Let the point charge be Q. Next, we may put a charge q to the point with distance r from Q. Therefore, the electric force will be
"F=k\\cdot\\dfrac{Qq} {r^2} ." Here k is a constant equal to "9\\cdot10^9\\mathrm{Nm^2\/C^2}."
The modulus of the electric field is
"E=\\dfrac{F} {q} =k\\cdot \\dfrac{Q} {r^2}"
The direction of the field is towards the vector from Q if it is positive and to Q if it is negative.
So we may rewrite it as
"\\vec{E} =k\\cdot\\dfrac{Q} {r^3} \\cdot\\vec{r}."
In case of non-vacuum, we should add a factor "\\varepsilon"
"\\vec{E} =k\\cdot\\dfrac{Q} {\\varepsilon r^3} \\cdot\\vec{r}."
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