Gauge symmetry is closely related to charge conservation. Suppose that there existed some process by which one could briefly violate conservation of charge by creating a charge "q" at a certain point in space, 1, moving it to some other point 2, and then destroying it. We might imagine that this process was consistent with conservation of energy. We could posit a rule stating that creating the charge required an input of energy "E"1="qV"1 and destroying it released "E"2="qV"2, which would seem natural since "qV" measures the extra energy stored in the electric field because of the existence of a charge at a certain point. Outside of the interval during which the particle exists, conservation of energy would be satisfied, because the net energy released by creation and destruction of the particle, "qV"2-"qV"1, would be equal to the work done in moving the particle from 1 to 2, "qV"2-"qV"1. But although this scenario salvages conservation of energy, it violates gauge symmetry. Gauge symmetry requires that the laws of physics be invariant under the transformation formula_2, which implies that no experiment should be able to measure the absolute potential, without reference to some external standard such as an electrical ground. But the proposed rules "E"1="qV"1 and "E"2="qV"2 for the energies of creation and destruction "would" allow an experimenter to determine the absolute potential, simply by comparing the energy input required to create the charge "q" at a particular point in space in the case where the potential is formula_1 and formula_5 respectively. The conclusion is that if gauge symmetry holds, and energy is conserved, then charge must be conserved.