness, high chemical stability, and good conductivity. [4] AC with high surface area has augmented electron transport efficiency that can transport ions, which are essential for preparing the carbon-based supercapacitors. On one hand, where carbon-based electrodes have excellent cycling stability but less energy density, CPs on the other hand have good conductivity but less stability. Also, nTiO 2 has already been verified as a promising candidate for