In this section, we consider a dipole composed of charges +q and -q, placed within a uniform electric field E. While the dipole does not experience a net force, it does experience a torque given by t = p × E, attempting to align the dipole with the electric field. An external torque can be applied to counter this effect, allowing us to calculate the work done, expressed by the formula W = pE (cos θ - cos θ0). This work accumulates as potential energy U(q), where a natural zero reference is chosen at an inclination of θ0 = π/2. Additionally, potential energy can be explored from the perspective of each charge’s location in the electric field. A practical example illustrates how changing the electric field's direction affects the energy dynamics of a substance's dipoles.