The electrostatic potential energy "U_E" of one point charge "q" at position "r" in the presence of an electric field "E" is defined as the negative of the work "W" done by the electrostatic force to bring it from the reference position "r_{ref}" to that position "r":
"U_E(r)=-W_{r_{ref}\\to r}=-\\int q E(r')dr'" .
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