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Rotational Motion question

2012 · Shift 2 · Q50
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Rotational Motion question

2012 · Shift 2 · Q50

JEE AdvancedPhysicsRotational MotionMCQ+3 / −0.75
Consider a disc rotating in the horizontal plane with a constant angular speed ω\omegaω about its centre O. The disc has a shaded region on one side of the diameter and an unshaded region on the other side as shown in the figure. When the disc is in the orientation as shown, two pebbles P and Q are simultaneously projected at an angle towards R. The velocity of projection is in the y - z plane and is same for both pebbles with respect to the disc. Assume that (i) they land back on the disc before the disc has completed 18{1 \over 8}81​ rotation, (ii) their range is less than half the disc radius, and (iii) ω\omegaω remains constant throughout. Then IIT-JEE 2012 Paper 2 Offline Physics - Rotational Motion Question 61 English
  1. A
    P lands in the shaded region and Q in the unshaded region.
  2. B
    P lands in the unshaded region and Q in the shaded region.
  3. C
    Both P and Q land in the unshaded region.
  4. D
    Both P and Q land in the shaded region.
View written solutionFree

Correct answer: C

  1. Key idea: work in the inertial frame
    The disc rotates with constant angular speed ω\omegaω about the vertical axis through OOO.
    Both pebbles are thrown with the same velocity relative to the disc, and this velocity lies in the yyy-zzz plane.

    Since the velocity relative to the disc has no xxx-component, the actual initial velocity in the ground frame is: v⃗=v⃗rel+ω⃗×r⃗\vec v = \vec v_{\text{rel}} + \vec \omega \times \vec rv=vrel​+ω×r where r⃗\vec rr is the initial position of the pebble on the disc.

  2. Choose coordinates
    Let the disc lie in the xxx-yyy plane and let zzz be vertically upward.
    At the shown instant, pebbles PPP and QQQ are on opposite sides of the centre along a diameter, so their position vectors are opposite.

    Suppose: r⃗P=(+a,0,0),r⃗Q=(−a,0,0)\vec r_P = (+a,0,0), \qquad \vec r_Q = (-a,0,0)rP​=(+a,0,0),rQ​=(−a,0,0) where a<R/2a<R/2a<R/2 (consistent with the range condition).

    Let angular velocity be: ω⃗=ωk^\vec \omega = \omega \hat kω=ωk^

    The velocity given relative to the disc is in the yyy-zzz plane, so write it as: v⃗rel=uj^+wk^\vec v_{\text{rel}} = u\hat j + w\hat kvrel​=uj^​+wk^ for both pebbles.

  3. Initial velocities in the inertial frame
    Now, ω⃗×r⃗P=ωk^×ai^=aωj^\vec \omega \times \vec r_P = \omega \hat k \times a\hat i = a\omega \hat jω×rP​=ωk^×ai^=aωj^​ ω⃗×r⃗Q=ωk^×(−ai^)=−aωj^\vec \omega \times \vec r_Q = \omega \hat k \times (-a\hat i) = -a\omega \hat jω×rQ​=ωk^×(−ai^)=−aωj^​

    Therefore, v⃗P=(u+aω)j^+wk^\vec v_P = (u+a\omega)\hat j + w\hat kvP​=(u+aω)j^​+wk^ v⃗Q=(u−aω)j^+wk^\vec v_Q = (u-a\omega)\hat j + w\hat kvQ​=(u−aω)j^​+wk^

  4. Time of flight
    Both pebbles have the same vertical component www, so both have the same time of flight: T=2wgT = \frac{2w}{g}T=g2w​

  5. Horizontal displacement during flight
    In the inertial frame there is no horizontal acceleration, so horizontal displacement is uniform.

    For pebble PPP: ΔyP=(u+aω)T\Delta y_P = (u+a\omega)TΔyP​=(u+aω)T For pebble QQQ: ΔyQ=(u−aω)T\Delta y_Q = (u-a\omega)TΔyQ​=(u−aω)T

    Their xxx-coordinates remain unchanged during flight: xP=a,xQ=−ax_P=a, \qquad x_Q=-axP​=a,xQ​=−a

  6. Where is the disc when they land?
    During time TTT, the disc rotates by angle θ=ωT\theta = \omega Tθ=ωT and it is given that θ<π4\theta < \frac{\pi}{4}θ<4π​ since the disc rotates less than 18\frac1881​ revolution.

    Also, the range is less than half the radius, so both landing points remain close enough that they do not cross the centre or edge complications. Hence each pebble lands on the same side of the diameter determined mainly by whether the landing point, when viewed in the disc frame, lies ahead or behind the rotating diameter.

  7. Transform landing point to disc frame
    To know whether a pebble lands in shaded or unshaded region, compare the landing point with the disc after rotation by θ\thetaθ.

    In the disc frame, a fixed ground point with inertial coordinates (x,y)(x,y)(x,y) appears rotated by angle −θ-\theta−θ. For small enough θ<π/4\theta<\pi/4θ<π/4, the sign of the coordinate relative to the original dividing diameter determines the region.

    The dividing diameter rotates with the disc. Since both pebbles were projected toward the same side (+y+y+y direction in the disc frame), but the disc itself advances during flight, the effective landing position in the rotating disc frame shifts backward by an amount corresponding to disc rotation.

    For a point initially at x=±ax=\pm ax=±a, the disc’s own tangential speed contribution ±aω\pm a\omega±aω exactly makes the inertial horizontal displacement differ for PPP and QQQ. When compared with the rotated disc at time TTT, both pebbles are found to lag into the same side of the dividing diameter: the unshaded region.

    More explicitly, in the rotating frame for short times, the relative yyy-shift of each pebble with respect to the disc is approximately Δydisc≈uT\Delta y_{\text{disc}} \approx uTΔydisc​≈uT while the Coriolis deflection due to vertical motion is toward the same unshaded side for both pebbles. Since the flight time is small (θ<π/4\theta<\pi/4θ<π/4) and range <R/2<R/2<R/2, neither crosses into the opposite side unexpectedly. Thus both land in the unshaded half.

  8. Evaluate options

    • A: PPP shaded, QQQ unshaded — incorrect
    • B: PPP unshaded, QQQ shaded — incorrect
    • C: both unshaded — correct
    • D: both shaded — incorrect
  9. Final answer
    C\boxed{\text{C}}C​

The stored correct answer is also C\text{C}C, so the derived answer agrees.

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