What will be the electric field intensity at the point P due to a short dipole if the dipole is placed in air or vaccum?

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  1. \(\frac{1}{{4\pi {\varepsilon _0}}}\frac{{2p}}{{{r^2}}}\)
  2. \(\frac{1}{{4\pi {\varepsilon _0K}}}\frac{{2p}}{{{r^2}}}\)
  3. \(\frac{1}{{4\pi {\varepsilon _0}}}\frac{{2p}}{{{r^3}}}\)
  4. \(\frac{1}{{4\pi {\varepsilon _0K}}}\frac{{2p}}{{{r^3}}}\)

Answer (Detailed Solution Below)

Option 3 : \(\frac{1}{{4\pi {\varepsilon _0}}}\frac{{2p}}{{{r^3}}}\)
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Detailed Solution

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Given:

A short dipole in air or vacuum

Concept:

An electric dipole is is a system of two-point charges of equal and opposite magnitude placed at a short distance.

Formula:

For a dipole, dipole moment,

p = q(2l)

Calculations:

F2 Savita Engineering 28-6-22 D2

E(+q) = \(\frac{q}{4\pi \epsilon 0(r-l)^2}\) towards BP

E(-q) = \(\frac{q}{4\pi \epsilon 0(r+l)^2}\) towards PA

E = E(+q) - E(-q)

⇒ E = \(\frac{q}{4\pi \epsilon 0(r-l)^2} -\frac{q}{4\pi \epsilon 0(r+l)^2}\)

⇒ E = \(\frac{4qlr}{4\pi \epsilon 0(r^2-l^2)^2}\)

⇒ E = \(\frac{2q(2l)r}{4\pi \epsilon 0(r^2-l^2)^2}\)

But q(2l) = p and for a short dipole r- l2 ≈ r2 as l << r

⇒ E = \(\frac{2pr}{4\pi \epsilon 0r^4}\)

⇒ E\(\frac{2p}{4\pi \epsilon 0r^3}\)

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