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Two identical charged spheres suspended from a common point by two massless strings of lengths l are initially at a distance d (d << l) apart because of their mutual repulsion. The charges begin to leak from both the spheres at a constant rate. As a result, the spheres approach each other with a velocity v. Then v varies as a function of the distance x between the spheres, as:

A

v \propto x

B

v \propto x⁻¹/²

C

v \propto x⁻¹

D

v \propto x¹/²

Step-by-Step Solution

At equilibrium, the electrostatic force (FeF_e) is balanced by the horizontal component of the tension, while gravity balances the vertical component. For small angles (since xlx \ll l), tanθsinθ=x2l\tan \theta \approx \sin \theta = \frac{x}{2l}.

  1. Equilibrium Condition: Fe=mgtanθkq2x2=mgx2lF_e = mg \tan \theta \Rightarrow \frac{kq^2}{x^2} = mg \frac{x}{2l}.
  2. Relation: This implies q2x3q^2 \propto x^3, or qx3/2q \propto x^{3/2}.
  3. Differentiation: Since charge leaks at a constant rate (dqdt=C\frac{dq}{dt} = C), differentiating with respect to time gives dqdtddt(x3/2)Cx1/2dxdt\frac{dq}{dt} \propto \frac{d}{dt}(x^{3/2}) \Rightarrow C \propto x^{1/2} \frac{dx}{dt}.
  4. Velocity: Substituting v=dxdtv = \frac{dx}{dt}, we get Cx1/2vC \propto x^{1/2} v, which leads to vx1/2v \propto x^{-1/2}.
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