In physics, the electric dipole moment (or electric dipole for short) is a measure of the polarity of a system of electric charges. In the simple case of two point charges, one with charge + q and one with charge − q, the electric dipole moment is: where r is the displacement vector pointing from the negative charge to the positive charge. This implies that the electric dipole moment vector More generally, for a system with an arbitrary number of point charges, the electric dipole moment is where each For a continuous distribution of charge, the corresponding expression is: where The dipole moment is most easily understood when the system has an overall neutral charge. For example, a pair of opposite charges, or a neutral conductor in a uniform electric field. For such systems, the value of the electric dipole moment is independent of the choice of reference point. When discussing the dipole moment of a non-neutral system, such as the dipole moment of the proton, a dependence on the choice of reference point arises. In such cases it is conventional to choose the reference point to be the center of mass of the system, not some arbitrary origin. This convention insures that the dipole moment is an intrinsic property of the system. See alsoExternal links
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