Electric field strength in point A
"E=\\frac{q}{4\\pi \\epsilon_0}\\left(\\frac{1}{r_2^2}-\\frac{1}{r_1^2}\\right)"We may apply the mean value theorem
"E=\\frac{q}{4\\pi \\epsilon_0}\\frac{d}{dr} \\left(\\frac{1}{r^2} \\right) \\bigg|_{r=\\xi}(r_2-r_1)=\\frac{1}{4\\pi \\epsilon_0}\\frac{2p}{\\xi^3}"where
"\\xi \\in [r_2,r_1]"Dipole is a point particle, hence
"\\xi=r"where r is a distance between dipole and point A.
So the electric field strength due to dipole of moment p at a distant point r along the axis of the dipole is
"E=\\frac{1}{4\\pi \\epsilon_0}\\frac{2p}{r^3}"or in vector form
"\\vec E=\\frac{1}{4\\pi \\epsilon_0}\\frac{2\\vec p}{r^3}"
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