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Electrostatics question

2008 · Shift 2 · Q46
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Electrostatics question

2008 · Shift 2 · Q46

JEE AdvancedPhysicsElectrostaticsMCQ+3 / −1
Consider a system of three charges q3,q3{q \over 3},{q \over 3}3q​,3q​ and −2q3- {{2q} \over 3}−32q​ 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 15 English
  1. A
    The electric field at point O is q8πε0R2{q \over {8\pi {\varepsilon _0}{R^2}}}8πε0​R2q​ directed along the negative x-axis
  2. B
    The potential energy of the system is zero
  3. C
    The magnitude of the force between the charges at C and B is q254πε0R2{{{q^2}} \over {54\pi {\varepsilon _0}{R^2}}}54πε0​R2q2​
  4. D
    The potential at point O is q12πε0R{q \over {12\pi {\varepsilon _0}R}}12πε0​Rq​
View written solutionFree

Correct answer: C

Step-by-step Derivations:

1. Determine the Geometry of the System

  • The charges are placed at points A, B, and C on a circle of radius R with center O.
  • The problem states that the angle ∠CAB = 60°. This is an angle subtended by the arc CB at point A on the circumference.
  • The angle subtended by the same arc at the center, ∠COB, is twice the angle at the circumference. Therefore, ∠COB = 2 × ∠CAB = 2 × 60° = 120°.
  • Let's determine the distance between points B and C. In triangle OBC, OB = OC = R (radii). We can use the law of cosines to find the length of the chord BC: BC2=OB2+OC2−2(OB)(OC)cos⁡(∠COB)BC^2 = OB^2 + OC^2 - 2(OB)(OC) \cos(∠COB)BC2=OB2+OC2−2(OB)(OC)cos(∠COB) BC2=R2+R2−2(R)(R)cos⁡(120°)BC^2 = R^2 + R^2 - 2(R)(R) \cos(120°)BC2=R2+R2−2(R)(R)cos(120°) Since cos⁡(120°)=−1/2\cos(120°) = -1/2cos(120°)=−1/2: BC2=2R2−2R2(−1/2)=2R2+R2=3R2BC^2 = 2R^2 - 2R^2(-1/2) = 2R^2 + R^2 = 3R^2BC2=2R2−2R2(−1/2)=2R2+R2=3R2 BC=R3BC = R\sqrt{3}BC=R3​
  • The figure shows a symmetric arrangement where C is on the negative y-axis and the chord AB is horizontal. This implies symmetry about the y-axis. Due to this symmetry, AC = BC. This also means ∠CBA = ∠CAB = 60°. Consequently, ∠ACB = 180° - 60° - 60° = 60°. So, triangle ABC is an equilateral triangle with side length L=R3L = R\sqrt{3}L=R3​.
  • We can assign coordinates based on the figure: C at (0, -R). With ∠COB = 120° and symmetry, B is at (Rcos⁡(30°),Rsin⁡(30°))=(R3/2,R/2)(R\cos(30°), R\sin(30°)) = (R\sqrt{3}/2, R/2)(Rcos(30°),Rsin(30°))=(R3​/2,R/2) and A is at (−R3/2,R/2)(-R\sqrt{3}/2, R/2)(−R3​/2,R/2).

2. Evaluate Each Option

A: The electric field at point O

  • The electric field is a vector quantity. E⃗O=E⃗A+E⃗B+E⃗C\vec{E}_O = \vec{E}_A + \vec{E}_B + \vec{E}_CEO​=EA​+EB​+EC​.
  • Charges: qA=q/3q_A = q/3qA​=q/3, qB=q/3q_B = q/3qB​=q/3, qC=−2q/3q_C = -2q/3qC​=−2q/3.
  • Distances: OA = OB = OC = R.
  • Electric field due to qAq_AqA​ at O: E⃗A\vec{E}_AEA​ points from A to O. Its magnitude is EA=k∣qA∣/R2E_A = k |q_A| / R^2EA​=k∣qA​∣/R2 where k=1/(4πϵ0)k=1/(4\pi\epsilon_0)k=1/(4πϵ0​).
  • Electric field due to qBq_BqB​ at O: E⃗B\vec{E}_BEB​ points from B to O.
  • The horizontal components of E⃗A\vec{E}_AEA​ and E⃗B\vec{E}_BEB​ are equal and opposite due to symmetry and qA=qBq_A=q_BqA​=qB​, so they cancel out. The vertical components add up.
  • The angle that OA and OB make with the y-axis is 60°. The vertical component of E⃗A\vec{E}_AEA​ is −EAcos⁡(60°)-E_A \cos(60°)−EA​cos(60°). The vertical component of E⃗B\vec{E}_BEB​ is −EBcos⁡(60°)-E_B \cos(60°)−EB​cos(60°). EA,y+EB,y=−2(k(q/3)/R2)cos⁡(60°)=−2(kq/(3R2))(1/2)=−kq/(3R2)E_{A,y} + E_{B,y} = -2 (k(q/3)/R^2) \cos(60°) = -2(kq/(3R^2))(1/2) = -kq/(3R^2)EA,y​+EB,y​=−2(k(q/3)/R2)cos(60°)=−2(kq/(3R2))(1/2)=−kq/(3R2).
  • Electric field due to qCq_CqC​ at O: qCq_CqC​ is negative, so E⃗C\vec{E}_CEC​ points towards C, which is in the negative y-direction. EC,y=−EC=−k∣qC∣/R2=−k∣−2q/3∣/R2=−2kq/(3R2)E_{C,y} = -E_C = -k|q_C|/R^2 = -k|-2q/3|/R^2 = -2kq/(3R^2)EC,y​=−EC​=−k∣qC​∣/R2=−k∣−2q/3∣/R2=−2kq/(3R2).
  • Total electric field at O: EO,y=EA,y+EB,y+EC,y=−kq/(3R2)−2kq/(3R2)=−3kq/(3R2)=−kq/R2E_{O,y} = E_{A,y} + E_{B,y} + E_{C,y} = -kq/(3R^2) - 2kq/(3R^2) = -3kq/(3R^2) = -kq/R^2EO,y​=EA,y​+EB,y​+EC,y​=−kq/(3R2)−2kq/(3R2)=−3kq/(3R2)=−kq/R2.
  • E⃗O=−q4πϵ0R2j^\vec{E}_O = -{q \over {4\pi\epsilon_0 R^2}} \hat{j}EO​=−4πϵ0​R2q​j^​. The field has magnitude q4πϵ0R2{q \over {4\pi\epsilon_0 R^2}}4πϵ0​R2q​ and is directed along the negative y-axis. Option A is incorrect.

B: The potential energy of the system

  • Potential energy U=k(qAqB/rAB+qBqC/rBC+qCqA/rCA)U = k(q_A q_B / r_{AB} + q_B q_C / r_{BC} + q_C q_A / r_{CA})U=k(qA​qB​/rAB​+qB​qC​/rBC​+qC​qA​/rCA​).
  • As established, triangle ABC is equilateral with side length L=R3L = R\sqrt{3}L=R3​. So rAB=rBC=rCA=R3r_{AB} = r_{BC} = r_{CA} = R\sqrt{3}rAB​=rBC​=rCA​=R3​.
  • U=kR3[(q/3)(q/3)+(q/3)(−2q/3)+(−2q/3)(q/3)]U = {k \over {R\sqrt{3}}} [ (q/3)(q/3) + (q/3)(-2q/3) + (-2q/3)(q/3) ]U=R3​k​[(q/3)(q/3)+(q/3)(−2q/3)+(−2q/3)(q/3)]
  • U=kR3[q2/9−2q2/9−2q2/9]=kR3[−3q2/9]=−kq23R3U = {k \over {R\sqrt{3}}} [ q^2/9 - 2q^2/9 - 2q^2/9 ] = {k \over {R\sqrt{3}}} [-3q^2/9] = -{k q^2 \over {3R\sqrt{3}}}U=R3​k​[q2/9−2q2/9−2q2/9]=R3​k​[−3q2/9]=−3R3​kq2​
  • U=−q212πϵ0R3U = -{q^2 \over {12\pi\epsilon_0 R\sqrt{3}}}U=−12πϵ0​R3​q2​. The potential energy is not zero. Option B is incorrect.

C: The magnitude of the force between the charges at C and B

  • Using Coulomb's law: FCB=k∣qCqB∣rBC2F_{CB} = k {|q_C q_B| \over r_{BC}^2}FCB​=krBC2​∣qC​qB​∣​.
  • Charges: qC=−2q/3q_C = -2q/3qC​=−2q/3, qB=q/3q_B = q/3qB​=q/3.
  • Distance: rBC=R3r_{BC} = R\sqrt{3}rBC​=R3​, so rBC2=3R2r_{BC}^2 = 3R^2rBC2​=3R2.
  • FCB=14πϵ0∣(−2q/3)(q/3)∣(R3)2=14πϵ0(2q2/9)3R2F_{CB} = {1 \over {4\pi\epsilon_0}} { |(-2q/3)(q/3)| \over (R\sqrt{3})^2 } = {1 \over {4\pi\epsilon_0}} { (2q^2/9) \over 3R^2 }FCB​=4πϵ0​1​(R3​)2∣(−2q/3)(q/3)∣​=4πϵ0​1​3R2(2q2/9)​
  • FCB=14πϵ02q227R2=2q2108πϵ0R2=q254πϵ0R2F_{CB} = {1 \over {4\pi\epsilon_0}} {2q^2 \over 27R^2} = {2q^2 \over 108\pi\epsilon_0 R^2} = {q^2 \over 54\pi\epsilon_0 R^2}FCB​=4πϵ0​1​27R22q2​=108πϵ0​R22q2​=54πϵ0​R2q2​.
  • This matches the expression in the option. Option C is correct.

D: The potential at point O

  • Potential is a scalar quantity: VO=VA+VB+VCV_O = V_A + V_B + V_CVO​=VA​+VB​+VC​.
  • VO=kqArA+kqBrB+kqCrCV_O = k{q_A \over r_A} + k{q_B \over r_B} + k{q_C \over r_C}VO​=krA​qA​​+krB​qB​​+krC​qC​​.
  • rA=rB=rC=Rr_A = r_B = r_C = RrA​=rB​=rC​=R.
  • VO=kR(qA+qB+qC)=kR(q/3+q/3−2q/3)V_O = {k \over R} (q_A + q_B + q_C) = {k \over R} (q/3 + q/3 - 2q/3)VO​=Rk​(qA​+qB​+qC​)=Rk​(q/3+q/3−2q/3)
  • VO=kR(0)=0V_O = {k \over R} (0) = 0VO​=Rk​(0)=0.
  • The potential at point O is zero. Option D is incorrect.

Conclusion

Based on the step-by-step analysis, only option C is correct.

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