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AIIMS 2009
Exam
AIIMS
Year
2009
Subject
Physics
Chapter
Electrostatics

AIIMS 2009 · Physics · Electrostatics

A wire of length l and mass m is bent in the form of a semicircle....

A wire of length ll and mass mm is bent in the form of a semicircle. The gravitational field intensity at the centre of semicircle is A wire of length l and mass m is bent in the form of a semicircle. The gravitational field intensity at the centre of

Options

  1. AGmπl\frac{G m}{\pi l} along xx-axis
  2. BGmπl\frac{G m}{\pi l} along yy-axis
  3. C2πGml2\frac{2 \pi G m}{l^2} along yy-axis
  4. D2πGml2\frac{2 \pi G m}{l^2} along xx-axis

Correct answer

C. 2πGml2\frac{2 \pi G m}{l^2} along yy-axis

Step-by-step solution

Consider two small elements each of length dl=rdθd l=r d \theta symmetrically. πr=l\pi r=l A wire of length l and mass m is bent in the form of a semicircle. The gravitational field intensity at the centre of
Resolve the elemental field intensities ∵∣dE1∣=∣dE2∣dE=2dE1cos⁡θ=2Grdθr2cos⁡θ\because\left|d E_1\right|=\left|d E_2\right|d E=2 d E_1 \cos \theta=\frac{2 G r d \theta}{r^2} \cos \thetaG= Gravitational constant λ= Linear massdensity =ml\begin{aligned} & \mathrm{G}=\text{ Gravitational constant } \\ & \lambda=\text{ Linear massdensity }=\frac{m}{l}\end{aligned}ordE=2λGr∫090∘cos⁡θdθ=2λGr=2πGml2or d E=\frac{2 \lambda G}{r} \int_0^{90^{\circ}} \cos \theta d \theta=\frac{2 \lambda G}{r}=\frac{2 \pi G m}{l^2}
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