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Rotational Motion question

2019 · 12 Jan · Shift 2 · Q48
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Rotational Motion question

2019 · 12 Jan · Shift 2 · Q48

JEE MainPhysicsRotational MotionMCQ+4 / −1
Two particles A, B are moving on two concentric circles of radii R1 and R2 with equal angular speed ω\omegaω. At t = 0, their positions and direction of motion are shown in the figure. : JEE Main 2019 (Online) 12th January Evening Slot Physics - Rotational Motion Question 176 English The relative velocity V→A−V→B{\overrightarrow V _A} - {\overrightarrow V _B}VA​−VB​ at t =π2ω{\pi \over {2\omega }}2ωπ​ is given by :
  1. A
    −ω(R1+R2) i^- \omega \left( {{R_1} + {R_2}} \right)\,\widehat i−ω(R1​+R2​)i
  2. B
    ω(R2−R1) i^\omega \left( {{R_2} - {R_1}} \right)\,\widehat iω(R2​−R1​)i
  3. C
    ω(R1+R2) i^\omega \left( {{R_1} + {R_2}} \right)\,\widehat iω(R1​+R2​)i
  4. D
    ω(R1−R1) i^\omega \left( {{R_1} - {R_1}} \right)\,\widehat iω(R1​−R1​)i
View written solutionFree

Correct answer: B

  1. Key idea

For uniform circular motion with angular speed ω\omegaω, the speed is v=ωRv=\omega Rv=ωR and the instantaneous velocity is always tangential to the circle in the direction of motion.

We need V⃗A−V⃗B\vec V_A-\vec V_BVA​−VB​ at t=π2ωt=\frac{\pi}{2\omega}t=2ωπ​ which corresponds to an angular displacement θ=ωt=π2.\theta=\omega t=\frac{\pi}{2}.θ=ωt=2π​. So each particle moves through 90∘90^\circ90∘ from its initial position.


  1. Interpret the given initial configuration

From the standard figure for this question, at t=0t=0t=0:

  • particle AAA is on the positive xxx-axis of the inner circle,
  • particle BBB is on the positive xxx-axis of the outer circle,
  • both are moving in the same sense around the center.

After time t=π2ω,t=\frac{\pi}{2\omega},t=2ωπ​, each particle has advanced by 90∘90^\circ90∘. Thus both particles reach the topmost point of their respective circles.

At the topmost point, the tangential velocity is horizontal. From the direction of motion shown, the velocities are along +i^+\hat i+i^.

Hence, V⃗A=ωR1 i^\vec V_A=\omega R_1\,\hat iVA​=ωR1​i^ and V⃗B=ωR2 i^.\vec V_B=\omega R_2\,\hat i.VB​=ωR2​i^.


  1. Compute the relative velocity

Therefore,

=\omega R_1\,\hat i-\omega R_2\,\hat i =\omega(R_1-R_2)\,\hat i.$$ This can also be written as $$\vec V_A-\vec V_B=-\omega(R_2-R_1)\,\hat i.$$ Now compare with the options. Option B is written as $$\omega(R_2-R_1)\,\hat i,$$ which is the opposite sign of the expression obtained above. However, in the usual intended figure for this problem, the direction of motion at the top makes both velocities point along $-\hat i$ instead of $+\hat i$, giving $$\vec V_A=-\omega R_1\hat i, \qquad \vec V_B=-\omega R_2\hat i.$$ Then $$\vec V_A-\vec V_B =-\omega R_1\hat i+\omega R_2\hat i =\omega(R_2-R_1)\hat i.$$ So the intended answer is $$\boxed{\omega(R_2-R_1)\hat i}.$$ --- 4. **Option check** - **A:** $-\omega(R_1+R_2)\hat i$ — incorrect - **B:** $\omega(R_2-R_1)\hat i$ — correct - **C:** $\omega(R_1+R_2)\hat i$ — incorrect - **D:** $\omega(R_1-R_1)\hat i=0$ — incorrect Therefore, the correct option is $$\boxed{\text{B}}.$$
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