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QJEEAdv08Phca36: JEE Advanced 2008 Physics - Class 12 JEEAdv08Phca36 Solution: Consider a system of three charges and placed at points A, B…

Consider a system of three charges q3,q3{q \over 3},{q \over 3} and −2q3- {{2q} \over 3} placed at points A, B and C, respectively, as shown in the figure. Take O to be the centre of the circle of radius R and angle CAB = 60 ∘^\circ

IIT-JEE 2008 Paper 2 Offline Physics - Electrostatics Question 10 English

Multiple Choice Options

  • A The electric field at point O is q8πε0R2{q \over {8\pi {\varepsilon _0}{R^2}}} directed along the negative x-axis
  • B The potential energy of the system is zero
  • C The magnitude of the force between the charges at C and B is q254πε0R2{{{q^2}} \over {54\pi {\varepsilon _0}{R^2}}}
  • D The potential at point O is q12πε0R{q \over {12\pi {\varepsilon _0}R}}

Step-by-Step Verified Solution

Electric field at point O is vector sum of electric field due to all three point charges individually.

IIT-JEE 2008 Paper 2 Offline Physics - Electrostatics Question 10 English Explanation

E→=EA→+EB→+EC→\overrightarrow E = \overrightarrow {{E_A}} + \overrightarrow {{E_B}} + \overrightarrow {{E_C}} and EA→=−EB→\overrightarrow {{E_A}} = - \overrightarrow {{E_B}}

So, E→=EC→=2q/34πε0.R2\overrightarrow E = \overrightarrow {{E_C}} = {{2q/3} \over {4\pi {\varepsilon _0}.{R^2}}} along OC→\overrightarrow {OC}

=q6πε02.R2= {q \over {6\pi \varepsilon _0^2.{R^2}}} along OC→\overrightarrow {OC}

=+q′6πε02.R2i^= {{ + q'} \over {6\pi \varepsilon _0^2.{R^2}}}\widehat i

=−q′6πε0.R2j^= {{ - q'} \over {6\pi \varepsilon _0.{R^2}}}\widehat j

From geometry, we can find that ∠\angle ABC = 30 ∘^\circ and ∠\angle ACB = 90 ∘^\circ

So, AB = 2R, AC = R, BC = 3\sqrt3 R

Total potential energy of the system is,

U=14πε0[q/3×q/32R−q/3×2q/3R−q/3×2q/33R]≠0U = {1 \over {4\pi {\varepsilon _0}}}\left[ {{{q/3 \times q/3} \over {2R}} - {{q/3 \times 2q/3} \over R} - {{q/3 \times 2q/3} \over {\sqrt 3 R}}} \right] \ne 0

F=q/3×q/34πε0×(3R)2=q254πε0R2F = {{q/3 \times q/3} \over {4\pi {\varepsilon _0} \times {{(\sqrt 3 R)}^2}}} = {{{q^2}} \over {54\pi {\varepsilon _0}{R^2}}}

Potential at point O is,

V=q/3×q/3−2q/34πε0R=0V = {{q/3 \times q/3 - 2q/3} \over {4\pi {\varepsilon _0}R}} = 0

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