A dielectric object is placed in an electric field. The object becomes polarised and
a large number of atomic/molecular dipoles in the object align in the direction of
the applied electric field. Derive an expression for the electric potential due to this
polarised dielectric at a point outside the dielectric.
"\\Delta\\varphi=\\frac 1{4\\pi\\varepsilon_0}\\frac{q^--q^+}{r_x^2+r_y^2}."
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