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QJEEM20Ph66b7: JEE Main 2020 Physics - Class 11 JEEM20Ph66b7 Solution: A uniform rod of length ‘ ’ is pivoted at one of its ends on a…

A uniform rod of length ‘ ll ’ is pivoted at one of its ends on a vertical shaft of negligible radius. When the shaft rotates at angular speed ω\omega the rod makes an angle θ\theta with it (see figure). To find θ\theta equate the rate of change of angular momentum (direction going into the paper) ml212ω2sin⁡θcos⁡θ{{m{l^2}} \over {12}}{\omega ^2}\sin \theta \cos \theta about the centre of mass (CM) to the torque provided by the horizontal and vertical forces FH and FV about the CM. The value of θ\theta is then such that : JEE Main 2020 (Online) 3rd September Evening Slot Physics - Rotational Motion Question 129 English

Multiple Choice Options

  • A cos⁡θ=2g3lω2\cos \theta = {{2g} \over {3l{\omega ^2}}}
  • B cos⁡θ=3g2lω2\cos \theta = {{3g} \over {2l{\omega ^2}}}
  • C cos⁡θ=g2lω2\cos \theta = {g \over {2l{\omega ^2}}}
  • D cos⁡θ=glω2\cos \theta = {g \over {l{\omega ^2}}}

Step-by-Step Verified Solution

JEE Main 2020 (Online) 3rd September Evening Slot Physics - Rotational Motion Question 129 English Explanation
Fv=mg{F_v} = mg

FH=mω2l2sin⁡θ{F_H} = m{\omega ^2}{l \over 2}\sin \theta

∴\therefore τnet about COM=Fv.l2sin⁡θ−FHl2cos⁡θ{\tau _{net}}\,about\,COM = {F_v}.{l \over 2}\sin \theta - {F_H}{l \over 2}\cos \theta

=ml212ω2sin⁡θcos⁡θ= {{m{l^2}} \over {12}}{\omega ^2}\sin \theta \cos \theta

⇒\Rightarrow mgl2sin⁡θ−mω2l2sin⁡θl2cos⁡θ=ml212ω2sin⁡θcos⁡θmg{l \over 2}\sin \theta - m{\omega ^2}{l \over 2}\sin \theta {l \over 2}\cos \theta = {{m{l^2}} \over {12}}{\omega ^2}\sin \theta \cos \theta

⇒gl2−ω2l24cos⁡θ=l212ω2cos⁡θ\Rightarrow {{gl} \over 2} - {{{\omega ^2}{l^2}} \over 4}\cos \theta = {{{l^2}} \over {12}}{\omega ^2}\cos \theta

⇒\Rightarrow gl2=ω2l2cos⁡θ(112+14){{gl} \over 2} ={\omega ^2}{l^2}\cos \theta \left( {{1 \over {12}} + {1 \over 4}} \right)

⇒\Rightarrow gl2=ω2l2cos⁡θ3{{gl} \over 2} = {{{\omega ^2}{l^2}\cos \theta } \over 3}

⇒\Rightarrow cos⁡θ=3g2ω2l\cos \theta = {{3g} \over {2{\omega ^2}l}}

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