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**Hint:**The Coulombic force of attraction or repulsion between 2 charges depends upon the medium. If the medium is a dielectric, that has some polarisable properties then it cancels some of the permittivity of electric field lines through the medium. To account for this the Columba’s law equation is modified and a relative permittivity term is added for the dielectric. The modified Coulomb’s Law equation is given below.

**Formula used:**

\[F=\dfrac{{{q}_{1}}{{q}_{2}}}{4\pi {{\epsilon }_{0}}{{\epsilon }_{r}}{{r}^{2}}}\]

**Complete answer:**

The Coulombic force of attraction or repulsion between 2 charges depends upon the medium. If the medium is polarisable then the charges polarise the medium itself and that polarised medium then counters some of the force of attraction or repulsion between the charges. And thus cancels some of the permittivity of electric field lines through the medium. Thus in a dielectric medium a relative permittivity term is used to account for this effect and thus a modified Coulomb’s equation is used. In a medium of relative permittivity \[{{\epsilon }_{r}}\] the force of attraction between charges \[{{q}_{1}}\] and \[{{q}_{2}}\] separated by a distance r is given as

\[F=\dfrac{{{q}_{1}}{{q}_{2}}}{4\pi {{\epsilon }_{0}}{{\epsilon }_{r}}{{r}^{2}}}\]

Now coming to our question, Let's start by listing the known values

\[{{q}_{1}}={{q}_{2}}=20\times {{10}^{-6}}C\]

\[\begin{align}

& {{\epsilon }_{r}}=4 \\

& r=40cm \\

& \Rightarrow r=0.4m \\

\end{align}\]

Plugging in the given values in the equation we get

\[F=\dfrac{{{q}_{1}}{{q}_{2}}}{4\pi {{\epsilon }_{0}}{{\epsilon }_{r}}{{r}^{2}}}\]

\[\Rightarrow F=\dfrac{1}{4\pi {{\epsilon }_{0}}{{\epsilon }_{r}}}\times \dfrac{(20\times {{10}^{-6}})(20\times {{10}^{-6}})}{{{(0.4)}^{2}}}\]

We also know that

\[\dfrac{1}{4\pi {{\epsilon }_{0}}}=9\times {{10}^{9}}\]

Thus,

\[\begin{align}

& F=\dfrac{1}{4\pi {{\epsilon }_{0}}{{\epsilon }_{r}}}\times \dfrac{(20\times {{10}^{-6}})(20\times {{10}^{-6}})}{{{(0.4)}^{2}}} \\

& \Rightarrow F=\dfrac{9\times {{10}^{9}}}{4}\times \dfrac{400\times {{10}^{-12}}}{16\times {{10}^{-2}}} \\

& \Rightarrow F=\dfrac{9\times 4\times {{10}^{4}}\times {{10}^{-12}}\times {{10}^{9}}}{4\times 16} \\

& \Rightarrow F=5.625N \\

\end{align}\]

So, the force acting between the two charges will be \[5.625N\]

**Note:**

The \[{{\epsilon }_{0}}\] used the Coulomb’s Law formula \[F=\dfrac{1}{4\pi {{\epsilon }_{0}}}\times \dfrac{{{q}_{1}}\times {{q}_{2}}}{{{r}^{2}}}\] is called the permittivity of free space. It is basically the capability of a vacuum to permit electric field lines within it. This permittivity changes with the medium thus the \[{{\epsilon }_{r}}\] term is used for relative permittivity through a dielectric. It is called the dielectric constant or relative permittivity and it reduces the force acting between the charges.

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