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Electrostatics question

2025 · 23 Jan · Shift 1 · Q52
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  5. /2025 · 23 Jan · Shift 1 · Q52

Electrostatics question

2025 · 23 Jan · Shift 1 · Q52

JEE MainPhysicsElectrostaticsMCQ+4 / −1
A point particle of charge QQQ is located at PPP along the axis of an electric dipole 1 at a distance rrr as shown in the figure. The point P is also on the equatorial plane of a second electric dipole 2 at a distance r. The dipoles are made of opposite charge q separated by a distance 2a2 a2a. For the charge particle at P not to experience any net force, which of the following correctly describes the situation? JEE Main 2025 (Online) 23rd January Morning Shift Physics - Electrostatics Question 28 English
  1. A
    ar∼0.5\frac{a}{r} \sim 0.5ra​∼0.5
  2. B
    ar∼3\frac{a}{r} \sim 3ra​∼3
  3. C
    ar∼10\frac{a}{r} \sim 10ra​∼10
  4. D
    ar∼20\frac{a}{r} \sim 20ra​∼20
View written solutionFree

Correct answer: B

  1. Field needed for zero force on charge QQQ

For the point charge QQQ at PPP to experience no net force, the net electric field at PPP must be zero:

F⃗=QE⃗net=0⇒E⃗net=0\vec F = Q\vec E_{\text{net}} = 0 \quad \Rightarrow \quad \vec E_{\text{net}}=0F=QEnet​=0⇒Enet​=0

So the field due to dipole 1 and dipole 2 at PPP must be equal in magnitude and opposite in direction.


  1. Electric field due to dipole 1 on its axial line

For a dipole made of charges ±q\pm q±q separated by distance 2a2a2a, the dipole moment magnitude is

p=q(2a)=2aqp = q(2a)=2aqp=q(2a)=2aq

At a point on the axis at distance rrr from the center, the exact electric field magnitude is

Eaxial=14πε0[q(r−a)2−q(r+a)2]E_{\text{axial}} = \frac{1}{4\pi\varepsilon_0}\left[\frac{q}{(r-a)^2}-\frac{q}{(r+a)^2}\right]Eaxial​=4πε0​1​[(r−a)2q​−(r+a)2q​]

Simplify:

Eaxial=14πε0q (r+a)2−(r−a)2(r2−a2)2E_{\text{axial}} = \frac{1}{4\pi\varepsilon_0}q\,\frac{(r+a)^2-(r-a)^2}{(r^2-a^2)^2}Eaxial​=4πε0​1​q(r2−a2)2(r+a)2−(r−a)2​ (r+a)2−(r−a)2=4ar(r+a)^2-(r-a)^2 = 4ar(r+a)2−(r−a)2=4ar

Hence,

Eaxial=14πε04aqr(r2−a2)2E_{\text{axial}} = \frac{1}{4\pi\varepsilon_0}\frac{4aqr}{(r^2-a^2)^2}Eaxial​=4πε0​1​(r2−a2)24aqr​
  1. Electric field due to dipole 2 on its equatorial line

At a point on the equatorial plane at distance rrr from the center, the exact field magnitude is

Eequatorial=14πε02aq(r2+a2)3/2E_{\text{equatorial}} = \frac{1}{4\pi\varepsilon_0}\frac{2aq}{(r^2+a^2)^{3/2}}Eequatorial​=4πε0​1​(r2+a2)3/22aq​

(Direction is opposite to dipole moment; we only need magnitude here.)


  1. Condition for zero net field

Since the two fields must cancel,

Eaxial=EequatorialE_{\text{axial}} = E_{\text{equatorial}}Eaxial​=Eequatorial​

So,

14πε04aqr(r2−a2)2=14πε02aq(r2+a2)3/2\frac{1}{4\pi\varepsilon_0}\frac{4aqr}{(r^2-a^2)^2} = \frac{1}{4\pi\varepsilon_0}\frac{2aq}{(r^2+a^2)^{3/2}}4πε0​1​(r2−a2)24aqr​=4πε0​1​(r2+a2)3/22aq​

Cancel common factors 14πε0\dfrac{1}{4\pi\varepsilon_0}4πε0​1​ and 2aq2aq2aq:

2r(r2−a2)2=1(r2+a2)3/2\frac{2r}{(r^2-a^2)^2} = \frac{1}{(r^2+a^2)^{3/2}}(r2−a2)22r​=(r2+a2)3/21​

Rearrange:

2r(r2+a2)3/2=(r2−a2)22r(r^2+a^2)^{3/2} = (r^2-a^2)^22r(r2+a2)3/2=(r2−a2)2
  1. Introduce the ratio x=arx=\dfrac{a}{r}x=ra​

Let

x=arx=\frac{a}{r}x=ra​

Then a=xra=xra=xr. Substitute into the equation:

2r(r2+a2)3/2=(r2−a2)22r\left(r^2+a^2\right)^{3/2} = (r^2-a^2)^22r(r2+a2)3/2=(r2−a2)2 2r(r2(1+x2))3/2=(r2(1−x2))22r\left(r^2(1+x^2)\right)^{3/2} = \left(r^2(1-x^2)\right)^22r(r2(1+x2))3/2=(r2(1−x2))2 2r⋅r3(1+x2)3/2=r4(1−x2)22r\cdot r^3(1+x^2)^{3/2} = r^4(1-x^2)^22r⋅r3(1+x2)3/2=r4(1−x2)2 2(1+x2)3/2=(1−x2)22(1+x^2)^{3/2} = (1-x^2)^22(1+x2)3/2=(1−x2)2

We now test the options.


  1. Check the options

Option A: x=0.5x=0.5x=0.5

LHS=2(1+0.25)3/2=2(1.25)3/2≈2(1.397)≈2.79\text{LHS} = 2(1+0.25)^{3/2}=2(1.25)^{3/2}\approx 2(1.397)\approx 2.79LHS=2(1+0.25)3/2=2(1.25)3/2≈2(1.397)≈2.79 RHS=(1−0.25)2=(0.75)2=0.5625\text{RHS}=(1-0.25)^2=(0.75)^2=0.5625RHS=(1−0.25)2=(0.75)2=0.5625

Not equal.

Option B: x=3x=3x=3

LHS=2(1+9)3/2=2(10)3/2=2⋅1010≈63.2\text{LHS}=2(1+9)^{3/2}=2(10)^{3/2}=2\cdot 10\sqrt{10}\approx 63.2LHS=2(1+9)3/2=2(10)3/2=2⋅1010​≈63.2 RHS=(1−9)2=64\text{RHS}=(1-9)^2=64RHS=(1−9)2=64

These are very close.

Option C: x=10x=10x=10

LHS=2(101)3/2≈2⋅101⋅101≫1000\text{LHS}=2(101)^{3/2}\approx 2\cdot 101\cdot \sqrt{101} \gg 1000LHS=2(101)3/2≈2⋅101⋅101​≫1000 RHS=(1−100)2=992=9801\text{RHS}=(1-100)^2=99^2=9801RHS=(1−100)2=992=9801

Not close.

Option D: x=20x=20x=20

Again, values are not close enough compared with option B.


  1. Conclusion

The condition is satisfied approximately for

ar≈3\frac{a}{r} \approx 3ra​≈3

So the correct option is B.


  1. Comparison with stored answer

Stored correct answer: B

Our derived answer: B

They agree.

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