In electrodynamics, potentials are considered arbitrary because physical predictions rely on the gradient of the potential rather than the potential itself. This concept mirrors classical electrostatics, where the electric field, not the electric potential, is crucial for predictions. The vector potential A is also arbitrary, but it is not limited to just a scalar constant. However, the energy stored in the field, determined by the integral of the field strength, is not arbitrary. Understanding these distinctions is essential for grasping the nature of potentials in electrodynamics.