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JIPMER 2007
Exam
JIPMER
Year
2007
Subject
Physics
Chapter
Magnetic Effects of Current

JIPMER 2007 · Physics · Magnetic Effects of Current

A coil in the shape of an equilateral triangle of side l is...

A coil in the shape of an equilateral triangle of side ll is suspended between the pole pieces of a permanent magnet such that B→\overrightarrow{\mathbf{B}} is in plane of the coil. If due to a current ii in the triangle a torque τ\tau acts on it, the side ll of the triangle isA coil in the shape of an equilateral triangle of side l is suspended between the pole pieces of a permanent magnet

Options

  1. A23(τBi)1/2\frac{2}{\sqrt{3}}\left(\frac{\tau}{B i}\right)^{1 / 2}
  2. B23(τBi)\frac{2}{\sqrt{3}}\left(\frac{\tau}{B i}\right)
  3. C2(τ3Bi)1/22\left(\frac{\tau}{\sqrt{3} B i}\right)^{1 / 2}
  4. D13τBi\frac{1}{\sqrt{3}} \frac{\tau}{B i}

Correct answer

C. 2(τ3Bi)1/22\left(\frac{\tau}{\sqrt{3} B i}\right)^{1 / 2}

Step-by-step solution

Torque acting on equilateral triangle in a magnetic field B→\overrightarrow{\mathbf{B}} is A coil in the shape of an equilateral triangle of side l is suspended between the pole pieces of a permanent magnet τ=iABsin⁡θ\tau=i A B \sin \theta Area of triangle LMN A=34l2andθ=90∘A=\frac{\sqrt{3}}{4} l^2 and \theta=90^{\circ} Substituting the given values in the expression for torque, we have τ=i×34l2Bsin⁡90∘&=34il2B(∵sin⁡90∘=1)\begin{aligned}\tau & =i \times \frac{\sqrt{3}}{4} l^2 B \sin 90^{\circ} \& =\frac{\sqrt{3}}{4} i l^2 B\left(\because \sin 90^{\circ}=1\right)\end{aligned} Hence, $l=2\left(\frac{\tau}{\sqrt{3} B i}\right)^{1 / 2}
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